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	<title>Concrete Nonsense &#187; Algebraic Geometry</title>
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		<title>Concrete Nonsense &#187; Algebraic Geometry</title>
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		<title>Finite field counts and the Grothendieck ring of varieties</title>
		<link>http://concretenonsense.wordpress.com/2009/11/23/finite-field-counts-and-the-grothendieck-ring-of-varieties/</link>
		<comments>http://concretenonsense.wordpress.com/2009/11/23/finite-field-counts-and-the-grothendieck-ring-of-varieties/#comments</comments>
		<pubDate>Mon, 23 Nov 2009 15:59:40 +0000</pubDate>
		<dc:creator>Steven Sam</dc:creator>
				<category><![CDATA[Algebraic Geometry]]></category>
		<category><![CDATA[Combinatorics]]></category>
		<category><![CDATA[finite fields]]></category>
		<category><![CDATA[homogeneous spaces]]></category>
		<category><![CDATA[motives]]></category>

		<guid isPermaLink="false">http://concretenonsense.wordpress.com/?p=830</guid>
		<description><![CDATA[Lately some of us at MIT have been thinking about counting -rational points on some classes of varieties related to linear algebra that provide natural q-analogues for various classes of permutations. One thing we came across was some classes that have the same counts over every finite field. Yan wanted me to post about the [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=concretenonsense.wordpress.com&blog=2918042&post=830&subd=concretenonsense&ref=&feed=1" />]]></description>
			<content:encoded><![CDATA[<div class='snap_preview'><br /><p>Lately some of us at MIT have been thinking about counting <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BF%7D_q&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{F}_q' title='\mathbf{F}_q' class='latex' />-rational points on some classes of varieties related to linear algebra that provide natural q-analogues for various classes of permutations. One thing we came across was some classes that have the same counts over every finite field. Yan wanted me to post about the following, so I&#8217;ll delay my post on the K-theory of the Grassmannian until next time.</p>
<p>We&#8217;ll consider varieties defined over a fixed field K. Form the free Abelian group on the isomorphism classes of such varieties. If Z is a closed subvariety of X, then we impose the relation </p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5BX%5D+%3D+%5BZ%5D+%2B+%5BX+%5Csetminus+Z%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[X] = [Z] + [X \setminus Z]' title='[X] = [Z] + [X \setminus Z]' class='latex' />.</p>
<p>We can put a product structure on this group via</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5BX%5D+%5Ccdot+%5BY%5D+%3D+%5BX+%5Ctimes+Y%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[X] \cdot [Y] = [X \times Y]' title='[X] \cdot [Y] = [X \times Y]' class='latex' /></p>
<p>though it will not be relevant for this post. Related to this product structure is a <a href="http://arxiv.org/abs/math/0204306">paper by Bjorn Poonen</a> which shows that if the characteristic is 0, then this ring is <b>not</b> an integral domain. And presumably the result is true over positive characteristic also, but the paper uses the existence of resolution of singularities. This is the <b>Grothendieck ring of varieties</b>. This is at least one way to make sense of statements of the form: <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BP%7D%5E2+%3D+%5Cmathbf%7BA%7D%5E2+%2B+%5Cmathbf%7BP%7D%5E1+%3D+%5Cmathbf%7BA%7D%5E2+%2B+%5Cmathbf%7BA%7D%5E1+%2B+%5Cmathbf%7BA%7D%5E0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{P}^2 = \mathbf{A}^2 + \mathbf{P}^1 = \mathbf{A}^2 + \mathbf{A}^1 + \mathbf{A}^0' title='\mathbf{P}^2 = \mathbf{A}^2 + \mathbf{P}^1 = \mathbf{A}^2 + \mathbf{A}^1 + \mathbf{A}^0' class='latex' />.<br />
<span id="more-830"></span><br />
In particular this works over a finite field, and then the equations can be turned into equations of numbers by replacing <img src='http://l.wordpress.com/latex.php?latex=%5BX%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[X]' title='[X]' class='latex' /> with <img src='http://l.wordpress.com/latex.php?latex=%5C%23X%28%5Cmathbf%7BF%7D_q%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\#X(\mathbf{F}_q)' title='\#X(\mathbf{F}_q)' class='latex' />.</p>
<p>Here&#8217;s one such example. Let G be a semisimple group defined over an algebraically closed field K of characteristic p &gt; 0, let B be a Borel subgroup, and let X = G/B be its full flag variety. Then B acts on X by left multiplication, and the orbits are indexed by elements of the Weyl group W. In particular, each orbit is an affine space, and its dimension is the length of the corresponding element. So we get a decomposition </p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+%5BX%5D+%3D+%5Csum_%7Bw+%5Cin+W%7D+%5B%5Cmathbf%7BA%7D%5E%7B%5Cell%28w%29%7D%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle [X] = \sum_{w \in W} [\mathbf{A}^{\ell(w)}]' title='\displaystyle [X] = \sum_{w \in W} [\mathbf{A}^{\ell(w)}]' class='latex' />.</p>
<p>All of this stuff is defined over the integers, so we can actually work in a finite field. Then we get the equation</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+%5C%23X%28%5Cmathbf%7BF%7D_q%29+%3D+%5Csum_%7Bw+%5Cin+W%7D+q%5E%7B%5Cell%28w%29%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle \#X(\mathbf{F}_q) = \sum_{w \in W} q^{\ell(w)}' title='\displaystyle \#X(\mathbf{F}_q) = \sum_{w \in W} q^{\ell(w)}' class='latex' />.</p>
<p>The odd spin group <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BSpin%7D_%7B2n%2B1%7D%28K%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{Spin}_{2n+1}(K)' title='\mathbf{Spin}_{2n+1}(K)' class='latex' /> (the double cover of the special orthogonal group <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BSO%7D_%7B2n%2B1%7D%28K%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{SO}_{2n+1}(K)' title='\mathbf{SO}_{2n+1}(K)' class='latex' />) and the symplectic groups <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BSp%7D_%7B2n%7D%28K%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{Sp}_{2n}(K)' title='\mathbf{Sp}_{2n}(K)' class='latex' /> have the same Weyl groups, so in particular, their flag varieties are equal in the Grothendieck ring of varieties, even though the varieties themselves are not isomorphic for <img src='http://l.wordpress.com/latex.php?latex=n+%5Cge+3&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n \ge 3' title='n \ge 3' class='latex' />. One way of seeing this is via the Borel&#8211;Weil construction: the global sections of a line bundle on G/B is either 0 or an indecomposable module called a Weyl module. The dimension of the Weyl module (after we pick a way to index the line bundles) is independent of characteristic since it has a <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BZ%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{Z}' title='\mathbf{Z}' class='latex' />-form which is a free Abelian group. In general the sections contain a unique irreducible representation as a submodule, and all irreducible representations arise in this way. </p>
<p>In characteristic 0, indecomposable is the same thing as irreducible, so we can calculate the dimensions using the Weyl character formula. Since these multisets of dimensions are different, we can&#8217;t have an isomorphism. </p>
<p>Does anyone know of a better reason why they are not isomorphic varieties?</p>
<p>-Steven</p>
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			<media:title type="html">masnevets</media:title>
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		<title>Chow rings and K-theory</title>
		<link>http://concretenonsense.wordpress.com/2009/11/09/chow-rings-and-k-theory/</link>
		<comments>http://concretenonsense.wordpress.com/2009/11/09/chow-rings-and-k-theory/#comments</comments>
		<pubDate>Mon, 09 Nov 2009 15:27:19 +0000</pubDate>
		<dc:creator>Steven Sam</dc:creator>
				<category><![CDATA[Algebraic Geometry]]></category>
		<category><![CDATA[chow ring]]></category>
		<category><![CDATA[intersection theory]]></category>
		<category><![CDATA[K-theory]]></category>

		<guid isPermaLink="false">http://concretenonsense.wordpress.com/?p=758</guid>
		<description><![CDATA[I want to write a post about the set-valued tableaux of Buch and how they are related to Schur polynomials. But since these two things are related to the K-theory and Chow ring, respectively, of the Grassmannian, I thought I would write a post explaining some basic generalities between the Chow ring and K-theory. Let [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=concretenonsense.wordpress.com&blog=2918042&post=758&subd=concretenonsense&ref=&feed=1" />]]></description>
			<content:encoded><![CDATA[<div class='snap_preview'><br /><p>I want to write a post about the set-valued tableaux of Buch and how they are related to Schur polynomials. But since these two things are related to the K-theory and Chow ring, respectively, of the Grassmannian, I thought I would write a post explaining some basic generalities between the Chow ring and K-theory. Let X be a variety over an algebraically closed field K.</p>
<p>First let&#8217;s define the Chow groups. We first form the k-cycles <img src='http://l.wordpress.com/latex.php?latex=Z_k%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='Z_k(X)' title='Z_k(X)' class='latex' /> to be the free Abelian group spanned by the k-dimensional subvarieties of X. Let [V] be the basis element corresponding to a subvariety V. Pick a subvariety W of X of dimension k+1, and a nonzero rational function f/g defined on W. If V is a codimension 1 subvariety of W, let <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BO%7D_%7BW%2CV%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{O}_{W,V}' title='\mathcal{O}_{W,V}' class='latex' /> be the ring obtained by taking the ring of polynomial functions on W and inverting all polynomial functions which are not identically zero on V. We define the <b>order</b> <img src='http://l.wordpress.com/latex.php?latex=%7B%5Crm+ord%7D_V%28f%2Fg%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\rm ord}_V(f/g)' title='{\rm ord}_V(f/g)' class='latex' /> to be <img src='http://l.wordpress.com/latex.php?latex=%5Cdim_K+%5Cmathcal%7BO%7D_%7BW%2CV%7D%2F%28f%29+-+%5Cdim_K+%5Cmathcal%7BO%7D_%7BW%2CV%7D%2F%28g%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\dim_K \mathcal{O}_{W,V}/(f) - \dim_K \mathcal{O}_{W,V}/(g)' title='\dim_K \mathcal{O}_{W,V}/(f) - \dim_K \mathcal{O}_{W,V}/(g)' class='latex' />, where the dimension is as K-vector spaces. The <b>divisor</b> of f/g is given by <img src='http://l.wordpress.com/latex.php?latex=%7B%5Crm+div%7D%28f%2Fg%29+%3D+%5Csum_%7B%5Cdim+V+%3D+k%7D+%7B%5Crm+ord%7D_V%28f%2Fg%29+%5BV%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\rm div}(f/g) = \sum_{\dim V = k} {\rm ord}_V(f/g) [V]' title='{\rm div}(f/g) = \sum_{\dim V = k} {\rm ord}_V(f/g) [V]' class='latex' />. We say these divisors are <b>rationally equivalent</b> to 0, and define the Chow group <img src='http://l.wordpress.com/latex.php?latex=%7B%5Crm+A%7D_k%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\rm A}_k(X)' title='{\rm A}_k(X)' class='latex' /> to be the group of k-cycles modulo rational equivalence.<br />
<span id="more-758"></span><br />
Now let&#8217;s assume that X is nonsingular of dimension n. Given subvarieties V and W of X, let Z be an irreducible component of the intersection <img src='http://l.wordpress.com/latex.php?latex=V+%5Ccap+W&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V \cap W' title='V \cap W' class='latex' />. Restrict to an open affine subset U of X, so that V and W are defined by ideals I and J, respectively. We define the <b>intersection multiplicity</b> to be the following alternating sum</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+%5Cmu%28Z%3B+V%2CW%29+%3D+%5Csum_%7Bi+%5Cge+0%7D+%28-1%29%5Ei+%7B%5Crm+length%7D_%7B%5Cmathcal%7BO%7D_%7BX%2CZ%7D%7D+%7B%5Crm+Tor%7D%5Ei_%7B%5Cmathcal%7BO%7D_%7BZ%2CZ%7D%7D+%28%5Cmathcal%7BO%7D_%7BX%2CZ%7D+%2F+I%2C+%5Cmathcal%7BO%7D_%7BX%2CZ%7D+%2F+J%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle \mu(Z; V,W) = \sum_{i \ge 0} (-1)^i {\rm length}_{\mathcal{O}_{X,Z}} {\rm Tor}^i_{\mathcal{O}_{Z,Z}} (\mathcal{O}_{X,Z} / I, \mathcal{O}_{X,Z} / J)' title='\displaystyle \mu(Z; V,W) = \sum_{i \ge 0} (-1)^i {\rm length}_{\mathcal{O}_{X,Z}} {\rm Tor}^i_{\mathcal{O}_{Z,Z}} (\mathcal{O}_{X,Z} / I, \mathcal{O}_{X,Z} / J)' class='latex' />.</p>
<p>Set <img src='http://l.wordpress.com/latex.php?latex=%7B%5Crm+A%7D%5Ek%28X%29+%3D+%7B%5Crm+A%7D_%7Bn-k%7D%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\rm A}^k(X) = {\rm A}_{n-k}(X)' title='{\rm A}^k(X) = {\rm A}_{n-k}(X)' class='latex' />. We can give <img src='http://l.wordpress.com/latex.php?latex=%7B%5Crm+A%7D%5E%2A%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\rm A}^*(X)' title='{\rm A}^*(X)' class='latex' /> a graded ring structure by defining <img src='http://l.wordpress.com/latex.php?latex=%5BV%5D+%5Ccdot+%5BW%5D+%3D+%5Csum+%5Cmu%28Z%3B+V%2CW%29+%5BZ%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[V] \cdot [W] = \sum \mu(Z; V,W) [Z]' title='[V] \cdot [W] = \sum \mu(Z; V,W) [Z]' class='latex' />, where the sum is over all irreducible components Z of <img src='http://l.wordpress.com/latex.php?latex=V+%5Ccap+W&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V \cap W' title='V \cap W' class='latex' />.</p>
<p>Now we discuss the K-theory K(X) of vector bundles. For now we don&#8217;t need to assume X nonsingular yet. We first consider the free Abelian group on isomorphism classes of vector bundles on X, modulo relations given by short exact sequences: for any sequence <img src='http://l.wordpress.com/latex.php?latex=0+%5Cto+E_1+%5Cto+E_2+%5Cto+E_3+%5Cto+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='0 \to E_1 \to E_2 \to E_3 \to 0' title='0 \to E_1 \to E_2 \to E_3 \to 0' class='latex' />, we add the relation <img src='http://l.wordpress.com/latex.php?latex=%5BE_1%5D+-+%5BE_2%5D+%2B+%5BE_3%5D+%3D+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[E_1] - [E_2] + [E_3] = 0' title='[E_1] - [E_2] + [E_3] = 0' class='latex' />. We endow K(X) with a ring structure via <img src='http://l.wordpress.com/latex.php?latex=%5BE%5D+%2B+%5BF%5D+%3D+%5BE+%5Coplus+F%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[E] + [F] = [E \oplus F]' title='[E] + [F] = [E \oplus F]' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=%5BE%5D+%5Ccdot+%5BF%5D+%3D+%5BE+%5Cotimes+F%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[E] \cdot [F] = [E \otimes F]' title='[E] \cdot [F] = [E \otimes F]' class='latex' /> which one verifies is well-defined. Similarly, we can form the K-theory <img src='http://l.wordpress.com/latex.php?latex=%7B%5Crm+K%7D_%5Ccirc%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\rm K}_\circ(X)' title='{\rm K}_\circ(X)' class='latex' /> of coherent sheaves on X, which doesn&#8217;t necessarily have a multiplication since tensoring with an arbitrary coherent sheaf need not preserve exact sequences. There is a map</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cvarepsilon+%5Ccolon+%7B%5Crm+K%7D%28X%29+%5Cto+%7B%5Crm+K%7D_%5Ccirc%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\varepsilon \colon {\rm K}(X) \to {\rm K}_\circ(X)' title='\varepsilon \colon {\rm K}(X) \to {\rm K}_\circ(X)' class='latex' /></p>
<p>obtained by sending the class of a vector bundle to itself, considered as a locally free sheaf. When X is nonsingular, this map is an isomorphism. The reason is that in this situation, one can always resolve any coherent sheaf by a finite resolution of vector bundles (one never needs more than <img src='http://l.wordpress.com/latex.php?latex=%5Cdim+X+%2B+1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\dim X + 1' title='\dim X + 1' class='latex' /> such vector bundles).</p>
<p>In general, we can define the topological filtration of <img src='http://l.wordpress.com/latex.php?latex=%7B%5Crm+K%7D_%5Ccirc%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\rm K}_\circ(X)' title='{\rm K}_\circ(X)' class='latex' /> by letting <img src='http://l.wordpress.com/latex.php?latex=F_k+%7B%5Crm+K%7D_%5Ccirc%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F_k {\rm K}_\circ(X)' title='F_k {\rm K}_\circ(X)' class='latex' /> be the subgroup generated by coherent sheaves whose support has dimension at most k. Let <img src='http://l.wordpress.com/latex.php?latex=%7B%5Crm+gr%7D_k+%7B%5Crm+K%7D_%5Ccirc%28X%29+%3D+F_k+%7B%5Crm+K%7D_%5Ccirc%28X%29+%2F+F_%7Bk-1%7D+%7B%5Crm+K%7D_%5Ccirc%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\rm gr}_k {\rm K}_\circ(X) = F_k {\rm K}_\circ(X) / F_{k-1} {\rm K}_\circ(X)' title='{\rm gr}_k {\rm K}_\circ(X) = F_k {\rm K}_\circ(X) / F_{k-1} {\rm K}_\circ(X)' class='latex' />. Given a coherent sheaf <img src='http://l.wordpress.com/latex.php?latex=%5Cmathscr%7BF%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathscr{F}' title='\mathscr{F}' class='latex' /> and a subvariety V of X, we can define the <b>multiplicity</b> <img src='http://l.wordpress.com/latex.php?latex=m_V%28%5Cmathscr%7BF%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='m_V(\mathscr{F})' title='m_V(\mathscr{F})' class='latex' /> as follows: on an affine open set U = Spec(A) which intersects V, V corresponds to a prime ideal P of A, <img src='http://l.wordpress.com/latex.php?latex=%5Cmathscr%7BF%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathscr{F}' title='\mathscr{F}' class='latex' /> corresponds to a finitely generated A-module M. So we can localize M at P to get a module over the local ring <img src='http://l.wordpress.com/latex.php?latex=A_P&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='A_P' title='A_P' class='latex' />, and <img src='http://l.wordpress.com/latex.php?latex=m_V%28%5Cmathscr%7BF%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='m_V(\mathscr{F})' title='m_V(\mathscr{F})' class='latex' /> is the length of <img src='http://l.wordpress.com/latex.php?latex=M_P&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='M_P' title='M_P' class='latex' /> as an <img src='http://l.wordpress.com/latex.php?latex=A_P&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='A_P' title='A_P' class='latex' />-module. Now for <img src='http://l.wordpress.com/latex.php?latex=%5Cmathscr%7BF%7D+%5Cin+F_k+%7B%5Crm+K%7D_%5Ccirc%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathscr{F} \in F_k {\rm K}_\circ(X)' title='\mathscr{F} \in F_k {\rm K}_\circ(X)' class='latex' />, we can define</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+Z_k%28%5Cmathscr%7BF%7D%29+%3D+%5Csum_%7B%5Cdim+V+%3D+k%7D+m_V%28%5Cmathscr%7BF%7D%29+%5BV%5D+%5Cin+%7B%5Crm+A%7D_k%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle Z_k(\mathscr{F}) = \sum_{\dim V = k} m_V(\mathscr{F}) [V] \in {\rm A}_k(X)' title='\displaystyle Z_k(\mathscr{F}) = \sum_{\dim V = k} m_V(\mathscr{F}) [V] \in {\rm A}_k(X)' class='latex' />.</p>
<p>There is a unique homomorphism <img src='http://l.wordpress.com/latex.php?latex=%5Cvarphi+%5Ccolon+Z_k%28X%29+%5Cto+%7B%5Crm+gr%7D_k+%7B%5Crm+K%7D_%5Ccirc%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\varphi \colon Z_k(X) \to {\rm gr}_k {\rm K}_\circ(X)' title='\varphi \colon Z_k(X) \to {\rm gr}_k {\rm K}_\circ(X)' class='latex' /> such that <img src='http://l.wordpress.com/latex.php?latex=%5BV%5D+%5Cmapsto+%5B%5Cmathcal%7BO%7D_V%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[V] \mapsto [\mathcal{O}_V]' title='[V] \mapsto [\mathcal{O}_V]' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=Z_k%28%5Cmathscr%7BF%7D%29+%5Cmapsto+%5B%5Cmathscr%7BF%7D%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='Z_k(\mathscr{F}) \mapsto [\mathscr{F}]' title='Z_k(\mathscr{F}) \mapsto [\mathscr{F}]' class='latex' />, and it factors through rational equivalence to give a map <img src='http://l.wordpress.com/latex.php?latex=%5Cvarphi+%5Ccolon+%7B%5Crm+A%7D_k%28X%29+%5Cto+%7B%5Crm+gr%7D_k+%7B%5Crm+K%7D_%5Ccirc%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\varphi \colon {\rm A}_k(X) \to {\rm gr}_k {\rm K}_\circ(X)' title='\varphi \colon {\rm A}_k(X) \to {\rm gr}_k {\rm K}_\circ(X)' class='latex' />. </p>
<p>In the case that X is nonsingular, we can tensor this map with the rational numbers to get an isomorphism <img src='http://l.wordpress.com/latex.php?latex=%5Cvarphi_%7B%5Cbf+Q%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\varphi_{\bf Q}' title='\varphi_{\bf Q}' class='latex' />. Then K-theory of coherent sheaves is the same as K-theory of vector bundles, and the topological filtration in this case is a filtration by subrings. In fact, after identifying <img src='http://l.wordpress.com/latex.php?latex=%7B%5Crm+A%7D_%2A%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\rm A}_*(X)' title='{\rm A}_*(X)' class='latex' /> with the Chow ring <img src='http://l.wordpress.com/latex.php?latex=%7B%5Crm+A%7D%5E%2A%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\rm A}^*(X)' title='{\rm A}^*(X)' class='latex' />, the map <img src='http://l.wordpress.com/latex.php?latex=%5Cvarphi_%7B%5Cmathbf%7BQ%7D%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\varphi_{\mathbf{Q}}' title='\varphi_{\mathbf{Q}}' class='latex' /> is an isomorphism of rings. This says that cohomology is a sort of approximation to K-theory.</p>
<p>Next time, I&#8217;ll specialize to the case when X is a Grassmannian, and explain the combinatorics involved with the Chow ring and K-theory. This will make the isomorphism above more clear.</p>
<p>-Steven</p>
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		<title>Exceptional sequences for the Grassmannian</title>
		<link>http://concretenonsense.wordpress.com/2009/10/26/exceptional-sequences-for-the-grassmannian/</link>
		<comments>http://concretenonsense.wordpress.com/2009/10/26/exceptional-sequences-for-the-grassmannian/#comments</comments>
		<pubDate>Mon, 26 Oct 2009 16:11:09 +0000</pubDate>
		<dc:creator>Steven Sam</dc:creator>
				<category><![CDATA[Algebraic Geometry]]></category>
		<category><![CDATA[Category Theory]]></category>
		<category><![CDATA[beilinson resolution]]></category>
		<category><![CDATA[derived category]]></category>
		<category><![CDATA[fourier-mukai transform]]></category>
		<category><![CDATA[grassmannian]]></category>

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		<description><![CDATA[Let K be a field of characteristic 0, and let V be a vector space over K of dimension n, and pick k &#60; n. Let X be the Grassmannian Grass(k, V). We&#8217;ll briefly explore the (bounded) derived category of coherent sheaves of X, denoted .
1. Derived category review
For those unfamiliar with derived categories, here&#8217;s [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=concretenonsense.wordpress.com&blog=2918042&post=733&subd=concretenonsense&ref=&feed=1" />]]></description>
			<content:encoded><![CDATA[<div class='snap_preview'><br /><p>Let K be a field of characteristic 0, and let V be a vector space over K of dimension n, and pick k &lt; n. Let X be the Grassmannian Grass(k, V). We&#8217;ll briefly explore the (bounded) derived category of coherent sheaves of X, denoted <img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+D%7D%5Eb%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf D}^b(X)' title='{\bf D}^b(X)' class='latex' />.</p>
<p><strong>1. Derived category review</strong></p>
<p>For those unfamiliar with derived categories, here&#8217;s a quick summary. If A is any Abelian category, set K(A) to be the category of (co)chain complexes of A with the morphisms being chain maps modulo homotopy equivalence. Chain maps which induce isomorphisms are formally inverted, and the result is the derived category <img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+D%7D%28A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf D}(A)' title='{\bf D}(A)' class='latex' /> of A. Usually we only want to consider bounded complexes, or at least complexes with finitely many nonzero (co)homology groups, and in this case we denote the category <img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+D%7D%5Eb%28A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf D}^b(A)' title='{\bf D}^b(A)' class='latex' />. The category is equipped with a shift functor, which just shifts the degrees of a given complex.</p>
<p>One thing we can do is reformulate derived functors. Given a left exact functor <img src='http://l.wordpress.com/latex.php?latex=F+%5Ccolon+A+%5Cto+B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F \colon A \to B' title='F \colon A \to B' class='latex' />, we define its right derived functor <img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+R%7Df+%5Ccolon+%7B%5Cbf+D%7D%5Eb%28A%29+%5Cto+%7B%5Cbf+D%7D%5Eb%28B%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf R}f \colon {\bf D}^b(A) \to {\bf D}^b(B)' title='{\bf R}f \colon {\bf D}^b(A) \to {\bf D}^b(B)' class='latex' /> as follows. Given an object X in A, an injective resolution <img src='http://l.wordpress.com/latex.php?latex=X+%5Cto+I%5E%5Cbullet&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X \to I^\bullet' title='X \to I^\bullet' class='latex' /> of X becomes an isomorphism in <img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+D%7D%5Eb%28A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf D}^b(A)' title='{\bf D}^b(A)' class='latex' /> (considering X as a complex with one nonzero term), so we define <img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+R%7DF%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf R}F(X)' title='{\bf R}F(X)' class='latex' /> to be the complex obtained by applying F to <img src='http://l.wordpress.com/latex.php?latex=I%5E%5Cbullet&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='I^\bullet' title='I^\bullet' class='latex' />. Actually, we don&#8217;t need an injective resolution, we only need a resolution consisting of F-acyclic objects (i.e., the usual right derived functors of F vanish for them). To define <img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+R%7DF&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf R}F' title='{\bf R}F' class='latex' /> on a general complex <img src='http://l.wordpress.com/latex.php?latex=C%5E%5Cbullet&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C^\bullet' title='C^\bullet' class='latex' />, we need to find a double complex <img src='http://l.wordpress.com/latex.php?latex=C%5E%5Cbullet+%5Cto+I%5E%7B%5Cbullet%2C+%5Cbullet%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C^\bullet \to I^{\bullet, \bullet}' title='C^\bullet \to I^{\bullet, \bullet}' class='latex' /> which is term by term an injective resolution for each <img src='http://l.wordpress.com/latex.php?latex=C%5Ei&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C^i' title='C^i' class='latex' /> (these are called Cartan&#8211;Eilenberg resolutions). Then we apply F to the total complex of <img src='http://l.wordpress.com/latex.php?latex=I%5E%7B%5Cbullet%2C+%5Cbullet%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='I^{\bullet, \bullet}' title='I^{\bullet, \bullet}' class='latex' />. A similar story is true for right exact functors G, so we get left derived functors <img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+L%7DG&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf L}G' title='{\bf L}G' class='latex' />. For notation, the left derived functor of the tensor product is denoted <img src='http://l.wordpress.com/latex.php?latex=%5Cstackrel%7B%5Cbf+L%7D%7B%5Cotimes%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\stackrel{\bf L}{\otimes}' title='\stackrel{\bf L}{\otimes}' class='latex' />.<br />
<span id="more-733"></span><br />
The replacement for exact sequences are now exact triangles, which are written as <img src='http://l.wordpress.com/latex.php?latex=A+%5Cto+B+%5Cto+C+%5Cto+A%5B1%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='A \to B \to C \to A[1]' title='A \to B \to C \to A[1]' class='latex' />. The relevant facts are that exact sequences of cochain complexes become exact triangles, and that if we try to calculate cohomology, exact triangles give long exact sequences. Most importantly, the total derived functors are exact in the sense that they preserve exact triangles.</p>
<p>We&#8217;ll need two facts. The first is the derived version of the projection formula. Let <img src='http://l.wordpress.com/latex.php?latex=f+%5Ccolon+X+%5Cto+Y&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f \colon X \to Y' title='f \colon X \to Y' class='latex' /> be a proper morphism of projective schemes, <img src='http://l.wordpress.com/latex.php?latex=E+%5Cin+%7B%5Cbf+D%7D%5Eb%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='E \in {\bf D}^b(X)' title='E \in {\bf D}^b(X)' class='latex' />, and <img src='http://l.wordpress.com/latex.php?latex=F+%5Cin+%7B%5Cbf+D%7D%5Eb%28Y%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F \in {\bf D}^b(Y)' title='F \in {\bf D}^b(Y)' class='latex' />. Then we have</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+R%7Df_%2A+%28E+%5Cstackrel%7B%5Cbf+L%7D%7B%5Cotimes%7D+%7B%5Cbf+L%7Df%5E%2A+F%29+%5Ccong+%7B%5Cbf+R%7Df_%2AE+%5Cstackrel%7B%5Cbf+L%7D%7B%5Cotimes%7D+F&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf R}f_* (E \stackrel{\bf L}{\otimes} {\bf L}f^* F) \cong {\bf R}f_*E \stackrel{\bf L}{\otimes} F' title='{\bf R}f_* (E \stackrel{\bf L}{\otimes} {\bf L}f^* F) \cong {\bf R}f_*E \stackrel{\bf L}{\otimes} F' class='latex' />.</p>
<p>The second is flat base change. If we have a pullback diagram</p>
<p><img src="http://concretenonsense.files.wordpress.com/2009/10/diagram.gif?w=267" alt="" /></p>
<p>with u flat and f proper, then we have a natural isomorphism</p>
<p><img src='http://l.wordpress.com/latex.php?latex=u%5E%2A%7B%5Cbf+R%7Df_%2A+E+%5Ccong+%7B%5Cbf+R%7Dg_%2A+v%5E%2A+E&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='u^*{\bf R}f_* E \cong {\bf R}g_* v^* E' title='u^*{\bf R}f_* E \cong {\bf R}g_* v^* E' class='latex' /></p>
<p>for all <img src='http://l.wordpress.com/latex.php?latex=E+%5Cin+%7B%5Cbf+D%7D%5Eb%28Y%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='E \in {\bf D}^b(Y)' title='E \in {\bf D}^b(Y)' class='latex' />.</p>
<p><strong>2. Exceptional sequences and the Fourier&#8211;Mukai transform</strong></p>
<p>For this post, we&#8217;ll look for a finite set of generators <img src='http://l.wordpress.com/latex.php?latex=%5C%7BE_1%2C+%5Cdots%2C+E_N%5C%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\{E_1, \dots, E_N\}' title='\{E_1, \dots, E_N\}' class='latex' /> of <img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+D%7D%5Eb%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf D}^b(X)' title='{\bf D}^b(X)' class='latex' />, i.e., using only the operations of mapping cones and shifting degrees (so we&#8217;re allowed to take kernels, cokernels, and direct sums also), we can obtain the isomorphism class of every object. More specifically, we will construct an <strong>exceptional sequence</strong>. This means the following things:</p>
<ol>
<li>Every object in the sequence is exceptional: <img src='http://l.wordpress.com/latex.php?latex=%7B%5Crm+Hom%7D%28E_i%2C+E_i%29+%3D+K&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\rm Hom}(E_i, E_i) = K' title='{\rm Hom}(E_i, E_i) = K' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=%7B%5Crm+Ext%7D%5Ek%28E_i%2C+E_i%29+%3D+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\rm Ext}^k(E_i, E_i) = 0' title='{\rm Ext}^k(E_i, E_i) = 0' class='latex' /> for k&gt;0.</li>
<li><img src='http://l.wordpress.com/latex.php?latex=%7B%5Crm+Ext%7D%5Ek%28E_j%2C+E_i%29+%3D+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\rm Ext}^k(E_j, E_i) = 0' title='{\rm Ext}^k(E_j, E_i) = 0' class='latex' /> for <img src='http://l.wordpress.com/latex.php?latex=k+%5Cge+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='k \ge 0' title='k \ge 0' class='latex' /> and i &lt; j.</li>
</ol>
<p>Using the Schubert cell decomposition of the Grassmannian, it can be shown that the length of an exceptional sequence must equal the number of its Schubert varieties (and more generally, this is true for any homogeneous space for a semisimple group, see the Böhning reference below).</p>
<p>The main tool will be the <strong>Fourier&#8211;Mukai transform</strong>. Suppose that Y and Z are any varieties let <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_Y%2C+%5Cpi_Z&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_Y, \pi_Z' title='\pi_Y, \pi_Z' class='latex' /> be the projections from <img src='http://l.wordpress.com/latex.php?latex=Y+%5Ctimes+Z&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='Y \times Z' title='Y \times Z' class='latex' /> to Y and Z, respectively. For <img src='http://l.wordpress.com/latex.php?latex=E+%5Cin+%7B%5Cbf+D%7D%5Eb%28Y+%5Ctimes+Z%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='E \in {\bf D}^b(Y \times Z)' title='E \in {\bf D}^b(Y \times Z)' class='latex' />, we define a map</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5CPhi_%7BY+%5Cto+Z%7D%5EE+%5Ccolon+%7B%5Cbf+D%7D%5Eb%28Y%29+%5Cto+%7B%5Cbf+D%7D%5Eb%28Z%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Phi_{Y \to Z}^E \colon {\bf D}^b(Y) \to {\bf D}^b(Z)' title='\Phi_{Y \to Z}^E \colon {\bf D}^b(Y) \to {\bf D}^b(Z)' class='latex' /></p>
<p><img src='http://l.wordpress.com/latex.php?latex=F+%5Cmapsto+%7B%5Cbf+R%7D+%5Cpi_%7BZ%2C%2A%7D%28%7B%5Cbf+L%7D%5Cpi_Y%5E%2AF+%5Cstackrel%7B%5Cbf+L%7D%7B%5Cotimes%7D+E%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F \mapsto {\bf R} \pi_{Z,*}({\bf L}\pi_Y^*F \stackrel{\bf L}{\otimes} E)' title='F \mapsto {\bf R} \pi_{Z,*}({\bf L}\pi_Y^*F \stackrel{\bf L}{\otimes} E)' class='latex' />.</p>
<p>Since it is a composition of exact functors, the Fourier&#8211;Mukai transform is itself exact. Also, we can let the argument stay fixed and vary the superscript to get another exact functor. So if we have an exact triangle</p>
<p><img src='http://l.wordpress.com/latex.php?latex=E+%5Cto+F+%5Cto+G+%5Cto+E%5B1%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='E \to F \to G \to E[1]' title='E \to F \to G \to E[1]' class='latex' /></p>
<p>in <img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+D%7D%5Eb%28Y+%5Ctimes+Z%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf D}^b(Y \times Z)' title='{\bf D}^b(Y \times Z)' class='latex' />, then we get, for any element <img src='http://l.wordpress.com/latex.php?latex=A+%5Cin+%7B%5Cbf+D%7D%5Eb%28Y%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='A \in {\bf D}^b(Y)' title='A \in {\bf D}^b(Y)' class='latex' />, an exact triangle</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5CPhi%5EE_%7BY+%5Cto+Z%7D%28A%29+%5Cto+%5CPhi%5EF_%7BY+%5Cto+Z%7D%28A%29+%5Cto+%5CPhi%5EG_%7BY+%5Cto+Z%7D%28A%29+%5Cto+%5CPhi%5EE_%7BY+%5Cto+Z%7D%28A%29%5B1%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Phi^E_{Y \to Z}(A) \to \Phi^F_{Y \to Z}(A) \to \Phi^G_{Y \to Z}(A) \to \Phi^E_{Y \to Z}(A)[1]' title='\Phi^E_{Y \to Z}(A) \to \Phi^F_{Y \to Z}(A) \to \Phi^G_{Y \to Z}(A) \to \Phi^E_{Y \to Z}(A)[1]' class='latex' /></p>
<p>in <img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+D%7D%5Eb%28Z%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf D}^b(Z)' title='{\bf D}^b(Z)' class='latex' />. The key point is that in the case that Y=Z, the Fourier&#8211;Mukai transform using the structure sheaf of the diagonal <img src='http://l.wordpress.com/latex.php?latex=%5CPhi_%7BY+%5Cto+Y%7D%5E%7B%5Cmathcal%7BO%7D_%5CDelta%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Phi_{Y \to Y}^{\mathcal{O}_\Delta}' title='\Phi_{Y \to Y}^{\mathcal{O}_\Delta}' class='latex' /> is the identity functor. To see this, let <img src='http://l.wordpress.com/latex.php?latex=i+%5Ccolon+X+%5Cto+X+%5Ctimes+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='i \colon X \to X \times X' title='i \colon X \to X \times X' class='latex' /> be the diagonal embedding. Letting <img src='http://l.wordpress.com/latex.php?latex=p_1%2Cp_2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='p_1,p_2' title='p_1,p_2' class='latex' /> be the two projections, then</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5CPhi_%7BY+%5Cto+Y%7D%5E%7B%7B%5Ccal+O%7D_%5CDelta%7D%28A%29+%3D+%7B%5Cbf+R%7Dp_%7B2%2C%2A%7D%28%7B%5Cbf+L%7Dp_1%5E%2AA+%5Cstackrel%7B%5Cbf+L%7D%7B%5Cotimes%7D_%7B%7B%5Ccal+O%7D_%7BY+%5Ctimes+Y%7D%7D+i_%2A%7B%5Ccal+O%7D_Y%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Phi_{Y \to Y}^{{\cal O}_\Delta}(A) = {\bf R}p_{2,*}({\bf L}p_1^*A \stackrel{\bf L}{\otimes}_{{\cal O}_{Y \times Y}} i_*{\cal O}_Y)' title='\Phi_{Y \to Y}^{{\cal O}_\Delta}(A) = {\bf R}p_{2,*}({\bf L}p_1^*A \stackrel{\bf L}{\otimes}_{{\cal O}_{Y \times Y}} i_*{\cal O}_Y)' class='latex' /></p>
<p><img src='http://l.wordpress.com/latex.php?latex=%3D+%7B%5Cbf+R%7Dp_%7B2%2C%2A%7D%28%7B%5Cbf+R%7Di_%2A%28%7B%5Cbf+L%7Di%5E%2A%7B%5Cbf+L%7Dp_1%5E%2AA+%5Cstackrel%7B%5Cbf+L%7D%7B%5Cotimes%7D_%7B%7B%5Ccal+O%7D_Y%7D+%7B%5Ccal+O%7D_Y%29+%3D+A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='= {\bf R}p_{2,*}({\bf R}i_*({\bf L}i^*{\bf L}p_1^*A \stackrel{\bf L}{\otimes}_{{\cal O}_Y} {\cal O}_Y) = A' title='= {\bf R}p_{2,*}({\bf R}i_*({\bf L}i^*{\bf L}p_1^*A \stackrel{\bf L}{\otimes}_{{\cal O}_Y} {\cal O}_Y) = A' class='latex' />,</p>
<p>where in the last equality, we use that <img src='http://l.wordpress.com/latex.php?latex=p_1+%5Ccirc+i+%3D+p_2+%5Ccirc+i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='p_1 \circ i = p_2 \circ i' title='p_1 \circ i = p_2 \circ i' class='latex' /> is the identity map. In light of this remark and the exactness remark, it makes sense to try to find a resolution for the diagonal if we&#8217;re trying to find a set of generators of <img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+D%7D%5Eb%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf D}^b(X)' title='{\bf D}^b(X)' class='latex' />. So we&#8217;ll do just that.</p>
<p><strong>3. Resolution of the diagonal</strong></p>
<p>Let <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BR%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{R}' title='\mathcal{R}' class='latex' /> be the rank k tautological subbundle of X, and let <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BQ%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{Q}' title='\mathcal{Q}' class='latex' /> be the tautological quotient bundle, so that we have a short exact sequence</p>
<p><img src='http://l.wordpress.com/latex.php?latex=0+%5Cto+%5Cmathcal%7BR%7D+%5Cto+X+%5Ctimes+V+%5Cto+%5Cmathcal%7BQ%7D+%5Cto+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='0 \to \mathcal{R} \to X \times V \to \mathcal{Q} \to 0' title='0 \to \mathcal{R} \to X \times V \to \mathcal{Q} \to 0' class='latex' />.</p>
<p>We&#8217;ll use <img src='http://l.wordpress.com/latex.php?latex=%5Cboxtimes&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\boxtimes' title='\boxtimes' class='latex' /> to denote the exterior tensor product of sheaves on X, i.e., if <img src='http://l.wordpress.com/latex.php?latex=p_i+%5Ccolon+X+%5Ctimes+X+%5Cto+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='p_i \colon X \times X \to X' title='p_i \colon X \times X \to X' class='latex' /> are the two projections, and F and G are two sheaves on X, then <img src='http://l.wordpress.com/latex.php?latex=F+%5Cboxtimes+G+%3D+p_1%5E%2AF+%5Cotimes+p_2%5E%2AG&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F \boxtimes G = p_1^*F \otimes p_2^*G' title='F \boxtimes G = p_1^*F \otimes p_2^*G' class='latex' /> is a sheaf on <img src='http://l.wordpress.com/latex.php?latex=X+%5Ctimes+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X \times X' title='X \times X' class='latex' />.There is a natural map <img src='http://l.wordpress.com/latex.php?latex=p_1%5E%2A+%5Cmathcal%7BR%7D+%5Cto+V+%5Ctimes+X+%5Ctimes+X+%5Cto+p_2%5E%2A+%5Cmathcal%7BQ%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='p_1^* \mathcal{R} \to V \times X \times X \to p_2^* \mathcal{Q}' title='p_1^* \mathcal{R} \to V \times X \times X \to p_2^* \mathcal{Q}' class='latex' /> where the first map identifies the trivial bundle V with <img src='http://l.wordpress.com/latex.php?latex=p_1%5E%2AV&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='p_1^*V' title='p_1^*V' class='latex' /> and is the corresponding inclusion, while the second map identifies V with <img src='http://l.wordpress.com/latex.php?latex=p_2%5E%2A+V&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='p_2^* V' title='p_2^* V' class='latex' /> and is the corresponding projection. Set-theoretically, the zero set of this map is the diagonal <img src='http://l.wordpress.com/latex.php?latex=%5CDelta&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Delta' title='\Delta' class='latex' />, and we can check locally that it also defines the diagonal scheme-theoretically.</p>
<p>So let s be the section of <img src='http://l.wordpress.com/latex.php?latex=%7B%5Ccal+H%7D%7B%5Crm+om%7D%28p_1%5E%2A+%5Cmathcal%7BR%7D%2C+p_2%5E%2A%5Cmathcal%7BQ%7D%29+%3D+%5Cmathcal%7BR%7D%5E%2A+%5Cboxtimes+%5Cmathcal%7BQ%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\cal H}{\rm om}(p_1^* \mathcal{R}, p_2^*\mathcal{Q}) = \mathcal{R}^* \boxtimes \mathcal{Q}' title='{\cal H}{\rm om}(p_1^* \mathcal{R}, p_2^*\mathcal{Q}) = \mathcal{R}^* \boxtimes \mathcal{Q}' class='latex' /> corresponding to this map. We get a Koszul complex</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+0+%5Cto+%5Cbigwedge%5E%7Bk%28n-k%29%7D+%28%5Cmathcal%7BR%7D+%5Cboxtimes+%5Cmathcal%7BQ%7D%5E%2A%29+%5Cto+%5Ccdots+%5Cto+%5Cbigwedge%5E2+%28%5Cmathcal%7BR%7D+%5Cboxtimes+%5Cmathcal%7BQ%7D%5E%2A%29+%5Cto+%5Cmathcal%7BR%7D+%5Cboxtimes+%5Cmathcal%7BQ%7D%5E%2A+%5Cto+%5Cmathcal%7BO%7D_%5CDelta&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle 0 \to \bigwedge^{k(n-k)} (\mathcal{R} \boxtimes \mathcal{Q}^*) \to \cdots \to \bigwedge^2 (\mathcal{R} \boxtimes \mathcal{Q}^*) \to \mathcal{R} \boxtimes \mathcal{Q}^* \to \mathcal{O}_\Delta' title='\displaystyle 0 \to \bigwedge^{k(n-k)} (\mathcal{R} \boxtimes \mathcal{Q}^*) \to \cdots \to \bigwedge^2 (\mathcal{R} \boxtimes \mathcal{Q}^*) \to \mathcal{R} \boxtimes \mathcal{Q}^* \to \mathcal{O}_\Delta' class='latex' /> (*)</p>
<p>which is exact: <img src='http://l.wordpress.com/latex.php?latex=%5CDelta&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Delta' title='\Delta' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=X+%5Ctimes+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X \times X' title='X \times X' class='latex' /> are nonsingular, so <img src='http://l.wordpress.com/latex.php?latex=%5CDelta&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Delta' title='\Delta' class='latex' /> is locally a complete intersection in <img src='http://l.wordpress.com/latex.php?latex=X+%5Ctimes+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X \times X' title='X \times X' class='latex' />. This idea is due to Beilinson, who did it for the case of projective space. The argument was extended to Grassmannians by Kapranov.</p>
<p><strong>4. Finishing things up</strong></p>
<p>Now we can splice (*) into exact triangles. To use the Fourier&#8211;Mukai transform, we have to decide if we&#8217;re going from the first factor to the second, or vice versa (there is an asymmetry in the terms of (*), so this matters). Both choices will give a different set of generators. For now, let&#8217;s go from the second factor to the first. Since the characteristic of K is zero, we get the decomposition</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+%5Cbigwedge%5Ei%28%5Cmathcal%7BR%7D%5E%2A+%5Cboxtimes+%5Cmathcal%7BQ%7D%29+%3D+%5Cbigoplus_%7B%7C%5Clambda%7C+%3D+i%7D+%7B%5Cbf+S%7D_%5Clambda%28%5Cmathcal%7BR%7D%5E%2A%29+%5Cboxtimes+%7B%5Cbf+S%7D_%7B%5Clambda%27%7D%28%5Cmathcal%7BQ%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle \bigwedge^i(\mathcal{R}^* \boxtimes \mathcal{Q}) = \bigoplus_{|\lambda| = i} {\bf S}_\lambda(\mathcal{R}^*) \boxtimes {\bf S}_{\lambda&#039;}(\mathcal{Q})' title='\displaystyle \bigwedge^i(\mathcal{R}^* \boxtimes \mathcal{Q}) = \bigoplus_{|\lambda| = i} {\bf S}_\lambda(\mathcal{R}^*) \boxtimes {\bf S}_{\lambda&#039;}(\mathcal{Q})' class='latex' /></p>
<p>where the sum is over partitions of size i, <img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+S%7D_%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf S}_\lambda' title='{\bf S}_\lambda' class='latex' /> denotes a Schur functor, and <img src='http://l.wordpress.com/latex.php?latex=%5Clambda%27&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda&#039;' title='\lambda&#039;' class='latex' /> is the transpose partition to <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />. This decomposition is the dual Cauchy identity, and is a consequence, for example, of the dual Robinson&#8211;Schensted&#8211;Knuth correspondence. If the field has positive characteristic, then we only get a filtration of the LHS whose associated graded is the RHS. Of course, if k=1, this is irrelevant.</p>
<p>Now pick any object <img src='http://l.wordpress.com/latex.php?latex=A+%5Cin+%7B%5Cbf+D%7D%5Eb%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='A \in {\bf D}^b(X)' title='A \in {\bf D}^b(X)' class='latex' />. If we want to generate A, we can apply the Fourier&#8211;Mukai transform to A using the exact triangles we got by splicing (*). This shows that the set <img src='http://l.wordpress.com/latex.php?latex=%5C%7B+%5CPhi%5E%7BE_%5Clambda%7D_%7BX+%5Cto+X%7D%28A%29+%5C%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\{ \Phi^{E_\lambda}_{X \to X}(A) \}' title='\{ \Phi^{E_\lambda}_{X \to X}(A) \}' class='latex' /> generates A, where <img src='http://l.wordpress.com/latex.php?latex=E_%5Clambda+%3D+%7B%5Cbf+S%7D_%5Clambda%28%5Cmathcal%7BR%7D%5E%2A%29+%5Cboxtimes+%7B%5Cbf+S%7D_%7B%5Clambda%27%7D%28%5Cmathcal%7BQ%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='E_\lambda = {\bf S}_\lambda(\mathcal{R}^*) \boxtimes {\bf S}_{\lambda&#039;}(\mathcal{Q})' title='E_\lambda = {\bf S}_\lambda(\mathcal{R}^*) \boxtimes {\bf S}_{\lambda&#039;}(\mathcal{Q})' class='latex' /> and the set is over all <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' /> which fit in the <img src='http://l.wordpress.com/latex.php?latex=k+%5Ctimes+%28n-k%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='k \times (n-k)' title='k \times (n-k)' class='latex' /> rectangle. Ranging over all A, this is an infinite set, but we can simplify further:</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+%5CPhi%5E%7BE_%5Clambda%7D_%7BX+%5Cto+X%7D%28A%29+%3D+%7B%5Cbf+R%7Dp_%7B1%2C%2A%7D%28%7B%5Cbf+L%7Dp_2%5E%2A%28A%29+%5Cstackrel%7B%5Cbf+L%7D%7B%5Cotimes%7D+%7B%5Cbf+L%7Dp_1%5E%2A%28%7B%5Cbf+S%7D_%5Clambda%28%5Cmathcal%7BR%7D%5E%2A%29%29+%5Cstackrel%7B%5Cbf+L%7D%7B%5Cotimes%7D+%7B%5Cbf+L%7Dp_2%5E%2A%28%7B%5Cbf+S%7D_%7B%5Clambda%27%7D%28%5Cmathcal%7BQ%7D%29%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle \Phi^{E_\lambda}_{X \to X}(A) = {\bf R}p_{1,*}({\bf L}p_2^*(A) \stackrel{\bf L}{\otimes} {\bf L}p_1^*({\bf S}_\lambda(\mathcal{R}^*)) \stackrel{\bf L}{\otimes} {\bf L}p_2^*({\bf S}_{\lambda&#039;}(\mathcal{Q})))' title='\displaystyle \Phi^{E_\lambda}_{X \to X}(A) = {\bf R}p_{1,*}({\bf L}p_2^*(A) \stackrel{\bf L}{\otimes} {\bf L}p_1^*({\bf S}_\lambda(\mathcal{R}^*)) \stackrel{\bf L}{\otimes} {\bf L}p_2^*({\bf S}_{\lambda&#039;}(\mathcal{Q})))' class='latex' /></p>
<p>by definition, and using the projection formula, this is isomorphic to</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+S%7D_%7B%5Clambda%7D%28%5Cmathcal%7BR%7D%5E%2A%29+%5Cstackrel%7B%5Cbf+L%7D%7B%5Cotimes%7D+%7B%5Cbf+R%7Dp_%7B1%2C%2A%7D+%7B%5Cbf+L%7Dp_2%5E%2A%28A+%5Cstackrel%7B%5Cbf+L%7D%7B%5Cotimes%7D+%7B%5Cbf+S%7D_%7B%5Clambda%27%7D%28%5Cmathcal%7BQ%7D%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf S}_{\lambda}(\mathcal{R}^*) \stackrel{\bf L}{\otimes} {\bf R}p_{1,*} {\bf L}p_2^*(A \stackrel{\bf L}{\otimes} {\bf S}_{\lambda&#039;}(\mathcal{Q}))' title='{\bf S}_{\lambda}(\mathcal{R}^*) \stackrel{\bf L}{\otimes} {\bf R}p_{1,*} {\bf L}p_2^*(A \stackrel{\bf L}{\otimes} {\bf S}_{\lambda&#039;}(\mathcal{Q}))' class='latex' />.</p>
<p>Using flat base change (with the notation in the above diagram, we have <img src='http://l.wordpress.com/latex.php?latex=Z+%3D+%7B%5Crm+Spec%7D%28K%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='Z = {\rm Spec}(K)' title='Z = {\rm Spec}(K)' class='latex' />, <img src='http://l.wordpress.com/latex.php?latex=Y+%3D+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='Y = X' title='Y = X' class='latex' />, <img src='http://l.wordpress.com/latex.php?latex=v+%3D+p_2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v = p_2' title='v = p_2' class='latex' />, and <img src='http://l.wordpress.com/latex.php?latex=g+%3D+p_1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g = p_1' title='g = p_1' class='latex' />), the above can be replaced by derived global sections:</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+S%7D_%5Clambda%28%5Cmathcal%7BR%7D%5E%2A%29+%5Cotimes+%7B%5Cbf+R%7D%5CGamma%28X%3B+A+%5Cstackrel%7B%5Cbf+L%7D%7B%5Cotimes%7D+%7B%5Cbf+S%7D_%7B%5Clambda%27%7D%28%5Cmathcal%7BQ%7D%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf S}_\lambda(\mathcal{R}^*) \otimes {\bf R}\Gamma(X; A \stackrel{\bf L}{\otimes} {\bf S}_{\lambda&#039;}(\mathcal{Q}))' title='{\bf S}_\lambda(\mathcal{R}^*) \otimes {\bf R}\Gamma(X; A \stackrel{\bf L}{\otimes} {\bf S}_{\lambda&#039;}(\mathcal{Q}))' class='latex' />,</p>
<p>where the second factor is isomorphic to a cochain complex consisting of its cohomology groups with zero differentials. Hence we see that the Fourier&#8211;Mukai transform is a complex consisting of copies of <img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+S%7D_%5Clambda%28%5Cmathcal%7BR%7D%5E%2A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf S}_\lambda(\mathcal{R}^*)' title='{\bf S}_\lambda(\mathcal{R}^*)' class='latex' /> in various degrees. So we see that <img src='http://l.wordpress.com/latex.php?latex=%5C%7B+%7B%5Cbf+S%7D_%5Clambda%28%5Cmathcal%7BR%7D%5E%2A%29+%5C%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\{ {\bf S}_\lambda(\mathcal{R}^*) \}' title='\{ {\bf S}_\lambda(\mathcal{R}^*) \}' class='latex' /> is a generating set, where <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' /> ranges over all partitions fitting inside of the <img src='http://l.wordpress.com/latex.php?latex=k+%5Ctimes+%28n-k%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='k \times (n-k)' title='k \times (n-k)' class='latex' /> box.</p>
<p>On the other hand, if we did the Fourier&#8211;Mukai transform going from the first factor to the second factor, we would get <img src='http://l.wordpress.com/latex.php?latex=%5C%7B+%7B%5Cbf+S%7D_%5Clambda%28%5Cmathcal%7BQ%7D%29+%5C%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\{ {\bf S}_\lambda(\mathcal{Q}) \}' title='\{ {\bf S}_\lambda(\mathcal{Q}) \}' class='latex' /> as a set of generators, where <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' /> ranges over all partitions which fit inside of the <img src='http://l.wordpress.com/latex.php?latex=%28n-k%29+%5Ctimes+k&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(n-k) \times k' title='(n-k) \times k' class='latex' /> box.</p>
<p>The last thing to check is that we get an exceptional sequence. We have a partial ordering: <img src='http://l.wordpress.com/latex.php?latex=%7B%5Cbf+S%7D_%5Clambda%28%5Cmathcal%7BR%7D%5E%2A%29+%5Cle+%7B%5Cbf+S%7D_%5Cmu%28%5Cmathcal%7BR%7D%5E%2A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{\bf S}_\lambda(\mathcal{R}^*) \le {\bf S}_\mu(\mathcal{R}^*)' title='{\bf S}_\lambda(\mathcal{R}^*) \le {\bf S}_\mu(\mathcal{R}^*)' class='latex' /> whenever <img src='http://l.wordpress.com/latex.php?latex=%5Clambda_i+%5Cle+%5Cmu_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda_i \le \mu_i' title='\lambda_i \le \mu_i' class='latex' /> for all i. Extending this to a total order will do the trick. To check that all of the appropriate Ext groups vanish, we need to use the Borel&#8211;Weil&#8211;Bott theorem, but I will omit this task.</p>
<p><strong>References</strong></p>
<ul>
<li>Christian Böhning, <a href="http://www.mathematik.uni-bielefeld.de/documenta/vol-11/11.pdf">Derived categories of coherent sheaves on rational homogeneous manifolds</a></li>
<li>Andrei Caldararu, <a href="http://arxiv.org/abs/math/0501094">Derived categories of sheaves: a skimming</a></li>
<li>D. Huybrechts, <em>Fourier-Mukai transforms in algebraic geometry</em> (book)</li>
<li>M. M. Kapranov, <a href="http://www.springerlink.com/content/k27qgh12842q662n/">On the derived categories of coherent sheaves on some homogeneous spaces</a></li>
</ul>
<p>-Steven</p>
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		<title>Tangent bundle of the Grassmannian</title>
		<link>http://concretenonsense.wordpress.com/2009/08/17/tangent-bundle-of-the-grassmannian/</link>
		<comments>http://concretenonsense.wordpress.com/2009/08/17/tangent-bundle-of-the-grassmannian/#comments</comments>
		<pubDate>Mon, 17 Aug 2009 13:35:20 +0000</pubDate>
		<dc:creator>Steven Sam</dc:creator>
				<category><![CDATA[Algebraic Geometry]]></category>
		<category><![CDATA[grassmannian]]></category>
		<category><![CDATA[tangent space]]></category>
		<category><![CDATA[functor of points]]></category>

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		<description><![CDATA[This post will be an exercise in algebraic (differential) geometry: I&#8217;ll calculate the tangent bundle of the Grassmannian  of r-dimensional subspaces of a fixed vector space E defined over a field k. We&#8217;ll deduce from this that Grassmannians are Fano varieties.
The two methods will be similar, but working in the differential category requires less [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=concretenonsense.wordpress.com&blog=2918042&post=582&subd=concretenonsense&ref=&feed=1" />]]></description>
			<content:encoded><![CDATA[<div class='snap_preview'><br /><p>This post will be an exercise in algebraic (differential) geometry: I&#8217;ll calculate the tangent bundle of the <a href="http://en.wikipedia.org/wiki/Grassmannian">Grassmannian</a> <img src='http://l.wordpress.com/latex.php?latex=X+%3D+%5Cmathbf%7BGr%7D%28r%2CE%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X = \mathbf{Gr}(r,E)' title='X = \mathbf{Gr}(r,E)' class='latex' /> of r-dimensional subspaces of a fixed vector space E defined over a field k. We&#8217;ll deduce from this that Grassmannians are <a href="http://en.wikipedia.org/wiki/Fano_variety">Fano varieties</a>.</p>
<p>The two methods will be similar, but working in the differential category requires less machinery, so we&#8217;ll assume k is the real numbers first. In this case, we&#8217;ll use the <a href="http://en.wikipedia.org/wiki/Tangent_space#Definition_as_directions_of_curves">definition of tangent spaces</a> at a point x as the tangent vectors of curves starting at x. We&#8217;ll need the tautological bundle R on X, which is the subbundle of E x X given by <img src='http://l.wordpress.com/latex.php?latex=%5C%7B%28x%2CW%29+%5Cmid+x+%5Cin+W%5C%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\{(x,W) \mid x \in W\}' title='\{(x,W) \mid x \in W\}' class='latex' />. The quotient bundle <img src='http://l.wordpress.com/latex.php?latex=%28E+%5Ctimes+X%29+%2F+R&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(E \times X) / R' title='(E \times X) / R' class='latex' /> will be denoted Q. Recall that the <a href="http://en.wikipedia.org/wiki/Plucker_embedding">Plücker embedding</a> is a map <img src='http://l.wordpress.com/latex.php?latex=X+%5Cto+%5Cmathbf%7BP%7D%28%5Cbigwedge%5Er+E%29+%3D+P&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X \to \mathbf{P}(\bigwedge^r E) = P' title='X \to \mathbf{P}(\bigwedge^r E) = P' class='latex' /> sends a subspace W of E to its rth exterior power <img src='http://l.wordpress.com/latex.php?latex=%5Cbigwedge%5Er+W&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\bigwedge^r W' title='\bigwedge^r W' class='latex' />. Under this embedding, the line bundle <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BO%7D%281%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{O}(1)' title='\mathcal{O}(1)' class='latex' /> on P restricts to <img src='http://l.wordpress.com/latex.php?latex=%5Cbigwedge%5Er+R%5E%2A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\bigwedge^r R^*' title='\bigwedge^r R^*' class='latex' /> since <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BO%7D%28-1%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{O}(-1)' title='\mathcal{O}(-1)' class='latex' /> is the tautological subbundle of <img src='http://l.wordpress.com/latex.php?latex=%5Cbigwedge%5Er+E+%5Ctimes+P&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\bigwedge^r E \times P' title='\bigwedge^r E \times P' class='latex' />.<br />
<span id="more-582"></span><br />
The image of X under the Plücker embedding are precisely all lines in P which have a generator of the form <img src='http://l.wordpress.com/latex.php?latex=e_1+%5Cwedge+%5Ccdots+%5Cwedge+e_r&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='e_1 \wedge \cdots \wedge e_r' title='e_1 \wedge \cdots \wedge e_r' class='latex' /> for <img src='http://l.wordpress.com/latex.php?latex=e_i+%5Cin+E&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='e_i \in E' title='e_i \in E' class='latex' />. So pick a point <img src='http://l.wordpress.com/latex.php?latex=W+%3D+%5Clangle+e_1+%5Cwedge+%5Ccdots+%5Cwedge+e_r+%5Crangle&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='W = \langle e_1 \wedge \cdots \wedge e_r \rangle' title='W = \langle e_1 \wedge \cdots \wedge e_r \rangle' class='latex' /> of X. Complete <img src='http://l.wordpress.com/latex.php?latex=%5C%7Be_1%2C+%5Cdots%2C+e_r+%5C%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\{e_1, \dots, e_r \}' title='\{e_1, \dots, e_r \}' class='latex' /> to a basis <img src='http://l.wordpress.com/latex.php?latex=%5C%7Be_1%2C+%5Cdots%2C+e_n%5C%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\{e_1, \dots, e_n\}' title='\{e_1, \dots, e_n\}' class='latex' /> of E. Given a map <img src='http://l.wordpress.com/latex.php?latex=%5Cphi+%5Ccolon+W+%5Cto+E&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi \colon W \to E' title='\phi \colon W \to E' class='latex' />, we can define a curve <img src='http://l.wordpress.com/latex.php?latex=%5Cphi_c+%5Ccolon+%5B-1%2C1%5D+%5Cto+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi_c \colon [-1,1] \to X' title='\phi_c \colon [-1,1] \to X' class='latex' /> by <img src='http://l.wordpress.com/latex.php?latex=%5Cphi_c%28t%29+%3D+%5Clangle+%28e_1+%2B+t%5Cphi%28e_1%29%29+%5Cwedge+%5Ccdots+%5Cwedge+%28e_r+%2B+t%5Cphi%28e_r%29%29+%5Crangle&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi_c(t) = \langle (e_1 + t\phi(e_1)) \wedge \cdots \wedge (e_r + t\phi(e_r)) \rangle' title='\phi_c(t) = \langle (e_1 + t\phi(e_1)) \wedge \cdots \wedge (e_r + t\phi(e_r)) \rangle' class='latex' />. Since <img src='http://l.wordpress.com/latex.php?latex=%5Cphi_c%280%29+%3D+W&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi_c(0) = W' title='\phi_c(0) = W' class='latex' />, this determines a tangent vector <img src='http://l.wordpress.com/latex.php?latex=%5Cphi%27_c%280%29+%3D+%5Clangle+%5Csum_%7Bi%3D1%7D%5Er+%28e_1+%5Cwedge+%5Ccdots+%5Cwedge+%5Cphi%28e_i%29+%5Cwedge+%5Ccdots+%5Cwedge+e_r%29+%5Crangle&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi&#039;_c(0) = \langle \sum_{i=1}^r (e_1 \wedge \cdots \wedge \phi(e_i) \wedge \cdots \wedge e_r) \rangle' title='\phi&#039;_c(0) = \langle \sum_{i=1}^r (e_1 \wedge \cdots \wedge \phi(e_i) \wedge \cdots \wedge e_r) \rangle' class='latex' />. Two curves given by <img src='http://l.wordpress.com/latex.php?latex=%5Cphi_c%2C+%5Cpsi_c&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi_c, \psi_c' title='\phi_c, \psi_c' class='latex' /> determine the same tangent vector if and only if the image of their difference <img src='http://l.wordpress.com/latex.php?latex=%5Cphi+-+%5Cpsi&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi - \psi' title='\phi - \psi' class='latex' /> lies in <img src='http://l.wordpress.com/latex.php?latex=W%27+%3D+%5Clangle+e_1%2C+%5Cdots%2C+e_r+%5Crangle&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='W&#039; = \langle e_1, \dots, e_r \rangle' title='W&#039; = \langle e_1, \dots, e_r \rangle' class='latex' />, so the tangent space naturally contains Hom(W&#8217;, E/W&#8217;) as a subspace. But this subspace has dimension r(n-r), which is the dimension of X, so in fact they are equal. Hence we conclude that the tangent bundle of X is Hom(R, Q). </p>
<p>How do we turn the above analytic argument into an algebraic one for an arbitrary field? Recall that the <a href="http://en.wikipedia.org/wiki/Zariski_tangent_space">Zariski tangent space</a> of a scheme X at a point p is defined to be <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BHom%7D_%7B%5Ckappa%28p%29%7D%28%5Cmathfrak%7Bm%7D_p+%2F+%5Cmathfrak%7Bm%7D_p%5E2%2C+%5Ckappa%28p%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{Hom}_{\kappa(p)}(\mathfrak{m}_p / \mathfrak{m}_p^2, \kappa(p))' title='\mathrm{Hom}_{\kappa(p)}(\mathfrak{m}_p / \mathfrak{m}_p^2, \kappa(p))' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=%5Cmathfrak%7Bm%7D_p&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathfrak{m}_p' title='\mathfrak{m}_p' class='latex' /> is the maximal ideal of the local ring <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BO%7D_%7BX%2Cp%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{O}_{X,p}' title='\mathcal{O}_{X,p}' class='latex' />, and <img src='http://l.wordpress.com/latex.php?latex=%5Ckappa%28p%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\kappa(p)' title='\kappa(p)' class='latex' /> is the residue field <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BO%7D_%7BX%2Cp%7D+%2F+%5Cmathfrak%7Bm%7D_p&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{O}_{X,p} / \mathfrak{m}_p' title='\mathcal{O}_{X,p} / \mathfrak{m}_p' class='latex' />. In the case that X is a scheme over a field k, and p is a k-rational point (i.e., its residue field is k), tangent vectors at p are equivalent to maps <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7BSpec+%7D%28k%5B%5Cvarepsilon%5D+%2F+%28%5Cvarepsilon%29%5E2%29+%5Cto+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{Spec }(k[\varepsilon] / (\varepsilon)^2) \to X' title='\text{Spec }(k[\varepsilon] / (\varepsilon)^2) \to X' class='latex' /> whose image is p. For simplicity of notation, set <img src='http://l.wordpress.com/latex.php?latex=S+%3D+k%5B%5Cvarepsilon%5D+%2F+%28%5Cvarepsilon%29%5E2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S = k[\varepsilon] / (\varepsilon)^2' title='S = k[\varepsilon] / (\varepsilon)^2' class='latex' />. This definition seems harder to understand, but we&#8217;ll see that it&#8217;s the natural one to use in the case of the Grassmannian. </p>
<p>This is true because the <a href="http://en.wikipedia.org/wiki/Functor_of_points">functor of points</a> Hom(&#8211;, X) of the Grassmannian has a nice description. To be specific, let F be the functor which sends a k-scheme Y to the set of all rank r locally free subsheaves <img src='http://l.wordpress.com/latex.php?latex=L+%5Csubseteq+%5Cmathcal%7BO%7D_Y+%5Cotimes+E&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='L \subseteq \mathcal{O}_Y \otimes E' title='L \subseteq \mathcal{O}_Y \otimes E' class='latex' /> whose quotient is also locally free. Then F is isomorphic to Hom(&#8211;, X). (Given a map <img src='http://l.wordpress.com/latex.php?latex=Y+%5Cto+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='Y \to X' title='Y \to X' class='latex' />, we get such a subsheaf L by pulling back the tautological sequence <img src='http://l.wordpress.com/latex.php?latex=0+%5Cto+R+%5Cto+E+%5Ctimes+X+%5Cto+Q+%5Cto+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='0 \to R \to E \times X \to Q \to 0' title='0 \to R \to E \times X \to Q \to 0' class='latex' /> from X, and conversely, every choice of L induces a map from Y to X). All closed points of the Grassmannian are k-rational. Using this language, X = F(Spec k), and for a closed point p of X, the tangent space is the fiber of p under the map <img src='http://l.wordpress.com/latex.php?latex=T+%5Ccolon+F%28%5Ctext%7BSpec+%7D+S%29+%5Cto+F%28%5Ctext%7BSpec+%7D+k%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='T \colon F(\text{Spec } S) \to F(\text{Spec } k)' title='T \colon F(\text{Spec } S) \to F(\text{Spec } k)' class='latex' />, which is obtained by applying <img src='http://l.wordpress.com/latex.php?latex=F+%5Ccirc+%5Ctext%7BSpec%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F \circ \text{Spec}' title='F \circ \text{Spec}' class='latex' /> to the quotient map <img src='http://l.wordpress.com/latex.php?latex=S+%5Cto+k&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S \to k' title='S \to k' class='latex' />. </p>
<p>A closed point of F(Spec k) is just a dimension r subspace of W of E whose quotient is free (this condition is automatic), and so the fiber under T is just all rank r locally free subsheaves of <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BO%7D_%7B%5Ctext%7BSpec+%7D+S%7D%5En&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{O}_{\text{Spec } S}^n' title='\mathcal{O}_{\text{Spec } S}^n' class='latex' /> whose quotient is locally free, and whose pullback under the map <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7BSpec+%7D+k+%5Cto+%5Ctext%7BSpec+%7D+S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{Spec } k \to \text{Spec } S' title='\text{Spec } k \to \text{Spec } S' class='latex' /> is W. Locally free sheaves on Spec S are equivalent to finitely generated projective S-modules, and since S is local, all such modules are free. Hence we have reduced to the following situation: find all free S-submodules M of <img src='http://l.wordpress.com/latex.php?latex=S%5En&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S^n' title='S^n' class='latex' /> whose quotient is free, and such that upon specializing <img src='http://l.wordpress.com/latex.php?latex=%5Cvarepsilon+%3D+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\varepsilon = 0' title='\varepsilon = 0' class='latex' />, M becomes W. </p>
<p>This is very similar to writing down tangent vectors for curves: let <img src='http://l.wordpress.com/latex.php?latex=%5Cphi+%5Ccolon+W+%5Cto+E&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi \colon W \to E' title='\phi \colon W \to E' class='latex' /> be any linear map. Identifying <img src='http://l.wordpress.com/latex.php?latex=S%5En&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S^n' title='S^n' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=E+%5Coplus+%5Cvarepsilon+E&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='E \oplus \varepsilon E' title='E \oplus \varepsilon E' class='latex' /> as vector spaces, we can define <img src='http://l.wordpress.com/latex.php?latex=M_%5Cphi+%3D+%5C%7B+x+%2B+%5Cvarepsilon+%5Cphi%28x%29%2C+%5Cvarepsilon+x+%5Cmid+x+%5Cin+W+%5C%7D+%5Csubset+S%5En&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='M_\phi = \{ x + \varepsilon \phi(x), \varepsilon x \mid x \in W \} \subset S^n' title='M_\phi = \{ x + \varepsilon \phi(x), \varepsilon x \mid x \in W \} \subset S^n' class='latex' />. This is a free S-submodule of <img src='http://l.wordpress.com/latex.php?latex=S%5En&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S^n' title='S^n' class='latex' /> with a basis given by any basis of W, and <img src='http://l.wordpress.com/latex.php?latex=M_%5Cphi+%3D+M_%7B%5Cpsi%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='M_\phi = M_{\psi}' title='M_\phi = M_{\psi}' class='latex' /> if and only if the image of the difference <img src='http://l.wordpress.com/latex.php?latex=%5Cphi+-+%5Cpsi&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi - \psi' title='\phi - \psi' class='latex' /> lies in W. So again we&#8217;ve concluded that Hom(W, E/W) is a subspace of the Zariski tangent space of W, which again must be whole thing by dimension counting since the Grassmannian is nonsingular.</p>
<p>Conclusion: the tangent bundle <img src='http://l.wordpress.com/latex.php?latex=T_X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='T_X' title='T_X' class='latex' /> of the Grassmannian is <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7BHom%7D%28R%2C+Q%29+%3D+R%5E%2A+%5Cotimes+Q&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{Hom}(R, Q) = R^* \otimes Q' title='\text{Hom}(R, Q) = R^* \otimes Q' class='latex' />, and hence the cotangent bundle is <img src='http://l.wordpress.com/latex.php?latex=%5COmega%5E1_X+%3D+R+%5Cotimes+Q%5E%2A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Omega^1_X = R \otimes Q^*' title='\Omega^1_X = R \otimes Q^*' class='latex' />. Taking the highest exterior power (determinant), the canonical bundle is <img src='http://l.wordpress.com/latex.php?latex=%5Comega_X+%3D+%28%5Cdet+R%29%5E%7B%5Cotimes+%28n-r%29%7D+%5Cotimes+%28%5Cdet+Q%5E%2A%29%5E%7B%5Cotimes+r%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\omega_X = (\det R)^{\otimes (n-r)} \otimes (\det Q^*)^{\otimes r}' title='\omega_X = (\det R)^{\otimes (n-r)} \otimes (\det Q^*)^{\otimes r}' class='latex' />. But using the short exact sequence <img src='http://l.wordpress.com/latex.php?latex=0+%5Cto+R+%5Cto+E+%5Ctimes+X+%5Cto+Q+%5Cto+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='0 \to R \to E \times X \to Q \to 0' title='0 \to R \to E \times X \to Q \to 0' class='latex' />, we see that det R and det Q are dual bundles. Recall from above also that det R is O(-1) under the Plücker embedding, so the canonical bundle simplifies to <img src='http://l.wordpress.com/latex.php?latex=%5Comega_X+%3D+%5Cmathcal%7BO%7D%28-n%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\omega_X = \mathcal{O}(-n)' title='\omega_X = \mathcal{O}(-n)' class='latex' />. In particular, the anticanonical bundle is <img src='http://l.wordpress.com/latex.php?latex=%5Comega%5E%2A_X+%3D+%5Cmathcal%7BO%7D%28n%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\omega^*_X = \mathcal{O}(n)' title='\omega^*_X = \mathcal{O}(n)' class='latex' />, which is very ample, and hence Grassmannians are Fano varieties (by definition, this means that the anticanonical bundle is ample).</p>
<p>-Steven</p>
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			<media:title type="html">masnevets</media:title>
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		<title>Chern classes and Riemann&#8211;Roch formalism</title>
		<link>http://concretenonsense.wordpress.com/2009/08/03/chern-classes-and-riemann-roch-formalism/</link>
		<comments>http://concretenonsense.wordpress.com/2009/08/03/chern-classes-and-riemann-roch-formalism/#comments</comments>
		<pubDate>Mon, 03 Aug 2009 13:10:22 +0000</pubDate>
		<dc:creator>Steven Sam</dc:creator>
				<category><![CDATA[Algebra]]></category>
		<category><![CDATA[Algebraic Geometry]]></category>
		<category><![CDATA[Chern classes]]></category>
		<category><![CDATA[K-theory]]></category>
		<category><![CDATA[lambda rings]]></category>
		<category><![CDATA[Riemann-Roch]]></category>

		<guid isPermaLink="false">http://concretenonsense.wordpress.com/?p=544</guid>
		<description><![CDATA[Last time I gave the definition of -rings and tried to motivate them from the perspective of K-theory. I&#8217;d like to continue with how to define abstract Chern classes for -rings and explain Riemann&#8211;Roch formalism. We&#8217;ll assume all -rings R have an augmentation, are equipped with a positive structure, and have an involution. I&#8217;ll once [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=concretenonsense.wordpress.com&blog=2918042&post=544&subd=concretenonsense&ref=&feed=1" />]]></description>
			<content:encoded><![CDATA[<div class='snap_preview'><br /><p><a href="http://concretenonsense.wordpress.com/2009/07/23/lambda-rings/">Last time</a> I gave the definition of <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-rings and tried to motivate them from the perspective of K-theory. I&#8217;d like to continue with how to define abstract Chern classes for <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-rings and explain Riemann&#8211;Roch formalism. We&#8217;ll assume all <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-rings R have an augmentation, are equipped with a positive structure, and have an involution. I&#8217;ll once again use K-theory as motivation for the definitions.</p>
<p>In topological K-theory, if we have a space X with a vector bundle E, there exists a map <img src='http://l.wordpress.com/latex.php?latex=f+%5Ccolon+X%27+%5Cto+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f \colon X&#039; \to X' title='f \colon X&#039; \to X' class='latex' /> such that the pullback <img src='http://l.wordpress.com/latex.php?latex=f%5E%2AE&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f^*E' title='f^*E' class='latex' /> decomposes into a direct sum of line bundles, and the map on cohomology rings <img src='http://l.wordpress.com/latex.php?latex=f%5E%2A+%5Ccolon+%5Cmathrm%7BH%7D%5E%2A%28X%29+%5Cto+%5Cmathrm%7BH%7D%5E%2A%28X%27%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f^* \colon \mathrm{H}^*(X) \to \mathrm{H}^*(X&#039;)' title='f^* \colon \mathrm{H}^*(X) \to \mathrm{H}^*(X&#039;)' class='latex' /> is injective. The corresponding statement for <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-rings is that we can embed any <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-ring R into a larger one such that every element can be written as a sum of elements with augmentation <img src='http://l.wordpress.com/latex.php?latex=%5Cpm+1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pm 1' title='\pm 1' class='latex' />.<br />
<span id="more-544"></span><br />
Let <img src='http://l.wordpress.com/latex.php?latex=A+%3D+%5Cbigoplus_%7Bd+%5Cge+0%7D+A_d&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='A = \bigoplus_{d \ge 0} A_d' title='A = \bigoplus_{d \ge 0} A_d' class='latex' /> be a graded ring. We let <img src='http://l.wordpress.com/latex.php?latex=1%2BA%5E%2B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1+A^+' title='1+A^+' class='latex' /> be the group under multiplication of formal power series of the form <img src='http://l.wordpress.com/latex.php?latex=1+%2B+%5Csum_%7Bn+%5Cge+0%7D+a_n+t%5En&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1 + \sum_{n \ge 0} a_n t^n' title='1 + \sum_{n \ge 0} a_n t^n' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=a_n+%5Cin+A_n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a_n \in A_n' title='a_n \in A_n' class='latex' />. A map of Abelian groups <img src='http://l.wordpress.com/latex.php?latex=c_t+%5Ccolon+R+%5Cto+1%2BA%5E%2B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='c_t \colon R \to 1+A^+' title='c_t \colon R \to 1+A^+' class='latex' /> (we use addition for R), written <img src='http://l.wordpress.com/latex.php?latex=c_t%28x%29+%3D+%5Csum_i+c%5Ei%28x%29+t%5Ei&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='c_t(x) = \sum_i c^i(x) t^i' title='c_t(x) = \sum_i c^i(x) t^i' class='latex' /> is a <strong>Chern class homomorphism</strong> if</p>
<ul>
<li> For each line element u, <img src='http://l.wordpress.com/latex.php?latex=c%5Ei%28u%29+%3D+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='c^i(u) = 0' title='c^i(u) = 0' class='latex' /> for i&gt;1.</li>
<li> For two line elements u and v, <img src='http://l.wordpress.com/latex.php?latex=c%5E1%28uv%29+%3D+c%5E1%28u%29+%2B+c%5E1%28v%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='c^1(uv) = c^1(u) + c^1(v)' title='c^1(uv) = c^1(u) + c^1(v)' class='latex' />.</li>
</ul>
<p>We will also assume that each <img src='http://l.wordpress.com/latex.php?latex=c_t%28x%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='c_t(x)' title='c_t(x)' class='latex' /> is a polynomial. Chern class homomorphisms are compatible with the splitting principle in the following way. If we want to split an element X in R, then there exists a <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-ring R&#8217; and a graded ring A&#8217; which extends A, together with a Chern class homomorphism <img src='http://l.wordpress.com/latex.php?latex=c_t+%5Ccolon+R%27+%5Cto+1%2BA%27%5E%2B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='c_t \colon R&#039; \to 1+A&#039;^+' title='c_t \colon R&#039; \to 1+A&#039;^+' class='latex' /> which restricts to the one for R. Hence, Chern classes are completely determined by what they do to line elements.</p>
<p>So we get &#8220;factorizations&#8221; <img src='http://l.wordpress.com/latex.php?latex=c_t%28x%29+%3D+%5Cprod_i+%281%2Ba_i+t%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='c_t(x) = \prod_i (1+a_i t)' title='c_t(x) = \prod_i (1+a_i t)' class='latex' />. This allows us to define the <strong>Chern character</strong> <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7Bch%7D+%5Ccolon+R+%5Cto+%5Cmathbf%7BQ%7D%5Bt%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{ch} \colon R \to \mathbf{Q}[t]' title='\mathrm{ch} \colon R \to \mathbf{Q}[t]' class='latex' /> via <img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+%5Cmathrm%7Bch%7D%28x%29+%3D+%5Csum_i+%5Cexp%28a_i%29+%3D++%5Csum_i+%5Csum_%7Bn+%5Cge+0%7D+%5Cfrac%7Ba_n%7D%7Bn%21%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle \mathrm{ch}(x) = \sum_i \exp(a_i) =  \sum_i \sum_{n \ge 0} \frac{a_n}{n!}' title='\displaystyle \mathrm{ch}(x) = \sum_i \exp(a_i) =  \sum_i \sum_{n \ge 0} \frac{a_n}{n!}' class='latex' /> and the <strong>Todd class</strong> <img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+%5Cmathrm%7Btd%7D%28x%29+%3D+%5Cprod_i+%5Cfrac%7Ba_i%5Cexp%28a_i%29%7D%7B%5Cexp%28a_i%29+-+1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle \mathrm{td}(x) = \prod_i \frac{a_i\exp(a_i)}{\exp(a_i) - 1}' title='\displaystyle \mathrm{td}(x) = \prod_i \frac{a_i\exp(a_i)}{\exp(a_i) - 1}' class='latex' />.</p>
<p>Now we move on to Riemann&#8211;Roch formalism. Let C be a category. A <strong>Riemann&#8211;Roch functor</strong> is a triple <img src='http://l.wordpress.com/latex.php?latex=%28K%2C+%5Crho%2C+A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(K, \rho, A)' title='(K, \rho, A)' class='latex' /> such that</p>
<ul>
<li> For all X in C, we have commutative rings K(X) and A(X). Let UK(X) and UA(X) be the underlying additive groups.</li>
<li> For every morphism <img src='http://l.wordpress.com/latex.php?latex=f+%5Ccolon+X+%5Cto+Y&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f \colon X \to Y' title='f \colon X \to Y' class='latex' />, we have ring homomorphisms (<strong>pullbacks</strong>) <img src='http://l.wordpress.com/latex.php?latex=f%5EK+%5Ccolon+K%28Y%29+%5Cto+K%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f^K \colon K(Y) \to K(X)' title='f^K \colon K(Y) \to K(X)' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=f%5EA+%5Ccolon+A%28Y%29+%5Cto+A%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f^A \colon A(Y) \to A(X)' title='f^A \colon A(Y) \to A(X)' class='latex' /> which make K and A into contravariant functors from C to commutative rings.</li>
<li> For every morphism <img src='http://l.wordpress.com/latex.php?latex=f+%5Ccolon+X+%5Cto+Y&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f \colon X \to Y' title='f \colon X \to Y' class='latex' />, we have group homomorphisms (<strong>pushforwards</strong>) <img src='http://l.wordpress.com/latex.php?latex=f_K+%5Ccolon+UK%28X%29+%5Cto+UK%28Y%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f_K \colon UK(X) \to UK(Y)' title='f_K \colon UK(X) \to UK(Y)' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=f_A+%5Ccolon+UA%28X%29+%5Cto+UA%28Y%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f_A \colon UA(X) \to UA(Y)' title='f_A \colon UA(X) \to UA(Y)' class='latex' /> which make UK and UA into covariant functors from C to Abelian groups.</li>
<li> The <strong>projection formula</strong> <img src='http://l.wordpress.com/latex.php?latex=f_H%28x+%5Ccdot+f%5EH%28y%29%29+%3D+f_H%28x%29+%5Ccdot+y&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f_H(x \cdot f^H(y)) = f_H(x) \cdot y' title='f_H(x \cdot f^H(y)) = f_H(x) \cdot y' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=f+%5Ccolon+X+%5Cto+Y&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f \colon X \to Y' title='f \colon X \to Y' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=x+%5Cin+H%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='x \in H(X)' title='x \in H(X)' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=y+%5Cin+H%28Y%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='y \in H(Y)' title='y \in H(Y)' class='latex' /> holds for H=K and H=A.</li>
<li> <img src='http://l.wordpress.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\rho' title='\rho' class='latex' /> is a natural transformation from K to A.</li>
</ul>
<p>The statement that Riemann&#8211;Roch holds for a morphism f in C means that there exists an element <img src='http://l.wordpress.com/latex.php?latex=%5Ctau_f+%5Cin+A%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\tau_f \in A(X)' title='\tau_f \in A(X)' class='latex' /> such that <img src='http://l.wordpress.com/latex.php?latex=%5Crho_Y+f_K%28x%29+%3D+f_A%28%5Ctau_f+%5Ccdot+%5Crho_X%28x%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\rho_Y f_K(x) = f_A(\tau_f \cdot \rho_X(x))' title='\rho_Y f_K(x) = f_A(\tau_f \cdot \rho_X(x))' class='latex' /> for all x in K(X). The element <img src='http://l.wordpress.com/latex.php?latex=%5Ctau_f&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\tau_f' title='\tau_f' class='latex' /> measures the failure for <img src='http://l.wordpress.com/latex.php?latex=%5Crho+%5Ccolon+UK+%5Cto+UA&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\rho \colon UK \to UA' title='\rho \colon UK \to UA' class='latex' /> to be a natural transformation of covariant functors.</p>
<p>If Riemann&#8211;Roch holds for two morphisms, then it also holds for their composition.</p>
<p>To bring in <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-rings, we focus more specifically on <strong>Chern class functors</strong>. This is a Riemann&#8211;Roch functor <img src='http://l.wordpress.com/latex.php?latex=%28K%2C+c%2C+A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(K, c, A)' title='(K, c, A)' class='latex' /> where we further assume that</p>
<ul>
<li> The image of K is the category of <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-rings with involution.</li>
<li> The image of A is the category of graded rings whose morphisms are degree 0 maps.</li>
<li> For every X in C, <img src='http://l.wordpress.com/latex.php?latex=c+%5Ccolon+K%28X%29+%5Cto+1%2BA%28X%29%5E%2B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='c \colon K(X) \to 1+A(X)^+' title='c \colon K(X) \to 1+A(X)^+' class='latex' /> is a Chern class homomorphism.</li>
</ul>
<p>Fix this Chern class functor. Since this post is already getting too technical, let me just mention that one defines what it means for a morphism in C to be an <strong>elementary embedding</strong> and <strong>elementary projection</strong>, and shows that Riemann&#8211;Roch holds for such morphisms. The elements <img src='http://l.wordpress.com/latex.php?latex=%5Ctau_f&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\tau_f' title='\tau_f' class='latex' /> in both cases are defined in terms of Todd classes.</p>
<p>Now we relate this to the Grothendieck&#8211;Riemann&#8211;Roch theorem. For this, we fix some Noetherian commutative ring R and let C be the category whose objects are schemes over Spec R that are quasi-projective and connected. The morphisms in our category are those which are projective local complete intersection morphisms: these are all morphisms of the form <img src='http://l.wordpress.com/latex.php?latex=X+%5Cxrightarrow%7Bi%7D+%5Cmathbf%7BP%7D%28E%29+%5Cxrightarrow%7Bp%7D+Y&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X \xrightarrow{i} \mathbf{P}(E) \xrightarrow{p} Y' title='X \xrightarrow{i} \mathbf{P}(E) \xrightarrow{p} Y' class='latex' /> where E is a vector bundle on Y, and <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BP%7D%28E%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{P}(E)' title='\mathbf{P}(E)' class='latex' /> is the corresponding projective bundle, and i is a closed embedding whose image is locally a complete intersection (i.e., there is an open affine cover where in each open affine, the ideal of X is generated by a regular sequence). Here K is the K-theory of algebraic vector bundles over X, and A is a certain associated graded ring of K(X). We have pullbacks of vector bundles which makes K and A into contravariant functors. The pushforward <img src='http://l.wordpress.com/latex.php?latex=f_K&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f_K' title='f_K' class='latex' /> on K is given by <img src='http://l.wordpress.com/latex.php?latex=f_K+%3D+%5Csum_%7Bi+%5Cge+0%7D+%28-1%29%5Ei+%5Cmathrm%7BR%7D%5Ei+f_%2A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f_K = \sum_{i \ge 0} (-1)^i \mathrm{R}^i f_*' title='f_K = \sum_{i \ge 0} (-1)^i \mathrm{R}^i f_*' class='latex' /> an alternating sum of higher direct images. In this case, i is an elementary embedding, and p is an elementary projection in the language used above.</p>
<p>What comes out of all of this (and the stuff I skipped on elementary embeddings and elementary projections), is that Riemann&#8211;Roch holds for all morphisms in this category, and the element <img src='http://l.wordpress.com/latex.php?latex=%5Ctau_f&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\tau_f' title='\tau_f' class='latex' /> can be written as the Todd class <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7Btd%7D%28T_f%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{td}(T_f)' title='\mathrm{td}(T_f)' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=T_f&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='T_f' title='T_f' class='latex' /> is the <strong>virtual tangent bundle</strong> of f defined as<br />
<img src='http://l.wordpress.com/latex.php?latex=T_f+%3D+%5Bi%5E%2A%5Cmathscr%7BT%7D_%7B%5Cmathbf%7BP%7D%28E%29+%2F+Y%7D%5D+-+%5B%5Cmathscr%7BN%7D_%7BX%2C%5Cmathbf%7BP%7D%28E%29%7D%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='T_f = [i^*\mathscr{T}_{\mathbf{P}(E) / Y}] - [\mathscr{N}_{X,\mathbf{P}(E)}]' title='T_f = [i^*\mathscr{T}_{\mathbf{P}(E) / Y}] - [\mathscr{N}_{X,\mathbf{P}(E)}]' class='latex' /> using the notation above. here <img src='http://l.wordpress.com/latex.php?latex=%5Cmathscr%7BT%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathscr{T}' title='\mathscr{T}' class='latex' /> denotes the relative tangent bundle, and <img src='http://l.wordpress.com/latex.php?latex=%5Cmathscr%7BN%7D_%7BX%2C%5Cmathbf%7BP%7D%28E%29%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathscr{N}_{X,\mathbf{P}(E)}' title='\mathscr{N}_{X,\mathbf{P}(E)}' class='latex' /> is the normal bundle of X inside of <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BP%7D%28E%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{P}(E)' title='\mathbf{P}(E)' class='latex' /> (this is a bundle because X is a local complete intersection).</p>
<p>We&#8217;ll do one last thing: specialize to the case that R=k is a field and we consider only connected nonsingular quasiprojective varieties over k and proper morphisms between them. Given X, we can embed it inside some projective space <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BP%7D%5En&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{P}^n' title='\mathbf{P}^n' class='latex' /> via a map i. A map is proper <img src='http://l.wordpress.com/latex.php?latex=f+%5Ccolon+X+%5Cto+Y&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f \colon X \to Y' title='f \colon X \to Y' class='latex' /> if and only if the graph morphism <img src='http://l.wordpress.com/latex.php?latex=X+%5Cto+%5Cmathbf%7BP%7D%5En+%5Ctimes+Y&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X \to \mathbf{P}^n \times Y' title='X \to \mathbf{P}^n \times Y' class='latex' /> induced by the maps i and f is a closed embedding. Whenever a nonsingular variety is embedded as a closed subvariety of another nonsingular variety, it is automatically a local complete intersection, so we see that this case is really a special case of the preceding paragraph (here E is a trivial rank n+1 vector bundle over Y). Also, on a nonsingular variety, every coherent sheaf has a finite resolution by vector bundles, so K(X) is in fact the Grothendieck group of coherent sheaves (though the multiplication for coherent sheaves which aren&#8217;t vector bundles involves sums and Tor functors). Furthermore, we can let A be the Chow ring functor (which shows that it coincides with the associated graded of K in this case), and our natural transformation <img src='http://l.wordpress.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\rho' title='\rho' class='latex' /> is the usual Chern character ch. We&#8217;ll finish with what Grothendieck&#8211;Riemann&#8211;Roch says in this case:</p>
<p>Let <img src='http://l.wordpress.com/latex.php?latex=f+%5Ccolon+X+%5Cto+Y&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f \colon X \to Y' title='f \colon X \to Y' class='latex' /> be a proper morphism between nonsingular quasiprojective varieties, and let [F] be an element in K(X). Then</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7Bch%7D%28f_K%28%5BF%5D%29%29+%3D+f_%2A%28%5Cmathrm%7Btd%7D%28%5BT_f%5D%29+%5Ccdot+%5Cmathrm%7Bch%7D%28%5BF%5D%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{ch}(f_K([F])) = f_*(\mathrm{td}([T_f]) \cdot \mathrm{ch}([F]))' title='\mathrm{ch}(f_K([F])) = f_*(\mathrm{td}([T_f]) \cdot \mathrm{ch}([F]))' class='latex' />.</p>
<p>-Steven</p>
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			<media:title type="html">masnevets</media:title>
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		<title>Lambda-rings</title>
		<link>http://concretenonsense.wordpress.com/2009/07/23/lambda-rings/</link>
		<comments>http://concretenonsense.wordpress.com/2009/07/23/lambda-rings/#comments</comments>
		<pubDate>Thu, 23 Jul 2009 22:04:02 +0000</pubDate>
		<dc:creator>Steven Sam</dc:creator>
				<category><![CDATA[Algebra]]></category>
		<category><![CDATA[Algebraic Geometry]]></category>
		<category><![CDATA[Combinatorics]]></category>
		<category><![CDATA[lambda rings]]></category>
		<category><![CDATA[K-theory]]></category>

		<guid isPermaLink="false">http://concretenonsense.wordpress.com/?p=534</guid>
		<description><![CDATA[In this post, I want to discuss Grothendieck&#8217;s -rings and how they provide an abstract setting for Riemann&#8211;Roch formalism. The references I&#8217;ll be using are 

Donald Knutson, Lambda-Rings and the Representation Theory of the Symmetric Group
William Fulton and Serge Lang, Riemann&#8211;Roch Algebra

The definition of a -ring is a bit technical, but it starts with a [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=concretenonsense.wordpress.com&blog=2918042&post=534&subd=concretenonsense&ref=&feed=1" />]]></description>
			<content:encoded><![CDATA[<div class='snap_preview'><br /><p>In this post, I want to discuss Grothendieck&#8217;s <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-rings and how they provide an abstract setting for Riemann&#8211;Roch formalism. The references I&#8217;ll be using are </p>
<ul>
<li>Donald Knutson, <i>Lambda-Rings and the Representation Theory of the Symmetric Group</i></li>
<li>William Fulton and Serge Lang, <i>Riemann&#8211;Roch Algebra</i></li>
</ul>
<p>The definition of a <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-ring is a bit technical, but it starts with a commutative ring R together with operations <img src='http://l.wordpress.com/latex.php?latex=%5Clambda%5Ei+%5Ccolon+R+%5Cto+R&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda^i \colon R \to R' title='\lambda^i \colon R \to R' class='latex' /> for all nonnegative integers i such that <img src='http://l.wordpress.com/latex.php?latex=%5Clambda%5E0%28r%29+%3D+1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda^0(r) = 1' title='\lambda^0(r) = 1' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=%5Clambda%5E1%28r%29+%3D+r&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda^1(r) = r' title='\lambda^1(r) = r' class='latex' /> for all r in R together with some axioms. In particular, we should say what these lambda operations do to sums and products, and we might also want to know what compositions of them look like. To motivate these axioms, we&#8217;ll look at K-theory (where it originates).<br />
<span id="more-534"></span><br />
Let X be a topological space, and consider the set of all vector bundles over X (topological, smooth, holomorphic, whatever you want). We define lambda operations using exterior powers: <img src='http://l.wordpress.com/latex.php?latex=%5Clambda%5Ei%28E%29+%3D+%5Cbigwedge%5Ei+E&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda^i(E) = \bigwedge^i E' title='\lambda^i(E) = \bigwedge^i E' class='latex' />. Of course, the set of vector bundles on X isn&#8217;t a ring, but the free Abelian group of isomorphism classes of vector bundles is a ring if we use tensor product as the multiplication. But we have to define exterior products on &#8220;negatives&#8221; of isomorphism classes of vector bundles. For actual vector bundles, we have the identity</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cbigwedge%5En%28E+%5Coplus+F%29+%3D+%5Cbigoplus_%7Bi%3D0%7D%5En+%5Cbigwedge%5Ei+E+%5Cotimes+%5Cbigwedge%5E%7Bn-i%7D+F&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\bigwedge^n(E \oplus F) = \bigoplus_{i=0}^n \bigwedge^i E \otimes \bigwedge^{n-i} F' title='\bigwedge^n(E \oplus F) = \bigoplus_{i=0}^n \bigwedge^i E \otimes \bigwedge^{n-i} F' class='latex' />,</p>
<p>so we can use this to extend to &#8220;negatives&#8221; and we make this an axiom for a general <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-ring:</p>
<p>(L1) <img src='http://l.wordpress.com/latex.php?latex=%5Clambda%5Ei%28r%2Bs%29+%3D+%5Csum_%7Bj%3D0%7D%5Ei+%5Clambda%5Ej%28r%29+%5Clambda%5E%7Bi-j%7D%28s%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda^i(r+s) = \sum_{j=0}^i \lambda^j(r) \lambda^{i-j}(s)' title='\lambda^i(r+s) = \sum_{j=0}^i \lambda^j(r) \lambda^{i-j}(s)' class='latex' /> for all r and s in R.</p>
<p>In fact, the above identity holds if we pass to the Grothendieck group <img src='http://l.wordpress.com/latex.php?latex=K_0%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K_0(X)' title='K_0(X)' class='latex' /> of vector bundles over X (add the relations <img src='http://l.wordpress.com/latex.php?latex=E%27%2BE%27%27+%3D+E&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='E&#039;+E&#039;&#039; = E' title='E&#039;+E&#039;&#039; = E' class='latex' /> whenever we have a short exact sequence of the form <img src='http://l.wordpress.com/latex.php?latex=0+%5Cto+E%27+%5Cto+E+%5Cto+E%27%27+%5Cto+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='0 \to E&#039; \to E \to E&#039;&#039; \to 0' title='0 \to E&#039; \to E \to E&#039;&#039; \to 0' class='latex' />) because in general, if E&#8217; is an extension of E and F, then <img src='http://l.wordpress.com/latex.php?latex=%5Cbigwedge%5En+E%27&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\bigwedge^n E&#039;' title='\bigwedge^n E&#039;' class='latex' /> has a filtration whose associated graded is the direct sum on the RHS above.</p>
<p>What about products? i.e., what should <img src='http://l.wordpress.com/latex.php?latex=%5Clambda%28rs%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda(rs)' title='\lambda(rs)' class='latex' /> be? The exterior power of a tensor product of two vector bundles has a rather complicated expression. Nonetheless, there exist integer valued polynomials <img src='http://l.wordpress.com/latex.php?latex=P_n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='P_n' title='P_n' class='latex' /> in 2n variables such that</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cbigwedge%5En%28E+%5Cotimes+F%29+%3D+P_n%28E%2C+%5Cbigwedge%5E2+E%2C+%5Cdots%2C+%5Cbigwedge%5En+E%2C+F%2C+%5Cbigwedge%5E2+F%2C+%5Cdots%2C+%5Cbigwedge%5En+F%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\bigwedge^n(E \otimes F) = P_n(E, \bigwedge^2 E, \dots, \bigwedge^n E, F, \bigwedge^2 F, \dots, \bigwedge^n F)' title='\bigwedge^n(E \otimes F) = P_n(E, \bigwedge^2 E, \dots, \bigwedge^n E, F, \bigwedge^2 F, \dots, \bigwedge^n F)' class='latex' />.</p>
<p>How do we get these polynomials? Let <img src='http://l.wordpress.com/latex.php?latex=X_1%2C+%5Cdots%2C+X_i%2C+%5Cdots%2C+Y_1+%5Cdots%2C+Y_i%2C+%5Cdots&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X_1, \dots, X_i, \dots, Y_1 \dots, Y_i, \dots' title='X_1, \dots, X_i, \dots, Y_1 \dots, Y_i, \dots' class='latex' /> be algebraically independent variables, and let <img src='http://l.wordpress.com/latex.php?latex=E_i%2C+F_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='E_i, F_i' title='E_i, F_i' class='latex' /> denote the ith elementary symmetric function in the Xs and Ys, respectively. Then we define the polynomials <img src='http://l.wordpress.com/latex.php?latex=P_n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='P_n' title='P_n' class='latex' /> via the identity</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+%5Csum_%7Bn+%5Cge+0%7D+P_n%28E_1%2C+%5Cdots%2C+E_n%2C+F_1%2C+%5Cdots%2C+F_n%29+T%5En+%3D+%5Cprod_%7Bi%2Cj+%5Cge+1%7D+%281%2BX_iY_jT%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle \sum_{n \ge 0} P_n(E_1, \dots, E_n, F_1, \dots, F_n) T^n = \prod_{i,j \ge 1} (1+X_iY_jT)' title='\displaystyle \sum_{n \ge 0} P_n(E_1, \dots, E_n, F_1, \dots, F_n) T^n = \prod_{i,j \ge 1} (1+X_iY_jT)' class='latex' />.</p>
<p>So we have some complicated family of polynomials, and the axiom</p>
<p>(L2) <img src='http://l.wordpress.com/latex.php?latex=%5Clambda%5En%28rs%29+%3D+P_n%28%5Clambda%5E1%28r%29%2C+%5Cdots%2C+%5Clambda%5En%28r%29%2C+%5Clambda%5E1%28s%29%2C+%5Cdots%2C+%5Clambda%5En%28s%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda^n(rs) = P_n(\lambda^1(r), \dots, \lambda^n(r), \lambda^1(s), \dots, \lambda^n(s))' title='\lambda^n(rs) = P_n(\lambda^1(r), \dots, \lambda^n(r), \lambda^1(s), \dots, \lambda^n(s))' class='latex' /> for all r and s in R.</p>
<p>There are also some integer-valued polynomials <img src='http://l.wordpress.com/latex.php?latex=P_%7Bnm%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='P_{nm}' title='P_{nm}' class='latex' /> of degree nm for expressing the compositions <img src='http://l.wordpress.com/latex.php?latex=%5Cbigwedge%5En+%5Cbigwedge%5Em+E&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\bigwedge^n \bigwedge^m E' title='\bigwedge^n \bigwedge^m E' class='latex' />. I won&#8217;t get into that, but this gives the third axiom</p>
<p>(L3) <img src='http://l.wordpress.com/latex.php?latex=%5Clambda%5En%28%5Clambda%5Em%28r%29%29+%3D+P_%7Bnm%7D%28%5Clambda%5E1%28r%29%2C+%5Cdots%2C+%5Clambda%5E%7Bnm%7D%28r%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda^n(\lambda^m(r)) = P_{nm}(\lambda^1(r), \dots, \lambda^{nm}(r))' title='\lambda^n(\lambda^m(r)) = P_{nm}(\lambda^1(r), \dots, \lambda^{nm}(r))' class='latex' /> for all r in R.</p>
<p>A <b>morphism</b> of <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-rings is a ring homomorphism which commutes with the lambda-operations.</p>
<p>For a simple combinatorial example, take X to be a point. In this case, vector bundles are just vector spaces, and <img src='http://l.wordpress.com/latex.php?latex=K_0%28X%29+%3D+%5Cmathbf%7BZ%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K_0(X) = \mathbf{Z}' title='K_0(X) = \mathbf{Z}' class='latex' />. Identifying vector spaces with their dimension, the lambda operations become <img src='http://l.wordpress.com/latex.php?latex=%5Clambda%5Ek%28n%29+%3D+%5Cfrac%7Bn%28n-1%29%5Ccdots+%28n-k%2B1%29%7D%7Bk%21%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda^k(n) = \frac{n(n-1)\cdots (n-k+1)}{k!}' title='\lambda^k(n) = \frac{n(n-1)\cdots (n-k+1)}{k!}' class='latex' />, which is just the binomial coefficient <img src='http://l.wordpress.com/latex.php?latex=%5Cbinom%7Bn%7D%7Bk%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\binom{n}{k}' title='\binom{n}{k}' class='latex' /> when n is nonnegative. A morphism <img src='http://l.wordpress.com/latex.php?latex=%5Cvarepsilon+%5Ccolon+R+%5Cto+%5Cmathbf%7BZ%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\varepsilon \colon R \to \mathbf{Z}' title='\varepsilon \colon R \to \mathbf{Z}' class='latex' /> is called an <b>augmentation</b>. For vector bundles, this map is given by sending a vector bundle to its rank and extending linearly to virtual vector bundles. We&#8217;ll assume our <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-rings are augmented.</p>
<p>We can place some further requirements and operations on our <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-rings. First, in <img src='http://l.wordpress.com/latex.php?latex=K_0%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K_0(X)' title='K_0(X)' class='latex' />, we naturally have a notion of what it means to be &#8220;positive&#8221;: any class which represents an actual vector bundle. The set of positive elements has the property that it&#8217;s closed under addition and multiplication, and every element of <img src='http://l.wordpress.com/latex.php?latex=K_0%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K_0(X)' title='K_0(X)' class='latex' /> can be expressed as a difference of two positive elements. Furthermore, whenever x is positive, <img src='http://l.wordpress.com/latex.php?latex=%5Clambda%5Ei%28x%29+%3D+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda^i(x) = 0' title='\lambda^i(x) = 0' class='latex' /> for sufficiently large i, and all positive elements of augmentation 1 (line bundles) have multiplicative inverses. We&#8217;ll take all of these features to be an axiom system for a &#8220;positive subset&#8221; of a <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-ring. Motivated by the K-theory, we&#8217;ll call positive elements of augmentation 1 <b>line elements</b>. We&#8217;ll assume that our <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-rings are equipped with a positive structure.</p>
<p>K-theory also has a nice involution: send a vector bundle to its dual bundle. In general, we&#8217;ll say that <img src='http://l.wordpress.com/latex.php?latex=x+%5Cmapsto+x%5E%5Cvee&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='x \mapsto x^\vee' title='x \mapsto x^\vee' class='latex' /> is an <b>involution</b> of our <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-ring if it satisfies </p>
<ul>
<li> <img src='http://l.wordpress.com/latex.php?latex=%28x%5E%5Cvee%29%5E%5Cvee+%3D+x&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(x^\vee)^\vee = x' title='(x^\vee)^\vee = x' class='latex' /> for all x,</li>
<li> <img src='http://l.wordpress.com/latex.php?latex=%5Cvarepsilon%28x%5E%5Cvee%29+%3D+%5Cvarepsilon%28x%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\varepsilon(x^\vee) = \varepsilon(x)' title='\varepsilon(x^\vee) = \varepsilon(x)' class='latex' /> for all x,</li>
<li> <img src='http://l.wordpress.com/latex.php?latex=u%5E%5Cvee+%3D+u%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='u^\vee = u^{-1}' title='u^\vee = u^{-1}' class='latex' /> for all line elements u.</li>
</ul>
<p>We&#8217;ll further assume that our <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-rings are equipped with an involution.</p>
<p>Another example of <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-rings comes from representation rings. Given a group G and a representation V, we define <img src='http://l.wordpress.com/latex.php?latex=%5Clambda%5Ei%28V%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda^i(V)' title='\lambda^i(V)' class='latex' /> to be the representation <img src='http://l.wordpress.com/latex.php?latex=%5Cbigwedge%5Ei+V&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\bigwedge^i V' title='\bigwedge^i V' class='latex' /> with the diagonal action of G. The augmentation here sends a representation to its dimension (over the ground field), the positive elements are the representations, and the involution sends a representation to its dual. One particular example is when G is the general linear group <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BGL%7D_n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{GL}_n' title='\mathbf{GL}_n' class='latex' /> and we consider only rational representations, so that the representation ring is the ring of symmetric functions in n variables (together with a multiplicative inverse for the product of the n variables). In this case, the lambda operations are plethysm: <img src='http://l.wordpress.com/latex.php?latex=%5Clambda%5En%28p%29+%3D+e_n+%5Ccirc+p&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda^n(p) = e_n \circ p' title='\lambda^n(p) = e_n \circ p' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=e_n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='e_n' title='e_n' class='latex' /> is the nth elementary symmetric function, and positive means Schur positive. [I first saw <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-rings in context of symmetric functions, so the definitions seemed a bit mysterious to me.]</p>
<p>In the next post, I&#8217;ll discuss abstract Chern classes in the context of <img src='http://l.wordpress.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lambda' title='\lambda' class='latex' />-rings and Riemann&#8211;Roch formalism, and say how this relates to Grothendieck&#8211;Riemann&#8211;Roch for proper maps between nonsingular varieties.</p>
<p>-Steven</p>
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			<media:title type="html">masnevets</media:title>
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		<title>q-analogues and homogeneous spaces</title>
		<link>http://concretenonsense.wordpress.com/2009/04/28/q-analogues-and-homogeneous-spaces/</link>
		<comments>http://concretenonsense.wordpress.com/2009/04/28/q-analogues-and-homogeneous-spaces/#comments</comments>
		<pubDate>Tue, 28 Apr 2009 22:13:10 +0000</pubDate>
		<dc:creator>Steven Sam</dc:creator>
				<category><![CDATA[Algebraic Geometry]]></category>
		<category><![CDATA[Combinatorics]]></category>
		<category><![CDATA[cohomology]]></category>
		<category><![CDATA[q-analogues]]></category>

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		<description><![CDATA[While I was working on my final paper for the course on quivers that I&#8217;m taking this semester, I came across the following result (the notation  means the finite field with  elements, and  is the field of complex numbers):
Theorem. Let X be a variety defined over Z and assume for some prime [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=concretenonsense.wordpress.com&blog=2918042&post=452&subd=concretenonsense&ref=&feed=1" />]]></description>
			<content:encoded><![CDATA[<div class='snap_preview'><br /><p>While I was working on my final paper for the course on quivers that I&#8217;m taking this semester, I came across the following result (the notation <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BF%7D_%7Bp%5Er%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{F}_{p^r}' title='\mathbf{F}_{p^r}' class='latex' /> means the finite field with <img src='http://l.wordpress.com/latex.php?latex=p%5Er&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='p^r' title='p^r' class='latex' /> elements, and <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BC%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{C}' title='\mathbf{C}' class='latex' /> is the field of complex numbers):</p>
<p><strong>Theorem.</strong> Let X be a variety defined over<strong> Z</strong> and assume for some prime p, and all r&gt;0, that the function <img src='http://l.wordpress.com/latex.php?latex=%5C%23X%28%7B%5Cbf+F%7D_%7Bp%5Er%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\#X({\bf F}_{p^r})' title='\#X({\bf F}_{p^r})' class='latex' /> is obtained by plugging in <img src='http://l.wordpress.com/latex.php?latex=p%5Er&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='p^r' title='p^r' class='latex' /> into some polynomial P(t). Then P(t) has integral coefficients, and P(1) is the Euler characteristic of <img src='http://l.wordpress.com/latex.php?latex=X%28%7B%5Cbf+C%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X({\bf C})' title='X({\bf C})' class='latex' />.</p>
<p>If you&#8217;re not comfortable with varieties, just think of the solution set of some collection of polynomials in multiple variables, and if you don&#8217;t know what the rest of the words mean, that won&#8217;t matter much for the stuff starting with the next paragraph. Here I&#8217;m using the notation X(F) to denote the solutions for X over F, and I&#8217;m thinking of <img src='http://l.wordpress.com/latex.php?latex=X%28%7B%5Cbf+C%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X({\bf C})' title='X({\bf C})' class='latex' /> as a complex analytic space. The proof uses <img src='http://l.wordpress.com/latex.php?latex=%5Cell&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\ell' title='\ell' class='latex' />-adic cohomology (with compact support) and the Grothendieck–Lefschetz trace formula. I won&#8217;t get into that, but I&#8217;d like to use this as an excuse to talk about the q-analogues of the natural numbers.<span id="more-452"></span></p>
<p>Let&#8217;s fix a field with q elements, and work over this field. First let&#8217;s use the theorem on projective space <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BP%7D%5E%7Bn-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{P}^{n-1}' title='\mathbf{P}^{n-1}' class='latex' />, whose points are the one-dimensional subspaces (lines) in an n-dimensional vector space V. The number of lines of an n-dimensional vector space is <img src='http://l.wordpress.com/latex.php?latex=%28q%5En-1%29%2F%28q-1%29+%3D+q%5E%7Bn-1%7D+%2B+q%5E%7Bn-2%7D+%2B+%5Ccdots+%2B+q+%2B+1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(q^n-1)/(q-1) = q^{n-1} + q^{n-2} + \cdots + q + 1' title='(q^n-1)/(q-1) = q^{n-1} + q^{n-2} + \cdots + q + 1' class='latex' /> because any nonzero vector defines a line, and each line is spanned by q-1 different vectors. Let&#8217;s denote this number [n] because substituting q=1 gives n, which is the Euler characteristic of n-1 dimensional complex projective space. Now let&#8217;s move onto complete flag varieties Flag(V) for V n-dimensional: the elements are just increasing chains <img src='http://l.wordpress.com/latex.php?latex=V_1+%5Csubset+V_2+%5Csubset+%5Ccdots+%5Csubset+V_n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V_1 \subset V_2 \subset \cdots \subset V_n' title='V_1 \subset V_2 \subset \cdots \subset V_n' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=%5Cdim+V_i+%3D+i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\dim V_i = i' title='\dim V_i = i' class='latex' />. The number of flags is <img src='http://l.wordpress.com/latex.php?latex=%5B+n+%5D+%5B+n+-+1+%5D+%5Ccdots+%5B+2+%5D+%5B1%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[ n ] [ n - 1 ] \cdots [ 2 ] [1]' title='[ n ] [ n - 1 ] \cdots [ 2 ] [1]' class='latex' /> because to define a flag, we first pick <img src='http://l.wordpress.com/latex.php?latex=v_1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v_1' title='v_1' class='latex' /> nonzero to get <img src='http://l.wordpress.com/latex.php?latex=V_1+%3D+%5Clangle+v_1+%5Crangle&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V_1 = \langle v_1 \rangle' title='V_1 = \langle v_1 \rangle' class='latex' />, and in general, after we pick <img src='http://l.wordpress.com/latex.php?latex=v_1%2C+%5Cdots%2C+v_%7Bi-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v_1, \dots, v_{i-1}' title='v_1, \dots, v_{i-1}' class='latex' />, we can pick any lift <img src='http://l.wordpress.com/latex.php?latex=v_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v_i' title='v_i' class='latex' /> of a nonzero vector <img src='http://l.wordpress.com/latex.php?latex=%5Coverline%7Bv%7D_i+%5Cin+V+%2F+%5Clangle+v_1%2C+%5Cdots%2C+v_%7Bi-1%7D+%5Crangle&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\overline{v}_i \in V / \langle v_1, \dots, v_{i-1} \rangle' title='\overline{v}_i \in V / \langle v_1, \dots, v_{i-1} \rangle' class='latex' />, and the space <img src='http://l.wordpress.com/latex.php?latex=V_i+%3D+%5Clangle+v_1%2C+%5Cdots%2C+v_i+%5Crangle&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V_i = \langle v_1, \dots, v_i \rangle' title='V_i = \langle v_1, \dots, v_i \rangle' class='latex' /> is independent of the choice of lift. So let&#8217;s call this number <img src='http://l.wordpress.com/latex.php?latex=%5B+n+%5D+%21&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[ n ] !' title='[ n ] !' class='latex' /> because specializing q=1 gives n!, which we now know is the Euler characteristic of the complex complete flag variety.</p>
<p>Let&#8217;s take a look at the Grassmannian Gr(k,V), whose points are the k-dimensional subspaces of an n-dimensional vector space V. To count its number of points, notice that we have a map Flag(n) to Gr(k,n) which just sends a flag <img src='http://l.wordpress.com/latex.php?latex=V_1+%5Csubset+%5Ccdots+%5Csubset+V_n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V_1 \subset \cdots \subset V_n' title='V_1 \subset \cdots \subset V_n' class='latex' /> to the subspace <img src='http://l.wordpress.com/latex.php?latex=V_k&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V_k' title='V_k' class='latex' />. This map is obviously surjective, but what are the fibers? It follows from the definitions that the preimage of a k-dimensional subspace W is Flag(W) x Flag(V/W), so the number of points is just <img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+%5Cfrac%7B%5B+n+%5D+%21+%7D%7B+%5B+k+%5D+%21+%5B+n+-+k+%5D+%21%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle \frac{[ n ] ! }{ [ k ] ! [ n - k ] !}' title='\displaystyle \frac{[ n ] ! }{ [ k ] ! [ n - k ] !}' class='latex' />. And we&#8217;ll call this number <img src='http://l.wordpress.com/latex.php?latex=%5Cleft%5B+%5Cbegin%7Bmatrix%7D+n+%5C%5C+k+%5Cend%7Bmatrix%7D+%5Cright%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\left[ \begin{matrix} n \\ k \end{matrix} \right]' title='\left[ \begin{matrix} n \\ k \end{matrix} \right]' class='latex' /> because it specializes to <img src='http://l.wordpress.com/latex.php?latex=%5Cbinom%7Bn%7D%7Bk%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\binom{n}{k}' title='\binom{n}{k}' class='latex' /> upon setting q=1, and as before, this is the Euler characteristic of the complex Grassmannian Gr(k,V) where now V is a complex n-dimensional vector space.</p>
<p>Now we can even do partial flag varieties for tuples <img src='http://l.wordpress.com/latex.php?latex=%28d_1%2C+%5Cdots%2C+d_r%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(d_1, \dots, d_r)' title='(d_1, \dots, d_r)' class='latex' />, whose points consists of partial flags <img src='http://l.wordpress.com/latex.php?latex=V_1+%5Csubset+%5Ccdots+%5Csubset+V_r&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V_1 \subset \cdots \subset V_r' title='V_1 \subset \cdots \subset V_r' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=%5Cdim+V_i+%3D+d_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\dim V_i = d_i' title='\dim V_i = d_i' class='latex' />. The number of points is going to be <img src='http://l.wordpress.com/latex.php?latex=%5Cleft%5B+%5Cbegin%7Bmatrix%7D+n+%5C%5C+d_1+%5Cend%7Bmatrix%7D+%5Cright%5D+%5Cleft%5B+%5Cbegin%7Bmatrix%7D+n-d_1+%5C%5C+d_2+-+d_1+%5Cend%7Bmatrix%7D+%5Cright%5D+%5Ccdots+%5Cleft%5B+%5Cbegin%7Bmatrix%7D+n-d_1+-+%5Ccdots+-+d_%7Br-1%7D+%5C%5C+d_r+-+d_%7Br-1%7D+-+%5Ccdots+-+d_1+%5Cend%7Bmatrix%7D+%5Cright%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\left[ \begin{matrix} n \\ d_1 \end{matrix} \right] \left[ \begin{matrix} n-d_1 \\ d_2 - d_1 \end{matrix} \right] \cdots \left[ \begin{matrix} n-d_1 - \cdots - d_{r-1} \\ d_r - d_{r-1} - \cdots - d_1 \end{matrix} \right]' title='\left[ \begin{matrix} n \\ d_1 \end{matrix} \right] \left[ \begin{matrix} n-d_1 \\ d_2 - d_1 \end{matrix} \right] \cdots \left[ \begin{matrix} n-d_1 - \cdots - d_{r-1} \\ d_r - d_{r-1} - \cdots - d_1 \end{matrix} \right]' class='latex' />, and setting q=1 gives the analogous product of binomial coefficients for the Euler characteristic.</p>
<p>In all of the cases, it turned out that each of the polynomials in q had positive coefficients. So we might ask what these numbers are counting, if anything. It turns out that setting <img src='http://l.wordpress.com/latex.php?latex=q%3Dt%5E2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='q=t^2' title='q=t^2' class='latex' /> gives the generating function <img src='http://l.wordpress.com/latex.php?latex=%5Csum_%7Bi+%5Cge+0%7D+%5Cdim_%7B%5Cmathbf%7BC%7D%7D+%5Cmathrm%7BH%7D%5Ei%28X%3B+%5Cmathbf%7BZ%7D%29+t%5Ei&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\sum_{i \ge 0} \dim_{\mathbf{C}} \mathrm{H}^i(X; \mathbf{Z}) t^i' title='\sum_{i \ge 0} \dim_{\mathbf{C}} \mathrm{H}^i(X; \mathbf{Z}) t^i' class='latex' /> where X is whichever variety we are talking about, and H refers to plain old singular cohomology. I can give a better answer though: in each of the cases of interest, there is an explicit cellular decomposition of variety in question, and the number of i-dimensional cells is exactly the coefficient of <img src='http://l.wordpress.com/latex.php?latex=q%5Ei&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='q^i' title='q^i' class='latex' /> in the corresponding polynomial. We could discuss this at length, but for now, I&#8217;ll just refer the interested reader to William Fulton&#8217;s book <em>Young Tableaux</em>.</p>
<p>And for those who don&#8217;t know what a homogeneous space is: a homogeneous space is a manifold (resp. algebraic variety) with a transitive smooth (resp. algebraic) action of a Lie (resp. algebraic) group. And one can verify that all of the examples I&#8217;ve discussed are homogeneous spaces for the group <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BGL%7D%28n%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{GL}(n)' title='\mathbf{GL}(n)' class='latex' /> of <img src='http://l.wordpress.com/latex.php?latex=n+%5Ctimes+n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n \times n' title='n \times n' class='latex' /> invertible matrices. For fun, the reader can work out the counts for the symplectic and orthogonal groups and/or figure out what the right analogues of Grassmannians and flag varieties are.</p>
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		<title>The Borel–Weil–Bott theorem</title>
		<link>http://concretenonsense.wordpress.com/2009/04/15/the-borel%e2%80%93weil%e2%80%93bott-theorem/</link>
		<comments>http://concretenonsense.wordpress.com/2009/04/15/the-borel%e2%80%93weil%e2%80%93bott-theorem/#comments</comments>
		<pubDate>Wed, 15 Apr 2009 01:21:43 +0000</pubDate>
		<dc:creator>Steven Sam</dc:creator>
				<category><![CDATA[Algebraic Geometry]]></category>
		<category><![CDATA[Representation Theory]]></category>
		<category><![CDATA[sheaf cohomology]]></category>
		<category><![CDATA[vector bundles]]></category>

		<guid isPermaLink="false">http://concretenonsense.wordpress.com/?p=395</guid>
		<description><![CDATA[In connection with my last post on the Boij–Söderberg conjectures, I mentioned constructing equivariant supernatural vector bundles and equivariant pure Cohen–Macaulay modules using the Borel–Weil–Bott theorem. So in this post, I&#8217;d like to say something about what this theorem says and next time discuss how it can be used. I learned the stuff on Bott&#8217;s [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=concretenonsense.wordpress.com&blog=2918042&post=395&subd=concretenonsense&ref=&feed=1" />]]></description>
			<content:encoded><![CDATA[<div class='snap_preview'><br /><p>In connection with my last post on the Boij–Söderberg conjectures, I mentioned constructing equivariant supernatural vector bundles and equivariant pure Cohen–Macaulay modules using the Borel–Weil–Bott theorem. So in this post, I&#8217;d like to say something about what this theorem says and next time discuss how it can be used. I learned the stuff on Bott&#8217;s theorem from Jerzy Weyman&#8217;s book <em>Cohomology of Vector Bundles and Syzygies</em> [warning: there are some mistakes in the statement of Bott's theorem for general reductive groups]. Bott&#8217;s theorem is usually stated for a reductive group, but for concreteness we&#8217;ll stick with the general linear group, since that&#8217;s all we&#8217;ll need.</p>
<p>The setup is as follows: k denotes some field of characteristic 0, <img src='http://l.wordpress.com/latex.php?latex=G+%3D+%5Cmathbf%7BGL%7D%28n%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G = \mathbf{GL}(n)' title='G = \mathbf{GL}(n)' class='latex' />, B is the subgroup of upper triangular matrices, and T is the subgroup of diagonal matrices. Then G/B is the <a href="http://en.wikipedia.org/wiki/Flag_variety">complete flag variety</a> whose k-points correspond to maximal flags <img src='http://l.wordpress.com/latex.php?latex=V_%5Cbullet+%3D+%280+%5Csubset+V_1+%5Csubset+%5Ccdots+%5Csubset+V_n+%3D+k%5En%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V_\bullet = (0 \subset V_1 \subset \cdots \subset V_n = k^n)' title='V_\bullet = (0 \subset V_1 \subset \cdots \subset V_n = k^n)' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=%5Cdim+V_i+%3D+i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\dim V_i = i' title='\dim V_i = i' class='latex' />. We are interested in realizing representations of G as cohomology groups of line bundles over G/B. But first we&#8217;ll state the relative version of the theorem.<br />
<span id="more-395"></span><br />
For this, let X be any variety (really, X could be any scheme) and <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BE%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{E}' title='\mathcal{E}' class='latex' /> be a vector bundle of rank n over X. We can construct the relative flag variety as follows. For any affine open set U inside of X where we get a trivialization <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BE%7D%7C_U+%3D+U+%5Ctimes+k%5En&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{E}|_U = U \times k^n' title='\mathcal{E}|_U = U \times k^n' class='latex' />, let <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BFl%7D%28%5Cmathcal%7BE%7D%2CU%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{Fl}(\mathcal{E},U)' title='\mathrm{Fl}(\mathcal{E},U)' class='latex' /> be the complete flag variety of <img src='http://l.wordpress.com/latex.php?latex=k%5En&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='k^n' title='k^n' class='latex' />. Using the gluing data of <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BE%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{E}' title='\mathcal{E}' class='latex' />, we can also glue together the spaces <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BFl%7D%28%5Cmathcal%7BE%7D%2C+U%29+%5Ctimes+U&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{Fl}(\mathcal{E}, U) \times U' title='\mathrm{Fl}(\mathcal{E}, U) \times U' class='latex' /> (on intersections, we have an isomorphism <img src='http://l.wordpress.com/latex.php?latex=k%5En+%5Cto+k%5En&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='k^n \to k^n' title='k^n \to k^n' class='latex' />, and this defines an isomorphism of complete flag varieties) to get a scheme <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BFl%7D%28%5Cmathcal%7BE%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{Fl}(\mathcal{E})' title='\mathrm{Fl}(\mathcal{E})' class='latex' /> which maps to X, call the map h. In fact, h is a locally trivial fibration whose fibers are complete flag varieties. To define the analogues of <img src='http://l.wordpress.com/latex.php?latex=R_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='R_i' title='R_i' class='latex' />, consider the vector bundle <img src='http://l.wordpress.com/latex.php?latex=h%5E%2A%28%5Cmathcal%7BE%7D%29+%3D+%5C%7B%28x%2C+F_%5Cbullet%2C+y%29+%5Cmid+x+%5Cin+X%2C%5C+F_%5Cbullet+%5Cin+%5Cmathrm%7BFl%7D%28%5Cmathcal%7BE%7D%29%7C_x%2C%5C+y+%5Cin+%5Cmathcal%7BE%7D%7C_x%5C%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='h^*(\mathcal{E}) = \{(x, F_\bullet, y) \mid x \in X,\ F_\bullet \in \mathrm{Fl}(\mathcal{E})|_x,\ y \in \mathcal{E}|_x\}' title='h^*(\mathcal{E}) = \{(x, F_\bullet, y) \mid x \in X,\ F_\bullet \in \mathrm{Fl}(\mathcal{E})|_x,\ y \in \mathcal{E}|_x\}' class='latex' /> on <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BFl%7D%28%5Cmathcal%7BE%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{Fl}(\mathcal{E})' title='\mathrm{Fl}(\mathcal{E})' class='latex' />. We define <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BR%7D_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{R}_i' title='\mathcal{R}_i' class='latex' /> to be the subbundle of <img src='http://l.wordpress.com/latex.php?latex=h%5E%2A%28E%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='h^*(E)' title='h^*(E)' class='latex' /> consisting of points where <img src='http://l.wordpress.com/latex.php?latex=y+%5Cin+F_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='y \in F_i' title='y \in F_i' class='latex' />. Note that if we took X to be a single point (in particular Spec(k)), then <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BE%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{E}' title='\mathcal{E}' class='latex' /> is just a k-vector space, and <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BFl%7D%28%5Cmathcal%7BE%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{Fl}(\mathcal{E})' title='\mathrm{Fl}(\mathcal{E})' class='latex' /> is the usual flag variety. So we can also define, in analogy, <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BL%7D%28%5Calpha%29+%3D+%5Cmathcal%7BR%7D_1%5E%7B-%5Calpha_1%7D+%5Cotimes+%28%5Cmathcal%7BR%7D_2+%2F+%5Cmathcal%7BR%7D_1%29%5E%7B-%5Calpha_2%7D+%5Cotimes+%5Ccdots+%5Cotimes+%28%5Cmathcal%7BE%7D+%2F+%5Cmathcal%7BR%7D_n%29%5E%7B-%5Calpha_n%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{L}(\alpha) = \mathcal{R}_1^{-\alpha_1} \otimes (\mathcal{R}_2 / \mathcal{R}_1)^{-\alpha_2} \otimes \cdots \otimes (\mathcal{E} / \mathcal{R}_n)^{-\alpha_n}' title='\mathcal{L}(\alpha) = \mathcal{R}_1^{-\alpha_1} \otimes (\mathcal{R}_2 / \mathcal{R}_1)^{-\alpha_2} \otimes \cdots \otimes (\mathcal{E} / \mathcal{R}_n)^{-\alpha_n}' class='latex' />.</p>
<p>Now let W be the Weyl group of G, i.e., the normalizer of T in G quotiented by T, in our case W is the symmetric group on n letters. In fact, W is a finite <a href="http://en.wikipedia.org/wiki/Coxeter_group">Coxeter group</a>, and hence is equipped with a <a href="http://en.wikipedia.org/wiki/Length_function">length function</a>, denoted <img src='http://l.wordpress.com/latex.php?latex=%5Cell&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\ell' title='\ell' class='latex' />. For a permutation w, <img src='http://l.wordpress.com/latex.php?latex=%5Cell%28w%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\ell(w)' title='\ell(w)' class='latex' /> is just the minimal number of simple transpositions <img src='http://l.wordpress.com/latex.php?latex=i+%5Cleftrightarrow+i%2B1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='i \leftrightarrow i+1' title='i \leftrightarrow i+1' class='latex' /> you need when expressing w as a product of them. So W has a natural action on the set of weights of T, and we define a dotted action of W on the weight lattice as follows. First, let <img src='http://l.wordpress.com/latex.php?latex=2%5Crho&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='2\rho' title='2\rho' class='latex' /> be the sum of the positive roots (i.e., the weights that appear when T acts on B via conjugation). In our case, we have <img src='http://l.wordpress.com/latex.php?latex=%5Crho+%3D+%28n-1%2C+n-2%2C+%5Cdots%2C+1%2C+0%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\rho = (n-1, n-2, \dots, 1, 0)' title='\rho = (n-1, n-2, \dots, 1, 0)' class='latex' />. Then for <img src='http://l.wordpress.com/latex.php?latex=w+%5Cin+W&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w \in W' title='w \in W' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha' title='\alpha' class='latex' /> a weight, we set <img src='http://l.wordpress.com/latex.php?latex=w%5E%5Cbullet%28%5Calpha%29+%3D+w%28%5Calpha+%2B+%5Crho%29+-+%5Crho&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w^\bullet(\alpha) = w(\alpha + \rho) - \rho' title='w^\bullet(\alpha) = w(\alpha + \rho) - \rho' class='latex' />. Let <img src='http://l.wordpress.com/latex.php?latex=K_%5Cbeta&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K_\beta' title='K_\beta' class='latex' /> denote the Weyl functor, or co-Schur functor associated to the weight <img src='http://l.wordpress.com/latex.php?latex=%5Cbeta&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\beta' title='\beta' class='latex' />. I&#8217;ll describe its construction in a later post. For now, it&#8217;s a functorial way of constructing, from E, an irreducible representation of <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BGL%7D%28E%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{GL}(E)' title='\mathbf{GL}(E)' class='latex' /> of highest weight <img src='http://l.wordpress.com/latex.php?latex=%5Cbeta&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\beta' title='\beta' class='latex' />. We have the following theorem:</p>
<p><strong>Theorem.</strong> With the notation above, one of two mutually exclusive cases occurs:</p>
<ol>
<li>There exists a nonidentity element <img src='http://l.wordpress.com/latex.php?latex=w+%5Cin+S_n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w \in S_n' title='w \in S_n' class='latex' /> such that <img src='http://l.wordpress.com/latex.php?latex=w%5E%5Cbullet%28%5Calpha%29+%3D+%5Calpha&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w^\bullet(\alpha) = \alpha' title='w^\bullet(\alpha) = \alpha' class='latex' />. In this case, all <a href="http://en.wikipedia.org/wiki/Higher_direct_image">higher direct images</a> <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BR%7D%5Eih_%2A%28%5Cmathcal%7BL%7D%28%5Calpha%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{R}^ih_*(\mathcal{L}(\alpha))' title='\mathrm{R}^ih_*(\mathcal{L}(\alpha))' class='latex' /> vanish.</li>
<li>Otherwise, there is a unique <img src='http://l.wordpress.com/latex.php?latex=w+%5Cin+S_n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w \in S_n' title='w \in S_n' class='latex' /> such that <img src='http://l.wordpress.com/latex.php?latex=%5Cbeta+%3D+w%5E%5Cbullet%28%5Calpha%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\beta = w^\bullet(\alpha)' title='\beta = w^\bullet(\alpha)' class='latex' /> is a dominant weight. In this case, if <img src='http://l.wordpress.com/latex.php?latex=i+%5Cne+%5Cell%28w%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='i \ne \ell(w)' title='i \ne \ell(w)' class='latex' />, then <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BR%7D%5Eih_%2A%5Ei%28%5Cmathcal%7BL%7D%28%5Calpha%29%29+%3D+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{R}^ih_*^i(\mathcal{L}(\alpha)) = 0' title='\mathrm{R}^ih_*^i(\mathcal{L}(\alpha)) = 0' class='latex' />, and <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BR%7D%5E%7B%5Cell%28w%29%7Dh_%2A%28%5Cmathcal%7BL%7D%28%5Calpha%29%29+%3D+K_%5Cbeta%28%5Cmathcal%7BE%7D%5E%2A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{R}^{\ell(w)}h_*(\mathcal{L}(\alpha)) = K_\beta(\mathcal{E}^*)' title='\mathrm{R}^{\ell(w)}h_*(\mathcal{L}(\alpha)) = K_\beta(\mathcal{E}^*)' class='latex' /> is an equivariant bundle whose fibers are the dual of the irreducible representation of <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BGL%7D%28n%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{GL}(n)' title='\mathbf{GL}(n)' class='latex' /> with highest weight <img src='http://l.wordpress.com/latex.php?latex=%5Cbeta&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\beta' title='\beta' class='latex' />.</li>
</ol>
<p>This gives us the cohomology for line bundles over G/B since when X is a point (and hence <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BE%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{E}' title='\mathcal{E}' class='latex' /> is just a vector space), the higher direct images become cohomology groups.</p>
<p>If we assume this theorem, we can use the Leray spectral sequence to extract some information about vector bundles on partial flag varieties. Let <img src='http://l.wordpress.com/latex.php?latex=b+%3D+%280%3Db_0%2C+b_1%2C+%5Cdots%2C+b_r%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='b = (0=b_0, b_1, \dots, b_r)' title='b = (0=b_0, b_1, \dots, b_r)' class='latex' /> be a sequence of increasing numbers, and let <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BFl%7D%28b%3B+%5Cmathcal%7BE%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{Fl}(b; \mathcal{E})' title='\mathrm{Fl}(b; \mathcal{E})' class='latex' /> be the relative partial flag variety (i.e., the fibers are flags <img src='http://l.wordpress.com/latex.php?latex=F_%5Cbullet+%3D+%28F_%7Bi_1%7D+%5Csubset+F_%7Bi_2%7D+%5Csubset+%5Ccdots+%5Csubset+F_%7Bi_r%7D+%5Csubset+k%5En%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F_\bullet = (F_{i_1} \subset F_{i_2} \subset \cdots \subset F_{i_r} \subset k^n)' title='F_\bullet = (F_{i_1} \subset F_{i_2} \subset \cdots \subset F_{i_r} \subset k^n)' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=%5Cdim+F_%7Bi_j%7D+%3D+b_j&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\dim F_{i_j} = b_j' title='\dim F_{i_j} = b_j' class='latex' />. So we still have the tautological bundles <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BR%7D_%7Bb_i%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{R}_{b_i}' title='\mathcal{R}_{b_i}' class='latex' />. For each r&gt;j&gt;0, let <img src='http://l.wordpress.com/latex.php?latex=%5Calpha%5Ej&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha^j' title='\alpha^j' class='latex' /> be a nonincreasing sequence of numbers of length <img src='http://l.wordpress.com/latex.php?latex=b_j+-+b_%7Bj-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='b_j - b_{j-1}' title='b_j - b_{j-1}' class='latex' />, and write <img src='http://l.wordpress.com/latex.php?latex=%5Calpha+%3D+%28%5Calpha%5E1%2C+%5Cdots%2C+%5Calpha%5Er%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha = (\alpha^1, \dots, \alpha^r)' title='\alpha = (\alpha^1, \dots, \alpha^r)' class='latex' /> (this is an n-tuple of numbers, not an r-tuple of sequences). Then we can define a bundle <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BV%7D%28%5Calpha%29+%3D+K_%7B%5Calpha%5E1%7D%28%5Cmathcal%7BR%7D_%7Bb_1%7D%29%5E%2A+%5Cotimes+%5Ccdots+%5Cotimes+K_%7B%5Calpha%5Er%7D%28%5Cmathcal%7BR%7D_%7Bb_r%7D+%2F+%5Cmathcal%7BR%7D_%7Bb_%7Br-1%7D%7D%29%5E%2A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{V}(\alpha) = K_{\alpha^1}(\mathcal{R}_{b_1})^* \otimes \cdots \otimes K_{\alpha^r}(\mathcal{R}_{b_r} / \mathcal{R}_{b_{r-1}})^*' title='\mathcal{V}(\alpha) = K_{\alpha^1}(\mathcal{R}_{b_1})^* \otimes \cdots \otimes K_{\alpha^r}(\mathcal{R}_{b_r} / \mathcal{R}_{b_{r-1}})^*' class='latex' />. Now Bott&#8217;s theorem is the same as above except <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BFl%7D%28b%3B+%5Cmathcal%7BE%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{Fl}(b; \mathcal{E})' title='\mathrm{Fl}(b; \mathcal{E})' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BV%7D%28%5Calpha%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{V}(\alpha)' title='\mathcal{V}(\alpha)' class='latex' /> replace <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BFl%7D%28%5Cmathcal%7BE%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{Fl}(\mathcal{E})' title='\mathrm{Fl}(\mathcal{E})' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BL%7D%28%5Calpha%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{L}(\alpha)' title='\mathcal{L}(\alpha)' class='latex' />, respectively.</p>
<p>To deduce this version, note that we have a forgetful morphism <img src='http://l.wordpress.com/latex.php?latex=f+%5Ccolon+%5Cmathrm%7BFl%7D%28%5Cmathcal%7BE%7D+%5Cto+%5Cmathrm%7BFl%7D%28b%3B+%5Cmathcal%7BE%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f \colon \mathrm{Fl}(\mathcal{E} \to \mathrm{Fl}(b; \mathcal{E})' title='f \colon \mathrm{Fl}(\mathcal{E} \to \mathrm{Fl}(b; \mathcal{E})' class='latex' />, which is a locally trivial fibration whose fibers are products of complete flag varieties. On <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BFl%7D%28%5Cmathcal%7BE%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{Fl}(\mathcal{E})' title='\mathrm{Fl}(\mathcal{E})' class='latex' />, we can construct the line bundle <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BL%7D%28%5Calpha%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{L}(\alpha)' title='\mathcal{L}(\alpha)' class='latex' /> as before. Using the relative version of Bott&#8217;s theorem and induction on the number of terms that we forget, we see that <img src='http://l.wordpress.com/latex.php?latex=f_%2A%28%5Cmathcal%7BL%7D%28%5Calpha%29%29+%3D+%5Cmathcal%7BV%7D%28%5Calpha%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f_*(\mathcal{L}(\alpha)) = \mathcal{V}(\alpha)' title='f_*(\mathcal{L}(\alpha)) = \mathcal{V}(\alpha)' class='latex' />, and its higher direct images vanish because we assumed that each <img src='http://l.wordpress.com/latex.php?latex=%5Calpha%5Ej&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha^j' title='\alpha^j' class='latex' /> was a dominant weight. Letting <img src='http://l.wordpress.com/latex.php?latex=h+%5Ccolon+%5Cmathrm%7BFl%7D%28b%3B+%5Cmathcal%7BE%7D%29+%5Cto+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='h \colon \mathrm{Fl}(b; \mathcal{E}) \to X' title='h \colon \mathrm{Fl}(b; \mathcal{E}) \to X' class='latex' /> be the structure map, we can also use the relative Bott&#8217;s theorem to calculate <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BR%7D%5Ei%28hf%29_%2A%28%5Cmathcal%7BL%7D%28%5Calpha%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{R}^i(hf)_*(\mathcal{L}(\alpha))' title='\mathrm{R}^i(hf)_*(\mathcal{L}(\alpha))' class='latex' />. Alternatively, we have the Leray spectral sequence <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BE%7D_2%5E%7Bp%2Cq%7D+%3D+%28%5Cmathrm%7BR%7D%5Eph_%2A+%5Ccirc+%5Cmathrm%7BR%7D%5Eqf_%2A%29%28%5Cmathcal%7BL%7D%28%5Calpha%29%29+%5CRightarrow+%5Cmathrm%7BR%7D%5E%7Bp%2Bq%7D%28hf%29_%2A%28%5Cmathcal%7BL%7D%28%5Calpha%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{E}_2^{p,q} = (\mathrm{R}^ph_* \circ \mathrm{R}^qf_*)(\mathcal{L}(\alpha)) \Rightarrow \mathrm{R}^{p+q}(hf)_*(\mathcal{L}(\alpha))' title='\mathrm{E}_2^{p,q} = (\mathrm{R}^ph_* \circ \mathrm{R}^qf_*)(\mathcal{L}(\alpha)) \Rightarrow \mathrm{R}^{p+q}(hf)_*(\mathcal{L}(\alpha))' class='latex' />. But we just showed that these terms are 0 for q=0, so the spectral sequence degenerates and we conclude that <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BR%7D%5Eph_%2A%28%5Cmathcal%7BV%7D%28%5Calpha%29%29+%3D+%5Cmathcal%7BR%7D%5Ep%28hf%29_%2A%28%5Cmathcal%7BL%7D%28%5Calpha%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{R}^ph_*(\mathcal{V}(\alpha)) = \mathcal{R}^p(hf)_*(\mathcal{L}(\alpha))' title='\mathrm{R}^ph_*(\mathcal{V}(\alpha)) = \mathcal{R}^p(hf)_*(\mathcal{L}(\alpha))' class='latex' />.</p>
<p>I&#8217;ll end this post with what this all says on projective space, and next time I&#8217;ll discuss how we can use this special case to construct equivariant pure modules and supernatural vector bundles.</p>
<p>Over projective space <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BP%7D%28E%29+%5Ccong+%5Cmathbf%7BP%7D%5E%7Bn-1%7D_k&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{P}(E) \cong \mathbf{P}^{n-1}_k' title='\mathbf{P}(E) \cong \mathbf{P}^{n-1}_k' class='latex' />, the fiber of the tautological bundle <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BR%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{R}' title='\mathcal{R}' class='latex' /> over a point (which is a line in <img src='http://l.wordpress.com/latex.php?latex=E+%5Ccong+k%5En&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='E \cong k^n' title='E \cong k^n' class='latex' />) is the simply the vectors lying in that line. This is also the total space of the dual of the Serre twisting sheaf <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BO%7D_%7B%5Cmathbf%7BP%7D%28E%29%7D%28-1%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{O}_{\mathbf{P}(E)}(-1)' title='\mathcal{O}_{\mathbf{P}(E)}(-1)' class='latex' />. Given the inclusion <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BR%7D+%5Csubset+E+%5Ctimes+%5Cmathbf%7BP%7D%28E%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{R} \subset E \times \mathbf{P}(E)' title='\mathcal{R} \subset E \times \mathbf{P}(E)' class='latex' />, the quotient will be called <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BQ%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{Q}' title='\mathcal{Q}' class='latex' /> and called the tautological quotient. Then our bundles of interest are of the form <img src='http://l.wordpress.com/latex.php?latex=K_u%5Cmathcal%7BR%7D+%5Cotimes+K_%5Calpha+%5Cmathcal%7BQ%7D+%3D+%28K_%5Calpha+%5Cmathcal%7BQ%7D%29%28-u%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K_u\mathcal{R} \otimes K_\alpha \mathcal{Q} = (K_\alpha \mathcal{Q})(-u)' title='K_u\mathcal{R} \otimes K_\alpha \mathcal{Q} = (K_\alpha \mathcal{Q})(-u)' class='latex' /> where u is an integer and <img src='http://l.wordpress.com/latex.php?latex=%5Calpha+%3D+%28%5Calpha_1+%5Cge+%5Calpha_2+%5Cge+%5Ccdots+%5Cge+%5Calpha_%7Bn-1%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha = (\alpha_1 \ge \alpha_2 \ge \cdots \ge \alpha_{n-1})' title='\alpha = (\alpha_1 \ge \alpha_2 \ge \cdots \ge \alpha_{n-1})' class='latex' />. Note that this is the same <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BV%7D%28%5Cgamma%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{V}(\gamma)' title='\mathcal{V}(\gamma)' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma+%3D+%28-u%2C+-%5Calpha_%7Bn-1%7D%2C+...%2C+-%5Calpha_1%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma = (-u, -\alpha_{n-1}, ..., -\alpha_1)' title='\gamma = (-u, -\alpha_{n-1}, ..., -\alpha_1)' class='latex' /> by duality. Hence the theorem says</p>
<p><strong>Theorem.</strong> With the notation above, one of two mutually exclusive cases occurs:</p>
<ol>
<li>There exists a nonidentity element <img src='http://l.wordpress.com/latex.php?latex=w+%5Cin+S_n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w \in S_n' title='w \in S_n' class='latex' /> such that <img src='http://l.wordpress.com/latex.php?latex=w%5E%5Cbullet%28%5Calpha_1%2C+%5Cdots%2C+%5Calpha_%7Bn-1%7D%2C+u%29+%3D+%5Calpha&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w^\bullet(\alpha_1, \dots, \alpha_{n-1}, u) = \alpha' title='w^\bullet(\alpha_1, \dots, \alpha_{n-1}, u) = \alpha' class='latex' />. In this case, all cohomology groups <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BH%7D%5Ei%28%5Cmathbf%7BP%7D%28E%29%3B+K_%5Calpha%5Cmathcal%7BQ%7D%28-u%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{H}^i(\mathbf{P}(E); K_\alpha\mathcal{Q}(-u))' title='\mathrm{H}^i(\mathbf{P}(E); K_\alpha\mathcal{Q}(-u))' class='latex' /> vanish.</li>
<li>Otherwise, there is a unique <img src='http://l.wordpress.com/latex.php?latex=w+%5Cin+S_n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w \in S_n' title='w \in S_n' class='latex' /> such that <img src='http://l.wordpress.com/latex.php?latex=%5Cbeta+%3D+w%5E%5Cbullet%28%5Calpha_1%2C+%5Cdots%2C+%5Calpha_%7Bn-1%7D%2C+u%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\beta = w^\bullet(\alpha_1, \dots, \alpha_{n-1}, u)' title='\beta = w^\bullet(\alpha_1, \dots, \alpha_{n-1}, u)' class='latex' /> is nondecreasing. In this case, if <img src='http://l.wordpress.com/latex.php?latex=i+%5Cne+%5Cell%28w%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='i \ne \ell(w)' title='i \ne \ell(w)' class='latex' />, then <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BH%7D%5Ei%28%5Cmathbf%7BP%7D%28E%29%3B+%28K_%5Calpha+%5Cmathcal%7BQ%7D%29%28-u%29%29+%3D+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{H}^i(\mathbf{P}(E); (K_\alpha \mathcal{Q})(-u)) = 0' title='\mathrm{H}^i(\mathbf{P}(E); (K_\alpha \mathcal{Q})(-u)) = 0' class='latex' />, and <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BH%7D%5E%7B%5Cell%28w%29%7D%28%5Cmathbf%7BP%7D%28E%29%3B+%28K_%5Calpha+%5Cmathcal%7BQ%7D%29%28-u%29%29+%3D+K_%5Cbeta%28E%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{H}^{\ell(w)}(\mathbf{P}(E); (K_\alpha \mathcal{Q})(-u)) = K_\beta(E)' title='\mathrm{H}^{\ell(w)}(\mathbf{P}(E); (K_\alpha \mathcal{Q})(-u)) = K_\beta(E)' class='latex' /> is an irreducible representation of <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BGL%7D%28E%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{GL}(E)' title='\mathbf{GL}(E)' class='latex' /> with highest weight <img src='http://l.wordpress.com/latex.php?latex=%5Cbeta&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\beta' title='\beta' class='latex' />.</li>
</ol>
<p>-Steven</p>
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		<title>Boij–Söderberg theory III: proofs</title>
		<link>http://concretenonsense.wordpress.com/2009/04/02/boij%e2%80%93soderberg-theory-iii-proofs/</link>
		<comments>http://concretenonsense.wordpress.com/2009/04/02/boij%e2%80%93soderberg-theory-iii-proofs/#comments</comments>
		<pubDate>Thu, 02 Apr 2009 01:11:55 +0000</pubDate>
		<dc:creator>Steven Sam</dc:creator>
				<category><![CDATA[Algebraic Geometry]]></category>
		<category><![CDATA[commutative algebra]]></category>
		<category><![CDATA[Betti tables]]></category>

		<guid isPermaLink="false">http://concretenonsense.wordpress.com/?p=379</guid>
		<description><![CDATA[It&#8217;s been a while since the last post, but I want to give an indication of how the Eisenbud and Schreyer proved the Boij–Söderberg conjectures. This fell into roughly 3 steps. There are some constructions that are involved which I will not mention, but may mention in a future post. In particular, I will take [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=concretenonsense.wordpress.com&blog=2918042&post=379&subd=concretenonsense&ref=&feed=1" />]]></description>
			<content:encoded><![CDATA[<div class='snap_preview'><br /><p>It&#8217;s been a while since the last post, but I want to give an indication of how the Eisenbud and Schreyer proved the Boij–Söderberg conjectures. This fell into roughly 3 steps. There are some constructions that are involved which I will not mention, but may mention in a future post. In particular, I will take it as a given that for any given degree sequence d, there exists a Cohen–Macaulay module M whose Betti diagram is pure with degree sequence d. Recall the setup from the <a href="http://concretenonsense.wordpress.com/2009/03/08/boij–soderberg-theory-ii-the-cohen–macaulay-property/">previous post</a>: we picked degree sequences <img src='http://l.wordpress.com/latex.php?latex=%5Coverline%7Bd%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\overline{d}' title='\overline{d}' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=%5Cunderline%7Bd%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\underline{d}' title='\underline{d}' class='latex' /> to restrict our attention to a finite-dimensional space of Betti tables.</p>
<p><strong>Step 1</strong>: Identify the exterior facets of the cone spanned by the pure diagrams.</p>
<p>This step was done by Boij and Söderberg in their <a href="http://arxiv.org/abs/math/0611081">original paper</a>. Recall that we put a partial ordering on the set of degree sequences given by pointwise comparison and that the cone spanned by the pure diagrams offers a geometric realization of this poset. In particular, the facets are given by chains of degree sequences which are obtained uniquely by removing a single element <img src='http://l.wordpress.com/latex.php?latex=%5Cpi%28d_i%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi(d_i)' title='\pi(d_i)' class='latex' /> from a maximal chain <img src='http://l.wordpress.com/latex.php?latex=%5Cpi+%3D+%28%5Cpi%28d_1%29+%3C+%5Ccdots+%5Cpi%28d_q%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi = (\pi(d_1) &lt; \cdots \pi(d_q))' title='\pi = (\pi(d_1) &lt; \cdots \pi(d_q))' class='latex' />. The uniqueness part means that there do not exist two different maximal chains such that one can remove a single element from each to get the same resulting chain. Let i denote the index of the degree sequence that was removed. They classified the exterior facets into three types:</p>
<p>Case 1: We remove the maximal or minimal element.</p>
<p>Case 2: The degree sequences <img src='http://l.wordpress.com/latex.php?latex=%5Cpi%28d_%7Bi-1%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi(d_{i-1})' title='\pi(d_{i-1})' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=%5Cpi%28d_%7Bi%2B1%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi(d_{i+1})' title='\pi(d_{i+1})' class='latex' /> differ in exactly one entry.</p>
<p>Case 3: The degree sequences <img src='http://l.wordpress.com/latex.php?latex=%5Cpi%28d_%7Bi-1%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi(d_{i-1})' title='\pi(d_{i-1})' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=%5Cpi%28d_%7Bi%2B1%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi(d_{i+1})' title='\pi(d_{i+1})' class='latex' /> differ in exactly two entries.<br />
<span id="more-379"></span><br />
In both cases 1 and 2, there is a unique coordinate x of the Betti table that is nonzero for <img src='http://l.wordpress.com/latex.php?latex=%5Cpi%28d_i%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi(d_i)' title='\pi(d_i)' class='latex' /> but zero for the other degree sequences in the chain. In this case, x gives a linear functional which is positive on the set of all Betti tables and is zero on the facet in question. The nontrivial case of course is case 3. The first thing Eisenbud and Schreyer show in this case is that there is a hyperplane which contains this facet and those degree sequences which are greater than or equal to <img src='http://l.wordpress.com/latex.php?latex=%5Cpi%28d_%7Bi%2B1%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi(d_{i+1})' title='\pi(d_{i+1})' class='latex' />, and furthermore that this hyperplane is unique. Similarly, one can obtain a hyperplane which contains all degree sequences less than or equal to <img src='http://l.wordpress.com/latex.php?latex=%5Cpi%28d_%7Bi-1%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi(d_{i-1})' title='\pi(d_{i-1})' class='latex' />. The construction of the linear functionals is inductive and we won&#8217;t repeat it here. The point is that given this uniqueness, one can hope to reconstruct these linear functionals in a different way which illucidates that they are nonnegative on the set of Betti tables. We sketch this in the next section.</p>
<p><strong>Step 2</strong>: Define a bilinear pairing between Betti tables and cohomology tables.</p>
<p>This may seem to stray from our goal, but in fact, this is the crucial observation to showing that the case 3 linear functionals in Step 1 are in fact positive on all Betti tables. The point will be that it is easy to show positivity for this pairing, and then one need only pick the right cohomology tables to get the desired facet-defining equations. Here of course I will sketch only the constructions and give some ideas, since there are far too many details to discuss.</p>
<p>First, let <img src='http://l.wordpress.com/latex.php?latex=%5Cbeta&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\beta' title='\beta' class='latex' /> be a graded Betti table, and let <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma' title='\gamma' class='latex' /> be a graded cohomology table (i.e., the degrees of some cochain complex). Eisenbud and Schreyer introduce a bilinear functional <img src='http://l.wordpress.com/latex.php?latex=%5Clangle+%5Cbeta%2C+%5Cgamma+%5Crangle+%3D+%5Csum_%7B%5C%7B+i%2Cj%2Ck+%5Cmid+j+%5Cle+i%5C%7D+%7D+%28-1%29%5E%7Bi-j%7D+%5Cbeta_%7Bi%2Ck%7D+%5Cgamma_%7Bj%2C-k%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\langle \beta, \gamma \rangle = \sum_{\{ i,j,k \mid j \le i\} } (-1)^{i-j} \beta_{i,k} \gamma_{j,-k}' title='\langle \beta, \gamma \rangle = \sum_{\{ i,j,k \mid j \le i\} } (-1)^{i-j} \beta_{i,k} \gamma_{j,-k}' class='latex' />. In the case that <img src='http://l.wordpress.com/latex.php?latex=%5Cbeta&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\beta' title='\beta' class='latex' /> comes from a free resolution F and <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma' title='\gamma' class='latex' /> comes from a cochain complex E, we can write this sum as <img src='http://l.wordpress.com/latex.php?latex=%5Csum_j+%5Cchi%28F_%7B%5Cge+j%7D+%5Cotimes+%5Cmathrm%7BH%7D%5Ej%28E%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\sum_j \chi(F_{\ge j} \otimes \mathrm{H}^j(E))' title='\sum_j \chi(F_{\ge j} \otimes \mathrm{H}^j(E))' class='latex' />. Here <img src='http://l.wordpress.com/latex.php?latex=F_%7B%5Cge+j%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F_{\ge j}' title='F_{\ge j}' class='latex' /> denotes the truncation of F to degrees at least j, and <img src='http://l.wordpress.com/latex.php?latex=%5Cchi&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\chi' title='\chi' class='latex' />  denotes the usual Euler characteristic. The next step is to examine the double complex <img src='http://l.wordpress.com/latex.php?latex=F+%5Cotimes+E&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F \otimes E' title='F \otimes E' class='latex' /> where we think of F as having cohomological indices, i.e., <img src='http://l.wordpress.com/latex.php?latex=F%5Ei+%3D+F_%7B-i%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F^i = F_{-i}' title='F^i = F_{-i}' class='latex' />. We assume that E is bounded and consists of free modules since we only need this case. Since F is a resolution, the total cohomology of this complex is zero in negative cohomological degrees (seen by using the spectral sequence that starts by computing cohomology of the rows <img src='http://l.wordpress.com/latex.php?latex=F_%5Cbullet+%5Cotimes+E%5Ej&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F_\bullet \otimes E^j' title='F_\bullet \otimes E^j' class='latex' />). But we&#8217;re really interested in some truncation of this double complex, so we go to the next page of the spectral sequence starting in the other direction (along columns) and then remove the things with positive cohomological index (they don&#8217;t appear in our bilinear form). Then in fact our bilinear form can be identified with the Euler characteristic of the total cohomology of this truncation. But we know that the total cohomology vanishes in negative degrees, and we&#8217;ve removed the positive part, so in fact our bilinear form is just the dimension of the degree 0 part of the total cohomology of the truncated double complex, and hence nonnegative. Doing some more analysis, one can determine when this total cohomology vanishes, but we&#8217;ll skip that.</p>
<p>Unfortunately, this isn&#8217;t quite good enough. For one thing, we have not used the fact that F should be a minimal free resolution. To get around this, Eisenbud and Schreyer introduce a second bilinear form which is some kind of augmentation of the one above. Then using nonnegativity of the original bilinear form, they show that the augmented one is nonnegative when F is a minimal free resolution, and this is form is the correct thing to proceed with.</p>
<p><strong>Step 3</strong>: Find the appropriate cochain complexes.</p>
<p>What is needed are cochain complexes which have the right vanishing conditions (which I didn&#8217;t explain) subject to the above bilinear form. Briefly I can say where these come from. The first way to get interesting cochain complexes is via linear monads for vector bundles on (n-1)-dimensional projective space (here n is the number of variables of our polynomial ring). What this means precisely is if <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BE%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{E}' title='\mathcal{E}' class='latex' /> is a vector bundle on <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BP%7D%5E%7Bn-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{P}^{n-1}' title='\mathbf{P}^{n-1}' class='latex' /> such that its dual bundle <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BE%7D%5E%2A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{E}^*' title='\mathcal{E}^*' class='latex' /> is a-regular (a-regular means that <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BH%7D%5Ei+%5Cmathcal%7BE%5E%2A%7D%28a-j%29%29+%3D+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{H}^i \mathcal{E^*}(a-j)) = 0' title='\mathrm{H}^i \mathcal{E^*}(a-j)) = 0' class='latex' /> for i&gt;0), then there exists a linear complex E such that <img src='http://l.wordpress.com/latex.php?latex=E%5Ek+%3D+A%28a%2Bk%29%5E%7Bb_k%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='E^k = A(a+k)^{b_k}' title='E^k = A(a+k)^{b_k}' class='latex' /> (here A is our polynomial ring, and the <img src='http://l.wordpress.com/latex.php?latex=b_k&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='b_k' title='b_k' class='latex' /> are just some integers) whose cohomology is close to the cohomology of <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BE%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{E}' title='\mathcal{E}' class='latex' />. To be more precise, <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BH%7D%5Ei%28E%29+%3D+%5Csum_d+%5Cmathrm%7BH%7D%5Ei+%5Cmathcal%7BE%7D%28d%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{H}^i(E) = \sum_d \mathrm{H}^i \mathcal{E}(d)' title='\mathrm{H}^i(E) = \sum_d \mathrm{H}^i \mathcal{E}(d)' class='latex' /> for i &lt; n-1, and <img src='http://l.wordpress.com/latex.php?latex=%5Cmathrm%7BH%7D%5E%7Bn-1%7D%28E%29+%3D+%5Csum_%7Bd+%3E+-a-n%7D+%5Cmathrm%7BH%7D%5E%7Bn-1%7D%5Cmathcal%7BE%7D%28d%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathrm{H}^{n-1}(E) = \sum_{d &gt; -a-n} \mathrm{H}^{n-1}\mathcal{E}(d)' title='\mathrm{H}^{n-1}(E) = \sum_{d &gt; -a-n} \mathrm{H}^{n-1}\mathcal{E}(d)' class='latex' />. Without going too much deeper, I will just end by saying then that the vector bundles whose linear monads give the desired linear functionals are those with supernatural cohomology. To be more precise, this means that 1) each twist of the vector bundle has at most one nonzero cohomology group, and 2) the roots of its Hilbert polynomial are all integers. Eisenbud and Schreyer show that given any prescribed set of integers, there indeed exists a supernatural vector bundle whose roots are precisely those integers (this is in some sense, dual to the problem of construction pure CM modules with a given degree sequence). To get the ones that give our linear functionals, the roots are chosen according to the chain of degree sequences that the facet is defined by. As an unexpected bonus, one can use the bilinear functionals to show that every cohomology table of a vector bundle on <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BP%7D%5E%7Bn-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{P}^{n-1}' title='\mathbf{P}^{n-1}' class='latex' /> is a positive linear combination of the supernatural cohomology tables.</p>
<p>And this is about as much as I want to say. Sorry if this post seemed much more dense than the others, but hopefully this gives some kind of picture of what goes behind this particular theorem. The interersted reader should of course consult <a href="http://arxiv.org/abs/0712.1843">Eisenbud and Schreyer&#8217;s paper</a>.</p>
<p>I may say some more about the existence of supernatural vector bundles and pure CM modules in a later post. They exist over any arbitrary field, but in characteristic 0, one can get <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BGL%7D%28n%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{GL}(n)' title='\mathbf{GL}(n)' class='latex' />-equivariant sheaves and modules using the Borel–Weil–Bott theorem, and I&#8217;ll try to say something about the equivariant constructions later.</p>
<p>-Steven</p>
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		<title>Boij–Söderberg theory II: the Cohen–Macaulay property</title>
		<link>http://concretenonsense.wordpress.com/2009/03/08/boij%e2%80%93soderberg-theory-ii-the-cohen%e2%80%93macaulay-property/</link>
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		<pubDate>Sun, 08 Mar 2009 21:59:44 +0000</pubDate>
		<dc:creator>Steven Sam</dc:creator>
				<category><![CDATA[Algebraic Geometry]]></category>
		<category><![CDATA[commutative algebra]]></category>
		<category><![CDATA[Betti tables]]></category>

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		<description><![CDATA[Last time in this post, I gave an introduction to minimal resolutions over polynomial rings and stated a theorem of Eisenbud and Schreyer. This time I want to describe the significance of the Cohen–Macaulay property, and in part III, I will start explaining the proof of the Boij–Söderberg conjectures.
The first point to address is the [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=concretenonsense.wordpress.com&blog=2918042&post=351&subd=concretenonsense&ref=&feed=1" />]]></description>
			<content:encoded><![CDATA[<div class='snap_preview'><br /><p>Last time in <a href="http://concretenonsense.wordpress.com/2009/02/24/boij–soderberg-theory-i-preliminaries/">this post</a>, I gave an introduction to minimal resolutions over polynomial rings and stated a theorem of Eisenbud and Schreyer. This time I want to describe the significance of the Cohen–Macaulay property, and in part III, I will start explaining the proof of the Boij–Söderberg conjectures.</p>
<p>The first point to address is the notion of a Cohen–Macaulay module. Let&#8217;s first assume that M is a module over a local ring R with maximal ideal P (either this is an actual local ring, or R is graded, and it has a unique homogeneous maximal ideal). An <strong>M-sequence</strong> <img src='http://l.wordpress.com/latex.php?latex=x_1%2C+%5Cdots%2C+x_n+%5Cin+P&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='x_1, \dots, x_n \in P' title='x_1, \dots, x_n \in P' class='latex' /> satisfies 1) multiplication by <img src='http://l.wordpress.com/latex.php?latex=x_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='x_i' title='x_i' class='latex' /> is an injective function <img src='http://l.wordpress.com/latex.php?latex=M_%7Bi-1%7D+%5Cto+M_%7Bi-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='M_{i-1} \to M_{i-1}' title='M_{i-1} \to M_{i-1}' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=M_0+%3D+M&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='M_0 = M' title='M_0 = M' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=M_%7Bi-1%7D+%3D+M+%2F+%28x_1%2C+%5Cdots%2C+x_%7Bi-1%7D%29+M&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='M_{i-1} = M / (x_1, \dots, x_{i-1}) M' title='M_{i-1} = M / (x_1, \dots, x_{i-1}) M' class='latex' /> for i&gt;0, and 2) <img src='http://l.wordpress.com/latex.php?latex=%28x_1%2C+%5Cdots%2C+x_n%29+M+%5Cne+M&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(x_1, \dots, x_n) M \ne M' title='(x_1, \dots, x_n) M \ne M' class='latex' />, and the <strong>depth</strong> of M, depth(P,M), is the longest length of an M-sequence. The <strong>dimension</strong> of M, denoted dim(M), is the Krull dimension of R / ann(M) where ann(M) denotes the annihilator ideal of M. In general, the inequality <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bdim%7D%28M%29+%5Cge+%5Ctext%7Bdepth%7D%28P%2CM%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{dim}(M) \ge \text{depth}(P,M)' title='\text{dim}(M) \ge \text{depth}(P,M)' class='latex' /> holds, and we say that M is <strong>Cohen–Macaulay</strong> (CM from now on) in case of equality. The ring R is CM if it is CM as a module over itself, and we extend these definitions to the global case by saying that a ring / module is CM if its localization at every maximal ideal is CM. But actually, since we will be dealing with graded modules, we will think of the polynomial ring <img src='http://l.wordpress.com/latex.php?latex=K%5Bx_1%2C+%5Cdots%2C+x_n%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K[x_1, \dots, x_n]' title='K[x_1, \dots, x_n]' class='latex' /> as a &#8220;local graded ring&#8221; because it has a unique homogeneous maximal ideal.<br />
<span id="more-351"></span><br />
The important point is that this is the right condition to be able to write down some nice equations. First we should point out that polynomial rings over fields are CM.  Now let M be a finitely generated module over a ring R with finite projective dimension, denoted pd(M) (this means that the shortest projective resolution we can find for M has length pd(M)). Furthermore, if either 1) R is a local ring and P is its maximal ideal, or 2) R is a finitely generated positively graded ring with <img src='http://l.wordpress.com/latex.php?latex=R_0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='R_0' title='R_0' class='latex' /> a field, M is a graded R-module, and P is its maximal homogeneous ideal <img src='http://l.wordpress.com/latex.php?latex=R_1+%5Coplus+R_2+%5Coplus+%5Ccdots&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='R_1 \oplus R_2 \oplus \cdots' title='R_1 \oplus R_2 \oplus \cdots' class='latex' />, then we have</p>
<p><strong>Theorem</strong> (Auslander–Buchsbaum).  pd(M) = depth(P,R) &#8211; depth(P,M).</p>
<p>In particular, if we let R be the polynomial ring in n variables over K, then depth(P,R) = n, and if in addition M is CM, this says that dim(M) = n &#8211; pd(M). How is this relevant? We&#8217;ll unfortunately need some more definitions. First, give M as above, define the <strong>Hilbert function</strong> <img src='http://l.wordpress.com/latex.php?latex=h_M%28n%29+%3D+%5Ctext%7Bdim%7D_K+M_n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='h_M(n) = \text{dim}_K M_n' title='h_M(n) = \text{dim}_K M_n' class='latex' /> (here we mean vector space dimension) and the <strong>Hilbert series</strong> <img src='http://l.wordpress.com/latex.php?latex=H_M%28t%29+%3D+%5Csum_%7Bn+%5Cge+0%7D+h_M%28n%29+t%5En&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H_M(t) = \sum_{n \ge 0} h_M(n) t^n' title='H_M(t) = \sum_{n \ge 0} h_M(n) t^n' class='latex' />.</p>
<p><strong>Theorem</strong> (Hilbert–Serre). Let M be a finitely generated positively graded module over <img src='http://l.wordpress.com/latex.php?latex=A+%3D+K%5Bx_1%2C+%5Cdots%2C+x_n%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='A = K[x_1, \dots, x_n]' title='A = K[x_1, \dots, x_n]' class='latex' />, and let d = dim(M). Then there exists a polynomial R(t) with integer coefficients such that</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+H_M%28t%29+%3D+%5Cfrac%7BR%28t%29%7D%7B%281-t%29%5Ed%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle H_M(t) = \frac{R(t)}{(1-t)^d}' title='\displaystyle H_M(t) = \frac{R(t)}{(1-t)^d}' class='latex' />.</p>
<p>Now here&#8217;s where we can begin. First, we will assume that all modules we are dealing with are CM and of codimension c=n-d. Let <img src='http://l.wordpress.com/latex.php?latex=A+%3D+K%5Bx_1%2C+%5Cdots%2C+x_n%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='A = K[x_1, \dots, x_n]' title='A = K[x_1, \dots, x_n]' class='latex' />, and write down the minimal resolution for a finitely generated graded A-module CM M (the Auslander&#8211;Buchsbaum formula tells us that the length of this resolution must be c):</p>
<p><img src='http://l.wordpress.com/latex.php?latex=0+%5Cto+%5Cbigoplus_j+A%28-j%29%5E%7B%5Cbeta_%7Bc%2Cj%7D%7D+%5Cto+%5Ccdots+%5Cto+%5Cbigoplus_j+A%28-j%29%5E%7B%5Cbeta_%7B0%2Cj%7D%7D+%5Cto+M+%5Cto+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='0 \to \bigoplus_j A(-j)^{\beta_{c,j}} \to \cdots \to \bigoplus_j A(-j)^{\beta_{0,j}} \to M \to 0' title='0 \to \bigoplus_j A(-j)^{\beta_{c,j}} \to \cdots \to \bigoplus_j A(-j)^{\beta_{0,j}} \to M \to 0' class='latex' />.</p>
<p>Since the Hilbert function is additive on degree 0 exact sequences, we can write <img src='http://l.wordpress.com/latex.php?latex=H_M%28t%29+%3D+%5Csum_%7Bi%3D0%7D%5Ec+%28-1%29%5Ei+H_%7BF_i%7D%28t%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H_M(t) = \sum_{i=0}^c (-1)^i H_{F_i}(t)' title='H_M(t) = \sum_{i=0}^c (-1)^i H_{F_i}(t)' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=F_i+%3D+%5Cbigoplus_j+A%28-j%29%5E%7B%5Cbeta_%7Bi%2Cj%7D%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F_i = \bigoplus_j A(-j)^{\beta_{i,j}}' title='F_i = \bigoplus_j A(-j)^{\beta_{i,j}}' class='latex' />. To get <img src='http://l.wordpress.com/latex.php?latex=H_%7BF_i%7D%28t%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H_{F_i}(t)' title='H_{F_i}(t)' class='latex' />, we just note that <img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+H_%7BA%28-j%29%7D%28t%29+%3D+%5Cfrac%7Bt%5Ej%7D%7B%281-t%29%5En%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle H_{A(-j)}(t) = \frac{t^j}{(1-t)^n}' title='\displaystyle H_{A(-j)}(t) = \frac{t^j}{(1-t)^n}' class='latex' />, so we conclude that</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+H_M%28t%29+%3D+%5Csum_%7Bi%3D0%7D%5Ec+%28-1%29%5Ei+%5Csum_j+%5Cfrac%7B%5Cbeta_%7Bi%2Cj%7D+t%5Ej%7D%7B%281-t%29%5En%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle H_M(t) = \sum_{i=0}^c (-1)^i \sum_j \frac{\beta_{i,j} t^j}{(1-t)^n}' title='\displaystyle H_M(t) = \sum_{i=0}^c (-1)^i \sum_j \frac{\beta_{i,j} t^j}{(1-t)^n}' class='latex' />.</p>
<p>Now since M is CM, the Hilbert–Serre theorem tells us that <img src='http://l.wordpress.com/latex.php?latex=H_M%28t%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H_M(t)' title='H_M(t)' class='latex' /> is a polynomial divided by <img src='http://l.wordpress.com/latex.php?latex=%281-t%29%5Ed&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(1-t)^d' title='(1-t)^d' class='latex' />. So this means that the polynomial <img src='http://l.wordpress.com/latex.php?latex=%5Cbeta_M%28t%29+%3D+%5Csum_%7Bi%3D0%7D%5En+%28-1%29%5Ei+%5Csum_j+%5Cbeta_%7Bi%2Cj%7D+t%5Ej&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\beta_M(t) = \sum_{i=0}^n (-1)^i \sum_j \beta_{i,j} t^j' title='\beta_M(t) = \sum_{i=0}^n (-1)^i \sum_j \beta_{i,j} t^j' class='latex' /> must have 1 as a root with multiplicity c. This can be expressed as saying that the first c derivatives of <img src='http://l.wordpress.com/latex.php?latex=%5Cbeta_M%28t%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\beta_M(t)' title='\beta_M(t)' class='latex' /> have 1 as a root, and this gives us c linearly independent equations on the possible Betti numbers of graded CM modules of codimension c. Call these the HK (for Herzog and Kühl) equations. Furthermore, if we assume that M has a pure free resolution, then we can figure out what the Betti numbers have to be up to a multiple. I&#8217;ll spare you the details, but mention that if the degrees of i-th syzygy module is <img src='http://l.wordpress.com/latex.php?latex=d_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='d_i' title='d_i' class='latex' />, i.e., if <img src='http://l.wordpress.com/latex.php?latex=%5Cbeta_%7Bi%2Cj%7D+%3D+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\beta_{i,j} = 0' title='\beta_{i,j} = 0' class='latex' /> unless <img src='http://l.wordpress.com/latex.php?latex=j+%3D+d_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='j = d_i' title='j = d_i' class='latex' />, then they must be of the form</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+%5Cbeta_%7Bi%2C+d_i%7D+%3D+r+%5Cprod_%7Bj+%5Cne+i%7D+%5Cfrac%7B1%7D%7B%7Cd_j+-+d_i%7C%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle \beta_{i, d_i} = r \prod_{j \ne i} \frac{1}{|d_j - d_i|}' title='\displaystyle \beta_{i, d_i} = r \prod_{j \ne i} \frac{1}{|d_j - d_i|}' class='latex' /> (*)</p>
<p>for <img src='http://l.wordpress.com/latex.php?latex=0+%5Cle+i+%5Cle+c&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='0 \le i \le c' title='0 \le i \le c' class='latex' />, and where r is some rational number.</p>
<p>Remember that the theorem of Eisenbud and Schreyer stated that every Betti table of a CM module (of a given codimension c) is a positive rational linear combination of pure Betti tables (of the same codimension). This last statement translates well into convex geometry where it says: in the vector space of all tables of rational numbers with c+1 columns and infinitely many rows, the cone spanned by the pure Betti tables contains all of the Betti tables of CM modules.</p>
<p>Of course, the space of all tables with c+1 columns is infinite-dimensional. To avoid doing infinite-dimensional convex geometry, we can always focus our attention on finite-dimensional subspaces. In particular, fix two degree sequences <img src='http://l.wordpress.com/latex.php?latex=%5Coverline%7Bd%7D+%3D+%28%5Coverline%7Bd%7D_0%2C+%5Cdots%2C+%5Coverline%7Bd%7D_c%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\overline{d} = (\overline{d}_0, \dots, \overline{d}_c)' title='\overline{d} = (\overline{d}_0, \dots, \overline{d}_c)' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=%5Cunderline%7Bd%7D+%3D+%28%5Cunderline%7Bd%7D_0%2C+%5Cdots%2C+%5Cunderline%7Bd%7D_c%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\underline{d} = (\underline{d}_0, \dots, \underline{d}_c)' title='\underline{d} = (\underline{d}_0, \dots, \underline{d}_c)' class='latex' />. We&#8217;ll set <img src='http://l.wordpress.com/latex.php?latex=B_%7B%5B%5Cunderline%7Bd%7D%2C+%5Coverline%7Bd%7D%5D%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='B_{[\underline{d}, \overline{d}]}' title='B_{[\underline{d}, \overline{d}]}' class='latex' /> to be the subspace of tables T such that <img src='http://l.wordpress.com/latex.php?latex=T_%7Bi%2Cj%7D+%3D+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='T_{i,j} = 0' title='T_{i,j} = 0' class='latex' /> unless <img src='http://l.wordpress.com/latex.php?latex=%5Cunderline%7Bd%7D_i+%5Cle+j+%5Cle+%5Coverline%7Bd%7D_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\underline{d}_i \le j \le \overline{d}_i' title='\underline{d}_i \le j \le \overline{d}_i' class='latex' /> and which satisfy the HK equations.</p>
<p>Also, define a partial ordering on the degree sequences by saying that <img src='http://l.wordpress.com/latex.php?latex=%28d_0%2C+%5Cdots%2C+d_c%29+%5Cle+%28d%27_0%2C+%5Cdots%2C+d%27_c%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(d_0, \dots, d_c) \le (d&#039;_0, \dots, d&#039;_c)' title='(d_0, \dots, d_c) \le (d&#039;_0, \dots, d&#039;_c)' class='latex' /> if <img src='http://l.wordpress.com/latex.php?latex=d_i+%5Cle+d%27_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='d_i \le d&#039;_i' title='d_i \le d&#039;_i' class='latex' /> for all i. It is something which remains to be proved that for every degree sequence d, there exists a CM module with a pure free resolution of degree d, but we will postpone that. The key point is that one can deduce from (*) that Betti tables corresponding to degree sequences in a chain are linearly independent. The number of degree sequences in a maximal chain <img src='http://l.wordpress.com/latex.php?latex=d%5E0+%3C+d%5E1+%3C+%5Ccdots+%3C+d%5EN&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='d^0 &lt; d^1 &lt; \cdots &lt; d^N' title='d^0 &lt; d^1 &lt; \cdots &lt; d^N' class='latex' /> is <img src='http://l.wordpress.com/latex.php?latex=N+%3D+1+%2B+%5Csum_%7Bi%3D0%7D%5Ec+%28%5Coverline%7Bd%7D_i+-+%5Cunderline%7Bd%7D_i%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='N = 1 + \sum_{i=0}^c (\overline{d}_i - \underline{d}_i)' title='N = 1 + \sum_{i=0}^c (\overline{d}_i - \underline{d}_i)' class='latex' /> since for each i, <img src='http://l.wordpress.com/latex.php?latex=d%5Ei&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='d^i' title='d^i' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=d%5E%7Bi%2B1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='d^{i+1}' title='d^{i+1}' class='latex' /> can only differ in exactly one spot, and this difference is 1. The dimension of <img src='http://l.wordpress.com/latex.php?latex=B_%7B%5B%5Cunderline%7Bd%7D%2C+%5Coverline%7Bd%7D%5D%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='B_{[\underline{d}, \overline{d}]}' title='B_{[\underline{d}, \overline{d}]}' class='latex' /> is <img src='http://l.wordpress.com/latex.php?latex=-c+%2B+%5Csum_%7Bi%3D0%7D%5Ec+%28%5Coverline%7Bd%7D_i+-+%5Cunderline%7Bd%7D_i+%2B+1%29+%3D+1+%2B+%5Csum_%7Bi%3D0%7D%5Ec+%28%5Coverline%7Bd%7D_i+-+%5Cunderline%7Bd%7D_i%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='-c + \sum_{i=0}^c (\overline{d}_i - \underline{d}_i + 1) = 1 + \sum_{i=0}^c (\overline{d}_i - \underline{d}_i)' title='-c + \sum_{i=0}^c (\overline{d}_i - \underline{d}_i + 1) = 1 + \sum_{i=0}^c (\overline{d}_i - \underline{d}_i)' class='latex' /> (the -c comes from the fact that there are c HK equations, and they are linearly independent). So we conclude that every maximal chain forms a basis for <img src='http://l.wordpress.com/latex.php?latex=B_%7B%5B%5Cunderline%7Bd%7D%2C+%5Coverline%7Bd%7D%5D%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='B_{[\underline{d}, \overline{d}]}' title='B_{[\underline{d}, \overline{d}]}' class='latex' />.</p>
<p>Not too interesting yet. We know only that every Betti table is a linear combination of pure Betti tables at this point. But now let&#8217;s restrict to positive linear combinations. In this case, each maximal chain forms a simplicial cone, and in fact any two such cones intersect in a facet of both, so we get a simplicial fan. So what we must do is 1) identify the exterior facets of this fan, 2) find the facet-defining equations, and 3) show that these equations are nonnegative on all Betti tables.</p>
<p>Step 1) was done by Boij and Söderberg, and 2) can be done (although since we are working in a proper subspace of a Euclidean space, these functionals will not be uniquely determined). The key insight of Eisenbud and Schreyer was to construct the functionals in 2) in terms of a bilinear pairing between minimal free resolutions and cochain complexes. Then the facet defining equations come from very special cochain complexes: the linear monads of &#8220;supernatural&#8221; vector bundles on projective space <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbf%7BP%7D_K%5E%7Bn-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbf{P}_K^{n-1}' title='\mathbf{P}_K^{n-1}' class='latex' />.</p>
<p>I&#8217;ll explain this last paragraph and discuss what to do next in the next installment: <a href="http://concretenonsense.wordpress.com/2009/04/02/boij–soderberg-theory-iii-proofs/">part III</a>.</p>
<p>-Steven</p>
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