Hopf Algebra

A hopf algebra A is a graded algebra A=\bigoplus_{n\geq 0}A_{n} over a commutative ring R so that there exists an identity 1\in A_{0} such that the map R\to A_{0} defined by r\mapsto r\cdot 1 is an isomorphism and there exists a homomorphism of graded algebra \Delta:A\to A\otimes A so that

\Delta (\alpha)=\alpha\otimes 1+1\otimes \alpha+\sum_{0<i<n}\alpha_{i}'\otimes \alpha_{n-i}''

for \alpha\in A_{n}, n>0 and \alpha_{j}',\alpha_{j}''\in A_{j}.

Let A=R[\alpha] be the polynomial ring over R. Then \Delta(\alpha)=\alpha\otimes 1+1\otimes \alpha. Assume that \alpha is odd dimensional. Then (\alpha \otimes 1)(1\otimes \alpha)=\alpha\otimes\alpha and (1\otimes\alpha)(\alpha\otimes 1)=-\alpha\otimes\alpha. This would implies that \Delta(\alpha)^{2}=\alpha^{2}\otimes 1+1\otimes\alpha^{2}=\Delta(\alpha^{2}).

Let \Lambda_{R}[\alpha] be the exterior algebra over R. Then \alpha^{2}=0. It is easy to see that \Delta(\alpha)^{2}=0.

An element \alpha in a Hopf algebra A is said to be primitive if \Delta\alpha=\alpha\otimes 1+1\otimes\alpha.

Exercise: Let A,B be hopf algebras over R. On A\otimes_{R} B, we define \Delta(a\otimes b)=\Delta(a)\otimes\Delta(b). Show that A\otimes_{R}B is again a hopf algebra.

Picard-Fuchs Equation

Let {M} be a smooth projective algebraic variety of dimension {n}. Given a holomorphic {n}-form {\omega} and {\gamma_{1},\cdots,\gamma_{r}} be a basis for {H_{n}(M)}. (We assume that the dimension of {H_{n}(M)} is {r}.) The periods of {\omega} associated with the basis {\{\gamma_{1},\cdots,\gamma_{r}\}} are the integrals:

\displaystyle  \int_{\gamma_{j}}\omega,\quad 1\leq j\leq r. \ \ \ \ \ (1)

Let us consider a family of {n}-dimensional projective algebraic varieties {\bar{\pi}:\bar{X}\rightarrow \bar{C}}, where {\bar{C}} is a compact Riemann surface. Assume that {C} is an open subset of {C} so that the induced family {\pi:X\rightarrow C} has smooth fibers. Let {\omega} be an {n}-form on a fiber {X_{0}} of {\pi} and {\{\gamma_{j}:1\leq j\leq r\}} be a basis for {H_{n}(X_{0})}. Assume that {\omega} can be extended to a family of {n}-forms {\{\omega(z)\}} with {\omega(z)\in X_{z}} for each {z} and {\{\gamma_{j}\}} can be extended to a family of basis {\{\gamma_{j}(z)\}} for {H_{n}(X_{z})}, where {z} is a local coordinates on {C}. Let {v(z)} be the vector whose components are periods of {\omega(z)} associated with the basis {\{\gamma_{j}(z)\}}:

\displaystyle  v(z)=\left[ \begin{array}{c} \int_{\gamma_{1}(z)}\omega(z) \\ \int_{\gamma_{2}(z)}\omega(z)\\ \vdots\\ \int_{\gamma_{r}(z)}\omega(z) \\ \end{array} \right]\in\mathbb{C}^{r}. \ \ \ \ \ (2)

Define

\displaystyle  v_{j}(z)=\frac{d^{j}}{dz^{j}}v(z) \ \ \ \ \ (3)

and denote

\displaystyle  d_{j}(z)=\mbox{span}\{v_{1}(z),\cdots,v_{j}(z)\}. \ \ \ \ \ (4)

Since {\mbox{span}\{v_{1}(z),\cdots,v_{j}(z)\}} is a vector subspace of {\mathbb{C}^{r}} for each {z}, {d_{j}(z)\leq r} for all {z} and for all {j}. Then there exists {s} so that

\displaystyle  v_{s}(z)\in \mbox{span}\{v_{1}(z),\cdots,v_{s-1}(z)\}. \ \ \ \ \ (5)

This shows that for each {z}, there exists {c_{j}(z)\in\mathbb{C}^{r}} so that

\displaystyle  v_{s}(z)=-\sum_{j=1}^{s-1}c_{j}(z)v_{j}(z). \ \ \ \ \ (6)

In other words, we obtain the following Picard-Fuchs equation:

\displaystyle  \frac{d^{s}}{dz^{s}}v(z)+\sum_{j=1}^{s-1}c_{j}(z)\frac{d^{j}}{dz^{j}}v(z)=0. \ \ \ \ \ (7)

Multiplying (7) by {z^{s}}, we obtain another equation:

\displaystyle  D^{s}v(z)+\sum_{j=1}^{s-1}b_{j}(z)D^{j}v(z)=0, \ \ \ \ \ (8)

where {D} is the differential operator {zd/dz}. Equation (8) is called the logarithmic form of the Picard-Fuchs equation.

Natural Representation of Fundamental groups on Cohomology Groups coming from Fibration

Let {X} be a space. A self homotopy equivalence is a map {f:X\rightarrow X} so that there is another map {g:X\rightarrow X} with the property that {f\circ g} and {g\circ f} are both homotopic to the identity map on {X}. Let {[f]} be the equivalent class of a self homotopy equivalence {f:X\rightarrow X}. The set of all homotopy equivalent classes forms a group. Let me denote this group by {G(X)}. Since a homotopy equivalence {f:X\rightarrow X} induces isomorphisms of {f^{*}:H^{n}(X)\rightarrow H^{n}(X)} cohomology of groups {H^{n}(X)} for each {n} with coefficient in any group {A}, we obtain representations:

\displaystyle  G(X)\rightarrow \mbox{Aut}(H^{n}(X)) \ \ \ \ \ (1)

defined by {[f]\mapsto f^{*}}. Similarly, we have a representation of {G(X)} in {H_{n}(X)} defined by {[f]\mapsto f_{*}}.

A fibration is a continuous map {p:E\rightarrow B} so that it has the homotopy lifting propery. Let {p:E\rightarrow B} be a fibration. Then all fibers {E_{b}} are homotopy equivalent. Every path {\alpha:[0,1]\rightarrow B} defines a homotopy class {\alpha_{*}} of homotopy equivalences {E_{\alpha(0)}\rightarrow E_{\alpha(1)}} which depends only on the homotopy class of {\alpha} rel to endpoints. Therefore every element in {\pi_{1}(B,b_{0})} defines a homotopy class of self homotopy equivalence of {E_{b_{0}}}. Thus we have a group homomorphism:

\displaystyle  \pi_{1}(B,b_{0})\rightarrow G(B) \ \ \ \ \ (2)

defined by {\alpha\mapsto \alpha_{*}}. Thus we obtain a representation of {\pi_{1}(B,b_{0})} on {H^{n}(B)}:

\displaystyle  \pi_{1}(B,b_{0})\rightarrow H^{n}(B). \ \ \ \ \ (3)

Similarly, we have a representation of {\pi_{1}(B,b_{0})} on {H_{n}(B)}.

A supplement note for Leray spectral sequence in Griffiths book: Local system

Let {\pi:E\rightarrow B} be a differentiable fiber bundle whose fiber {F} is a compact differentiable manifold. Choose an open set {U} in {B} diffeomorphic to {\mathbb{R}^{k}} to obtain a diffeomorphism {\pi^{-1}(U)\cong U\times F}. The cohomology of {\pi^{-1}(U)} can be computed by the K\”{u}nneth formula which states that

\displaystyle H^{k}(X\times Y,\mathbb{Q})=\bigoplus_{i+j=k}H^{i}(X,\mathbb{Q})\otimes H^{j}(Y,\mathbb{Q}), \ \ \ \ \ (1)

 

for any spaces {X} and {Y}. Then we have an isomorphism {H^{q}(\pi^{-1}(U),\mathbb{Q})\cong H^{q}(F,\mathbb{Q})}. This isomorphism suggests two definitions. The first suggestion gives us the definition of the higher direct image sheaf. It is very natural to consider the sheaf associated with the presheaf {U\mapsto H^{q}(\pi^{-1}(U),\mathbb{Q})}. In general, given a continuous map {f:X\rightarrow Y}, the {q}-th direct image sheaf {R^{q}f_{*}\mathcal{F}} over {Y} is the sheaf associated with the presheaf

\displaystyle U\mapsto H^{q}(f^{-1}(U),\mathcal{F}). \ \ \ \ \ (2)

The second suggestion is the notion of locally constant sheaves (or a local system).

Let {A} be an abelian group. On a space {X}, we define a presheaf {\mathcal{A}} by {U\mapsto \mathcal{A}(U)=A}. The sheaf {\mathcal{A}^{+}} associated with the presheaf {\mathcal{A}} is called a constant sheaf. A locally constant sheaf {\mathcal{F}} over a space {X} is a sheaf over {X} with the property that there exists an open cover {\{U_{i}\}} such that the restriction { \mathcal{F}|_{U_{i}}} are constant sheaves for all {i}.

By {H^{q}(\pi^{-1}(U),\mathbb{Q})\cong H^{q}(F,\mathbb{Q})}, it is very natural to think that the {q}-th direct image sheaf {R^{q}f_{*}\mathbb{Q}} is isomorphic to the constant sheaf given by {H^{q}(F,\mathbb{Q})} but this is not always true. It does depend on the fundamental group {\pi_{1}(B,x_{0})} and is a locally constant sheaf. Since {\pi:E\rightarrow B} is a fibration, by the homotopy lifting properties of fibrations, an element {\gamma\in \pi_{1}(B,x_{0})} gives a homotopy equivalence {\gamma_{*}} on the fiber {E_{x_{0}}} and thus determines an isomorphism on the cohomology group {H^{n}(E_{x_{0}},M)} (and also the homology group) for any {n} and for any abelian group {M}. From here, we obtain a representation of {\pi_{1}(B,x_{0})} on {H^{n}(E_{x_{0}},\mathbb{Q})}. Read

Suppose that {\rho:\pi_{1}(B,x_{0})\rightarrow \mbox{Aut}(V)} is a representation on a vector space {V} and {\widetilde{B}} is the universal covering space for {B}. The associated vector bundle {V_{\rho}=\widetilde{B}\times_{\pi_{1}}V} gives a locally constant sheaf {\mathcal{V}_{\rho}} on {B} whose sections over an open set {U} of {B} are those which lift to constant sections of {\widetilde{B}\times V}. We call {\mathcal{V}_{\rho}} the sheaf associated with the representation {\rho:\pi_{1}(B,x_{0})\rightarrow \mbox{Aut}(V)}. The direct image sheaf {R^{q}f_{*}\mathbb{Q}} is the locally constant sheaf associated with the representation of {\pi_{1}(B,x_{0})} on {H^{q}(F_{x_{0}},\mathbb{Q})}.

Witten’s conjecture: Kontsevich’s Theorem

1. Witten’s Conjecture: Kontevich’s Theorem

Let {\mathcal{M}_{g,n}} be the moduli space of smooth curves of genus {g} with {n}-marked points and {\bar{\mathcal{M}}_{g,n}} is its Deligne-Mumford compactification. A point in {\bar{\mathcal{M}}_{g,n}} is of the form {(C,x_{1},\cdots,x_{n})}, where {C} is a stable curve of genus {g} and {x_{i}} are smooth points on {C}. Let {\mathbb{L}_{i}} be the line bundle over {\bar{\mathcal{M}}_{g,n}} whose fiber over a point {(C,x_{1},\cdots,x_{n})} is the cotangent line {T_{x_{i}}^{*}C}. Denote the Chern class of the line bundle {\mathbb{L}_{i}} by {\psi_{i}=c_{1}(\mathbb{L}_{i})}. Introduce a sequence of variables {\{\tau_{i}:i\geq 0\}}. Define the intersection index:

\displaystyle  \langle \tau_{d_{1}}\cdots \tau_{d_{n}}\rangle = \int_{\bar{\mathcal{M}}_{g,n}}\psi_{1}^{d_{1}}\cdots \psi_{n}^{d_{n}}, \ \ \ \ \ (1)

where {d_{1},\cdots,d_{n}} are nonnegative integers. If {d_{1}+\cdots+d_{n}\neq 3g-3+n}, we set {\langle \tau_{d_{1}}\cdots \tau_{d_{n}}\rangle=0}. Then we obtain a linear functional:

\displaystyle  \langle\cdot\rangle:\mathbb{Q}[\tau_{0},\tau_{1},\cdots]\rightarrow\mathbb{Q}. \ \ \ \ \ (2)

Let {\{t_{j}:j\geq 0\}} be another sequence of variables. Define a formal power series {F} in the variable {\{t_{i}\}} by

\displaystyle  F(t_{0},t_{1},\cdots)=\langle\exp\left(\sum_{i=0}^{\infty}t_{i}\tau_{i}\right)\rangle. \ \ \ \ \ (3)

Witten states that the series {F} coincides with the partition function in the standard matrix model theory and obeys the K.D.V hierarchy. The first equation is the classical KdV equation:

\displaystyle  \frac{\partial U}{\partial t_{1}}=U\frac{\partial U}{\partial t_{0}}+\frac{1}{12}\frac{\partial^{3}U}{\partial t_{0}^{3}}, \ \ \ \ \ (4)

where {U=\partial^{2}F/\partial t_{0}^{2}}. In 1991, M. Kontevich proved the following theorem: The series {\exp(F)} in variables {T_{2i+1}=t_{i}/(2i+1)!!} is a {\tau}-function for the KdV hierarchy. It follows from this theorem that the Witten’s conjecture is true.

Calabi Conjecture( Yau’s Theorem): The path to Calabi-Yau manifolds

1. Calabi Conjecture: Yau’s Theorem

Let {M} be a compact complex manifold. A Hermitian metric {g=g_{i\bar{j}}dz^{i}\otimes d\bar{z}^{j}} on {M} is a K\”{a}hler metric if its associated {(1,1)}-form {\omega=g_{i\bar{j}}dz^{i}\wedge d\bar{z}^{j}} is closed, i.e. {d\omega=0}. Denote the Ricci tensor of {M} w.r.t the K\”{a}hler metric {g} by {R_{i\bar{j}}dz^{i}\otimes d\bar{z}^{j}}. Then its associated Ricci-form {\frac{\sqrt{-1}}{2\pi}R_{i\bar{j}}dz^{i}\wedge d\bar{z}^{j}} represents the first Chern class {c_{1}(M)}.

The Calabi conjecture states the followings. Let {\frac{\sqrt{-1}}{2\pi}\widetilde{R}_{i\bar{j}}dz^{i}\wedge d\bar{z}^{j}} representing {c_{1}(M)}. Can we find a K\”{a}hler metric {\widetilde{g}_{i\bar{j}}dz^{i}\otimes d\bar{z}^{j}} whose Ricci form is the above given {(1,1)}-form? Suppose that it is true. We need to find a smooth function {\varphi} on {M} so that

\displaystyle  \left[g_{i\bar{j}}+\frac{\partial^{2}\varphi}{\partial z^{i}\partial\bar{z}^{j}}\right]dz^{i}\otimes d\bar{z}^{j} \ \ \ \ \ (1)

is a K\”{a}hler metric whose Ricci form is given above. Therefore by simple computation,

\displaystyle  \frac{\sqrt{-1}}{2\pi}\widetilde{R}_{i\bar{j}}dz^{i}\wedge d\bar{z}^{j}=-\frac{\sqrt{-1}}{2\pi}\partial\bar{\partial}\log \det\left[g_{i\bar{j}}+\frac{\partial^{2}\varphi}{\partial z^{i}\partial\bar{z}^{j}}\right]. \ \ \ \ \ (2)

Since the {(1,1)}-form {\frac{\sqrt{-1}}{2\pi}\widetilde{R}_{i\bar{j}}dz^{i}\wedge d\bar{z}^{j}} is cohomologous to {\frac{\sqrt{-1}}{2\pi}R_{i\bar{j}}dz^{i}\wedge d\bar{z}^{j}}, there exists a smooth function {F} so that

\displaystyle  -\frac{\sqrt{-1}}{2\pi}\partial\bar{\partial}\log \det\left[g_{i\bar{j}}+\frac{\partial^{2}\varphi}{\partial z^{i}\partial\bar{z}^{j}}\right]+\frac{\sqrt{-1}}{2\pi}\partial\bar{\partial}\log \det g_{i\bar{j}}=\frac{\sqrt{-1}}{2\pi}\partial\bar{\partial}F \ \ \ \ \ (3)

which is equivalent to the following equation

\displaystyle  \det\left[g_{i\bar{j}}+\frac{\partial^{2}\varphi}{\partial z^{i}\partial\bar{z}^{j}}\right]\det (g_{ij}^{-1})=\exp (F). \ \ \ \ \ (4)

Here we require that {\int_{M}\exp(F)=\mbox{vol}_{g}(M)}. To solve the Calabi conjecture is equivalent to solve (4). We study a more general partial differential equation:

\displaystyle  \det\left[g_{i\bar{j}}+\frac{\partial^{2}\varphi}{\partial z^{i}\partial\bar{z}^{j}}\right]\det (g_{ij}^{-1})=\exp (c\varphi+F). \ \ \ \ \ (5)

Here {c} is a number. In 1977, Yau proved that if {c\geq 0}, (5) can be solved with a smooth {\varphi} on {M}. Hence any {(1,1)}-form on {M} representing {c_{1}(M)} can be realized as the Ricci-form of a unique K\”{a}hler metric. The uniqueness of such a K\”{a}hler metric was proved by Calabi in 1954. The Calabi conjecture leads to the definition of Calabi-Yau manifold. A Calabi-Yau manifold is a compact K\”{a}hler manifold whose {c_{1}(M)=0}. By the Yau’s theorem, a Calabi-Yau manifold is a compact Ricci flat K\”{a}hler manifold.

Definition of Singular Homology

1. Singular Homology

1.1. Definition of a Singular Homological Module

Let {X} be a topological space. A singular {n}-simplexes {\sigma} is a continuous map {\sigma:\Delta_{n}\rightarrow X}. Here the standard {n}-dimensional simplex {\Delta_{n}} is the set of points in {\mathbb{R}^{n+1}}:

\displaystyle  \Delta_{n}=\{(t_{0},t_{1},\cdots,t_{n})\in\mathbb{ R}^{n+1}:\sum_{i=1}^{n}t_{n}=1,\ t_{i}\geq 0,\quad t\geq 0\}. \ \ \ \ \ (1)

Given a ring {R}, the free {R}-module generated by the set of all singular {n}-simplexes is denoted by {C_{n}(X,R)}. Elements of {C_{n}(X,R)} called the {n}-chains are of the form:

\displaystyle  c=\sum_{k=1}^{m}n_{k}\sigma_{k}, \ \ \ \ \ (2)

where {n_{k}\in R} and {\sigma_{k}:\Delta_{n}\rightarrow X} are singular {n}-simplex on {X}. For convenience, let us denote the {R}-module {C_{n}(X,R)} by {C_{n}(X)}. For {n<0}, we define {C_{n}(X)=\{0\}}. For any {n>0}, define so-called the face maps

\displaystyle  F_{n}^{i}:\Delta_{n-1}\rightarrow\Delta_{n} \ \ \ \ \ (3)

by {F_{n}^{i}(s_{0},s_{1},\cdots,s_{n-1})=(s_{0},\cdots,s_{i-1},0,s_{i},\cdots,s_{n})}. We leave to the reader to check that the equations {F_{n}^{i}F_{n-1}^{j}=F_{n}^{j}F_{n-1}^{i-1}} for {j<i}.

Given an {n}-simplex {\sigma} in {X}, the {i}-th face {\sigma^{(i)}} of {\sigma} is defined to be the singular {n-1} simplex {\sigma\circ F_{n}^{i}:\Delta_{n-1}\rightarrow X}. The boundary {\partial_{n}} of {\sigma} is defined to be the {n-1} chain:

\displaystyle  \partial_{n}\sigma=\sum_{i=0}^{n}(-1)^{i}\sigma^{(i)} \ \ \ \ \ (4)

Extend {\partial_{n}} to a module homomorphism from {C_{n}(X)} into {C_{n-1}(X)} by defining

\displaystyle  \partial\left(\sum_{j=1}^{k}r_{j}\sigma_{j}\right)=\sum_{j=1}^{k}r_{j}\partial\sigma_{j} \ \ \ \ \ (5)

for any {n}-chain {\sum_{j=1}^{k}r_{j}\sigma_{j}} in {C_{n}(X)}. It is also your job to check

\displaystyle  \partial_{n-1}\circ\partial_{n}=0,\quad n\geq 1. \ \ \ \ \ (6)

For {n<0}, we set {\partial_{n}=0}. Thus we obtain a chain complex

\displaystyle  C_{*}(X)=(C_{n}(X),\partial_{n})_{n\in\mathbb{Z}}. \ \ \ \ \ (7)

The homology {H_{*}(C_{*}(X))} defined by the chain complex is called the singular homology of {X}. We also denote {H_{*}(C_{*}(X))} by {H_{*}(X)} for short.

A singular {n}-chain {c} is called a cycle if {\partial_{n} c=0} and if {c=\partial c'} for some {n+1}-chain {c'}, {c} is called a boundary. Two {n}-chains {c_{1}} and {c_{2}} are called homologous if they are differed by an {n+1} boundary, i.e. there exists an {n+1} chain {c'} so that

\displaystyle  c_{1}-c_{2}=\partial_{n+1}c'. \ \ \ \ \ (8)

By (6), the boundaries form a submodule {B_{n}(X)=\mbox{Im} \partial_{n+1}} of the module {Z_{n}(X)=\ker\partial_{n}} of cycles. The quotient module {Z_{n}(X)/B_{n}(X)} is called the {n}-th singular homology module of {X}, denoted by {H_{n}(X,R)} or simply {H_{n}(X)}. An element of {H_{n}(X)} is denoted by {[c]} and called a homology class. Two representatives in the same homology class are homologous. By definition, the homology of the complex {C_{*}(X)} is the direct sum of homological module

\displaystyle  H_{*}(C_{*}(X))=\bigoplus_{n\in\mathbb{Z}}H_{n}(X). \ \ \ \ \ (9)

Here we set {H_{n}(X)=0} if {n<0}. For the singular homology module, we only need to compute {H_{n}(X)} for {n\geq 0}.

Let us now consider the case when {X} consists of one point. Then all maps from {\Delta_{n}} to {X} is continuous and there is only one map from {\Delta_{n}} to {X} for each {n}. Let {\sigma_{n}} be the unique map from {\Delta_{n}} to {X}. Then {S_{n}(X)} is the cyclic {R}-module {R\sigma_{n}} generated by {\sigma_{n}}. Then by definition

\displaystyle  H_{0}(X)=C_{0}(X)=R\sigma_{0}\cong R. \ \ \ \ \ (10)

We can compute the boundary of {\sigma_{n}}: {\partial_{n}\sigma_{n}=0} when {n} is odd and {\partial_{n}\sigma_{n}=\sigma_{n-1}} when {n} is even. Hence we find {Z_{2m+1}(X)=C_{2m+1}(X)} and {B_{2m+1}(X)=\mbox{Im}\partial_{2m+2}=C_{2m+1}(X)}; {Z_{2m}(X)=0} and {B_{2m}(X)=\mbox{Im} \partial_{2m+1}=0}. We conclude that {H_{n}(X)=0} for all {n\geq 1}.

Hochschild Homology

1. Hochschild Homology

Assume that {k} is a commutative ring and {A} is an associative {k}-algebra. Define an {A}-module by setting

\displaystyle \notag C_{n}(A,M)=M\otimes_{k}A^{\otimes n} \ \ \ \ \ (1)

and some operators {d_{i}:C_{n}(A,M)\rightarrow C_{n-1}(A,M)} as follows. Define

\displaystyle  d_{0}(m\otimes a_{1}\otimes\cdots\otimes a_{n})=ma_{1}\otimes a_{2}\otimes\cdots\otimes a_{n} \ \ \ \ \ (2)

and

\displaystyle  d_{i}(m\otimes a_{1}\otimes\cdots\otimes a_{n})=m\otimes a_{1}\otimes\cdots\otimes a_{i}a_{i+1}\otimes\cdots\otimes a_{n},\quad 1\leq i\leq n-1 \ \ \ \ \ (3)

and

\displaystyle  d_{n}(m\otimes a_{1}\otimes \cdots \otimes a_{n})=a_{m}m\otimes a_{1}\otimes\cdots\otimes a_{n-1}. \ \ \ \ \ (4)

When {i<j}, one can check that {d_{i}d_{j}=d_{j-1}d_{i}}. We define a linear operator

\displaystyle  b=\sum_{i=0}^{n}(-1)^{i}d_{i} \ \ \ \ \ (5)

and an { A}-module

\displaystyle  C_{*}(A,M)=\bigoplus_{n\geq 0}C_{n}(A,M). \ \ \ \ \ (6)

It is not hard to verify that {b:C_{*}(A,M)\rightarrow C_{*}(A,M)} is a differential. The differential complex {(C_{*}(A,M),b)} is called a Hochschild complex. The homology theory defined by a Hochschild complex is denoted by {H_{*}(A,M)} and called a Hochschild homology. If {M=A}, the Hochschild homology is also denoted by {HH_{*}(A)}.

Atiyah Singer Index Theory

Sir Michael Atiyah

I.Singer

1. The index of elliptic operators on compact manifolds

Let {X} be a compact oriented Riemannian manifold. Denote {\pi:S(X)\rightarrow X} the unit sphere bundle in {T^{*}X} over {X}. Given a linear differential operator {D:\Gamma(E)\rightarrow\Gamma(F)} on the vector bundles {E} and {F} over {X}, there is an induced bundle map {\sigma(D):\pi^{*}E\rightarrow \pi^{*}F} associated with {D}. The differential operator {D} is elliptic if {\sigma(D)} is a linear isomorphism. If {D} is an elliptic operator, {\ker D} and {\mbox{coker} D} are both finite dimensional. It is reasonable to define the index of {D} by

\displaystyle  \gamma(D)=\dim\ker D-\dim\mbox{coker} D. \ \ \ \ \ (1)

Here comes a problem:“Can we express {\gamma(D)} in terms of {\sigma(D)}?”

Let {E} and {F} be vector bundles over a space {Y} and {\sigma:Y_{0}\rightarrow Y_{0}} be an isomorphism on the subspace {Y_{0}} of {Y}. There is a difference element

\displaystyle  d(E,F,\sigma)\in K(Y/Y_{0}). \ \ \ \ \ (2)

Denote {p:B(X)\rightarrow X} the unit ball bundle in {T^{*}X} over {X}. If {D} is a elliptic operator, {\sigma(D):S(X)\rightarrow S(X)} is an isomorphism. Hence we obtain an element

\displaystyle  d(p^{*}E,p^{*}F,\sigma(D))\in K(B(X)/S(X)). \ \ \ \ \ (3)

Using the ring homomorphism {\mbox{ch}:K(Z)\rightarrow H^{*}(Z,\mathbb{Q})} for any space {Z}, we obtain an element in the cohomology of {B(X)/S(X)}:

\displaystyle  \mbox{ch} (d(p^{*}E,p^{*}F,\sigma(D)))\in H^{*}(B(X)/S(X),\mathbb{Q}). \ \ \ \ \ (4)

Using the Thom isomorphism:

\displaystyle  \phi_{*}:H^{k}(X,\mathbb{Q})\rightarrow H^{n+k}(B(X)/S(X),\mathbb{Q}), \ \ \ \ \ (5)

we obtain

\displaystyle  \phi_{*}^{-1}\mbox{ch}(d(p^{*}E,p^{*}F,\sigma(D)))\in H^{*}(X,\mathbb{Q}). \ \ \ \ \ (6)

Define the Chern character of {D} (or of {\sigma(D)}) by

\displaystyle  \mbox{ch}(D)=\phi_{*}^{-1}\mbox{ch}(d(p^{*}E,p^{*}F,\sigma(D))). \ \ \ \ \ (7)

Given a complex vector bundle {\xi} over {X}, we define

\displaystyle  \mbox{Td}(\xi)=\prod_{i=1}^{n}\frac{x_{i}}{1-e^{-x_{i}}}, \ \ \ \ \ (8)

where {x_{i}} are Chern roots of the bundle {\xi}. If {\eta} is a real vector bundle over {X}, we define

\displaystyle  \mbox{Td}(\eta)=\mbox{Td}(\eta\otimes_{\mathbb{R}}\mathbb{C}). \ \ \ \ \ (9)

We also denote {\mbox{Td}(TX)} by {\mbox{Td}(X)}.

Let {[X]} be the fundamental class of {X} in {H_{n}(X,\mathbb{Q})}. For any {\alpha\in H^{*}(X,\mathbb{Q})}, we denote {\alpha[X]} the value of {\alpha} at {[X]}.

Let {D:\Gamma(E)\rightarrow\Gamma(F)} be an elliptic differential operator on {X}. Then

\displaystyle \gamma(D)=\{\mbox{ch}(D)\cdot \mbox{Td}(X)\}[X].

Test

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