M721: Index Theory

Ruminations of a Graduate Class

Examples of Atiyah-Singer Index Theorem

leave a comment »

Let’s begin with some notations.

Let D:C^\infty (E) \rightarrow C^\infty (F) be an elliptic differential operator, where E and F are vector bundles over a closed oriented manifold X^n. Suppose E, F and TX have smooth inner product structures. Let D(X):=D(T^*X) and S(X):=S(T^*X) be the disk and sphere bundle of the cotangent bundle, respectively. Let \pi: D(X)\rightarrow X be the projection. Let [\sigma_D]=[\pi^*E, \pi^*F; \sigma_D]\in K(D(X),S(X)) be the associated symbol class. Let \textrm{ch} ([\sigma_D])\in H^{2*}(D(X),S(X);\Bbb{Q}) be its Chern character. Let \textrm{td} (X) denote the pullback of the Todd class \pi^*\textrm{td} (T^*X\otimes \Bbb{C})\in H^{2*}(D(X);\Bbb{Q}). Let [D(X)]\in H_{2n}(D(X),S(X)) be the fundamental class.

Definition.  The topological index of D is defined to be \textrm{t-ind} \ D:=(-1)^n\langle \textrm{ch}[\sigma_D]\textrm{td} (X),[D(X)]\rangle.

Atiyah-Singer Index Theorem.  \textrm{ind} \ D=\textrm{t-ind} \ D, where \textrm{ind} \ D:=\textrm{dim}_{\Bbb{C}}(\textrm{ker} D)-\textrm{dim}_{\Bbb{C}}(\textrm{cok} \ D) is the analytical index.

Example. [Point Case] Let X be a point. Then E and F are finite dimensional vector spaces. Any non-trivial differential operator D is a linear map between them, and hence of order 0. Thus, \sigma_D=D. Note that D(X)=X, S(X) is empty set. Recall the definition of Chern character, then we have \textrm{ch} (E)=\textrm{dim} E and \textrm{ch} (F)=\textrm{dim} F. Since S(X) is empty set, then [\sigma _D]=[E]-[F] and hence \textrm{ch} ([\sigma _D])=\textrm{dim} E-\textrm{dim} F. Recall the definition of Todd class, we then have \textrm{td} (X)=1. Therefore, by the definition of topological index, we have \textrm{t-ind} \ D=\textrm{dim} E-\textrm{dim} F. By Atiyah-Singer, \textrm{dim} (\textrm{ker} D)-\textrm{dim} (\textrm{cok} \ D)=\textrm{dim} E-\textrm{dim} F.

Example [S^1 Case] Let X=S^1=\Bbb{R}/2\pi\Bbb{Z}, E=F=S^1\times\Bbb{C}, D=\frac{d}{dx}: C^\infty(S^1,\Bbb{C})\rightarrow C^\infty(S^1,\Bbb{C}). Then D is a first order elliptic operator. We now claim that \textrm{ind} \ D=0. We give four different proofs.
Proof 1. We compute \textrm{ind} \ D directly. Note that \textrm{ker} \frac{d}{dx}=\{constant functions\} and that \textrm{cok} \ \frac{d}{dx}\xrightarrow{\approx}\Bbb{C} via [f]\mapsto\int_{S^1}f.
Proof 2. Since E=F, we have [\sigma_D]=[\pi^*E,\pi^*F;\sigma_D]=[\pi^*E\cup_{\sigma_D}\pi^*F]-[\pi^*F\cup_{\textrm{id}}\pi^*F]=[\pi^*F\cup_{\textrm{id}}\pi^*F]-[\pi^*F\cup_{\textrm{id}}\pi^*F]=0.
Proof 3. \textrm{ind} \ \frac{d}{dx}=\textrm{ind} \ i\frac{d}{dx}=0, since i\frac{d}{dx} is self-adjoint.
Proof 4. We will show that the topological index vanishes whenever n is odd. See next example.

Example [Odd Dimensional Case, Theorem 13.12 in Lawson-Michaelson]
We will show that the topological index of any elliptic differential operator vanishes whenever n is odd.

We want to show that \textrm{t-ind} \ D =-\textrm{t-ind} \ D, where D is an elliptic differential operator of order m. Consider the diffeomorphic involution c: TX\rightarrow TX given by c(v)=-v. Since
\textrm{t-ind}\ D=-\textrm{ch} ([\sigma_D])\textrm{td} (X)[D(X)]

\ \ \ \ \ \ \ \ \ \ \ \ =-\textrm{ch} ([\sigma_D])\textrm{td} (X)c_*c_*[D(X)]

=-c^*(\textrm{ch} ([\sigma_D])\textrm{td} (X)) c_*[D(X)]

=-(\textrm{ch} (c^*[\sigma_D]))\textrm{td} (X) (-[D(X)]),
it suffices to show c^*[\sigma_D]=[\sigma_D]. In fact, c^*[\sigma_D]=[\pi^*E,\pi^* F;(-1)^m\sigma_D]=[\pi^*E,\pi^* F;\sigma_D]=[\sigma_D], since \sigma_D is homotopic to -\sigma_D via e^{i\pi t}D, t\in [0,1].
Next, we need to introduce the Thom Isomorphism to talk about the de Rham operator.

Let E be an oriented \Bbb{R}^k-vector bundle over X, with inner product on each fiber. We now give the notion of Thom class and Thom space.

Definition. u(E)\in H^k(D(E)),S(E)) is a Thom Class of E if it restricts to a generator of H^k(D^k,S^{k-1})\approx H^k(\pi^{-1}\{x\}\cap D(E),\pi^{-1}\{x\}\cap S(E)) on each fiber. The quotient D(E)/S(E) is called the Thom space of E, and denoted by \textrm{Th} (E).

Thom Isomorphism Theorem. The composition H^*(X)\xrightarrow{\approx}H^*(D(E))\xrightarrow{\smallsmile u}H^{*+k}(D(E),S(E)) is an isomorphism.

We denote the composition by \textrm{-}\smallsmile u : H^*(X)\xrightarrow{\approx}H^{*+k}(D(E),S(E))=\widetilde{H}^{*+k}(\textrm{Th}(E)) and denote its inverse by \pi_!.

Remark.  \pi_! has the following two other interpretations.

(1). Integration over the fiber. \pi_! : \Omega^{i+k}(E)\rightarrow\Omega^i(X), where E is a \Bbb{R}^k bundle over X.
Let \tau\in\Omega^{i+k}(E) be given and choose x\in X and v_1,...,v_i\in T_xX. Associated to these data is a form \tau^{x,v_1,...,v_i}\in\Omega^k(E_x), defined as follows. Given e\in E_x and a basis e_1,...,e_k\in T_e E_x, choose lifts \widetilde{v_l}\in T_e E_x such that d\pi (e)\widetilde{v_l}=v_l, for each l\leq i, and define

(\tau^{x,v_1,...,v_i})_e(e_1,...,e_k):=\tau_e(\widetilde{v_1},...,\widetilde{v_i},e_1,...,e_k). Now \pi_! \tau\in\Omega^k(X) is defined by


Integrating over the fibers will give the second formulation of the topological index, which is the next theorem. The factor (-1)^{\frac{n(n+1)}{2}} compensates for the difference between the orientation on TX induced by the one on X, and the canonical orientation on TX inherited from its almost complex structure.

(2) . Also, we can use the second interpretation of \pi_! to give that formulation.

\pi_! is the composition (Poincare duality) \ \circ\ \pi_*\ \circ (Poincare-Lefschetz duality),

H^{*+k}(D(E),S(E))\rightarrow H_{n-*}(D(E))\xrightarrow{\pi_*} H_{n-*}(X)\rightarrow H^*(X).
Then, we compute
\textrm{t-ind}\ D=(-1)^n \textrm{ch}[\sigma_D]\textrm{td} (X)[D(X)]
=(-1)^{\frac{n(n+1)}{2}}\textrm{td} (X) \pi_*(\textrm{ch} ([\sigma_D])\smallfrown [D(X)])
= (-1)^{\frac{n(n+1)}{2}}\textrm{td} (X) \pi_!(\textrm{ch} ([\sigma_D])\smallfrown [X])
= (-1)^{\frac{n(n+1)}{2}}\pi_!( \textrm{ch} ([\sigma_D]))\textrm{td} (X)\ [X].

Theorem.  \textrm{t-ind} \ D=(-1)^{\frac{n(n+1)}{2}}\pi_!( \textrm{ch} ([\sigma_D]))\textrm{td} (X)\ [X].

We will then give the third formulation of the topological index. To do this we need the notion of Euler class.

Definition. The Euler class of an oriented \Bbb{R}^k-bundle over X, denoted by $latexe(E)$, is the image of the Thom class u under the following isomorphism: H^k(D(E),S(E))\xrightarrow{i^*}H^k(D(E))\xrightarrow{\approx}H^k(X). We may denote the composition by i^*.

Theorem. [Gysin Sequence]  To any bundle E as above there is associated an exact sequence of the form \cdots\rightarrow H^i(X)\xrightarrow{\smallsmile e(E)} H^{i+k}(X)\xrightarrow{\pi^*} H^{i+k}(S(E))\rightarrow H^{i+1}(X)\xrightarrow{\smallsmile e}\cdots.

Definition. The Euler characteristic of X is defined to be \chi (X):=\langle e(TX),[X]\rangle.


From now on, we assume n=2m.

We want to analyze \pi_!\textrm{ch}([\sigma_D]) to give the third formulation of the topological index. For details please see Lawson-Michaelson, P258, Theorem 13.13.

Since –\smallsmile u and \pi_! are inverse to each other, we have (\pi_!\textrm{ch}([\sigma_D]))\smallsmile u(TX)=\textrm{ch}([\sigma_D]). Applying i^* to both sides, we then get (\pi_!\textrm{ch}([\sigma_D]))\smallsmile e(TX)=i^*\textrm{ch}([\sigma_D])=\textrm{ch} (i^*\sigma_D])=\textrm{ch}(E)-\textrm{ch}(F). Thus we can write \pi_!\textrm{ch}([\sigma_D])=\frac{\textrm{ch}(E)-\textrm{ch}(F)}{e(TX)}, if e(TX)\neq 0.

Theorem. \textrm{t-ind} \ D=(-1)^{\frac{n(n+1)}{2}}\frac{\textrm{ch}(E)-\textrm{ch}(F)}{e(TX)}\textrm{td} (X)\ [X], if e(TX) is not zero.

Now, we are trying to apply this formula to the de Rham operator.

Example. [de Rham operator]  Let \Omega^k_\Bbb{C}=C^\infty(\Lambda^k\ T^*X\otimes \Bbb{C}). Then we already know that (\Omega_\Bbb{C}^\bullet, d) is an elliptic complex, that d: \Omega_\Bbb{C}^{even}\rightarrow\Omega_\Bbb{C}^{odd} is an elliptic operator and that \textrm{ind} \ d=\Sigma(-1)^i\ \textrm{rk}(H^i_{DR}(X)). We want to use the above theorem to show that \textrm{t-ind}\ d=\Sigma (-1)^i \ \textrm{rk}( H^i(X)), the Euler charateristic.

For a complex vector bundle E, by the splitting principle, we can write E as \oplus_i L_i. Then \Sigma_0^n \Lambda^i E=\otimes_1^n\Lambda L_i=\otimes_1^n (\Bbb{C}\oplus L_i). It follows that \textrm{ch} (\Sigma_0^n \Lambda^i E)=\prod_1^n (1+e^{x_i}). Similarly, we have \textrm{ch} (\Sigma_0^n (-1)^i\Lambda^i E)=\prod_1^n (1-e^{x_i}).

Back to our example, applying the real splitting principle to T^*X, we compute

\textrm{ch} (\Sigma (-1)^i \Lambda^i T^*X\otimes\Bbb{C})=\prod_1^n (1-e^{x_i})=\prod_1^n (1-e^{-x_i}),

since x_i=-x_{i+m} for 1\leq i\leq m. Note that \textrm{td} (X)=\prod_1^n \frac{x_i}{1-e^{-x_i}}, and that e=\prod_1^m x_i, then by the theorem above, we obtain

\textrm{t-ind} \ d=(-1)^{\frac{n(n+1)}{2}}\frac{\prod_1^n (1-e^{-x_i})}{\prod_1^m x_i}\prod_1^n \frac{x_i}{1-e^{-x_i}} [X]=(-1)=\prod_1^m x_i [X]=\chi (X).


Written by topoclyb

January 13, 2013 at 7:37 pm

Posted in Uncategorized

The index theorem for the signature and Dirac operators

leave a comment »

This post will be converted into WordPress later. In the meantime, view it in PDF form here: DiracIndexTheory

Written by Henry T. Horton

December 15, 2012 at 3:43 pm

Posted in Uncategorized

The Dirac operator

with one comment

We begin by endowing a vector bundle with a Clifford module structure. It is with additional structure that we may define a Dirac operator.

Let (X^n, g) be an n-dimensional Riemannian manifold with covariant derivative \nabla^X (on TX) , and let \mathbb{R}^N\to S\to X be a vector bundle.

Clifford Module Bundles and a Dirac “Type” Operator

Definition (Clifford module)

A Clifford module T for a real inner product space (V,\beta) is a left module over Cl(V,\beta). Equivalently, there is a -algebra homomorphism c: Cl(V,\beta) \to \text{Hom(T,T)} given by c(v) = (t\mapsto v\cdot t). Since v^2:=v\cdot v = -||v||^2 for any v\in Cl(V,\beta) (see the Glossary below), one has that c satisfies c(v)^2 = - ||v||^2\text{Id}.

Definition (Bundle of Clifford Modules)

A bundle S (as above) is a bundle of Clifford modules if there is a map of bundles of \mathbb{R}-algebras C:Cl(TX)\to \text{Hom}(S,S) such that c(v)^2s = -||v||^2 s for any section s\in C^{\infty}(S). In other words, for each x\in X, \text{Hom}(S_x, S_x) is a Clifford module for (T_x X, g_x).

Definition (Dirac type operator)

Let S be a Clifford module bundle equipped with a covariant derivative \nabla^S. Let D:C^\infty(S)\to C^\infty(S) be the map defined by the composition

C^\infty(S)=\Omega^0(S) \xrightarrow{\nabla^S} \Omega^1(S) = C^\infty(\text{Hom}(TX,S)) \xrightarrow{H} C^\infty(TX\otimes S)\xrightarrow{c} \Omega^0(S)

where H is the inverse of the bundle isomorphism C^\infty(TX\otimes S) \to C^\infty(\text{Hom}(TX,S)), v\otimes s \mapsto g(v,.)\otimes s, and where c(v\otimes s) = v\cdot s is Clifford multiplication. We call such a map (which depends on the Clifford module bundle S, \nabla^S and g) a Dirac type operator.

If we a fix an orthonormal frame \{e_1,\ldots, e_n\} for TX over some neighborhood U\subset X and, using the metric g, let \{e^i\} be the corresponding frame for T^\ast X|_U, we may write this composition locally as

s\overset{\nabla^S}{\mapsto} \sum_{i=1}^n e^i\otimes \nabla^S_{e_i} s \overset{H}{\mapsto} \sum_{i=1}^n e_i\otimes \nabla^S_{e_i} s \overset{c}{\mapsto} \sum_{i=1}^n e_i\cdot \nabla^S_{e_i} s

That is, a Dirac type operator is locally of the form

Ds = \sum_{i=1}^n e_i\cdot \nabla^S_{e_i} s.


A Dirac type operator is a first order differential operator.


Let s\in C^\infty(S) and f\in C^{\infty}(X). Using the local description above, we compute:

[D, f]s = D(fs) - f(Ds)

= \sum_{i=1}^n \bigl[ e_i\cdot \nabla^S_{e_i} (fs) - f e_i\cdot \nabla^S_{e_i} s\bigr]

= \sum_{i=1}^n \bigl[ e_i\cdot (e_i(f)s + f \nabla^S_{e_i} s) - f  e_i\cdot \nabla^S_{e_i} s\bigr]

= \sum_{i=1}^n \bigl[ e_i\cdot e_i(f)s +  e_i\cdot f \nabla^S_{e_i} s - f  e_i\cdot \nabla^S_{e_i} s \bigr]

= \sum_{i=1}^n \bigl[ e_i\cdot e_i(f)s + f e_i\cdot \nabla^S_{e_i} s - f  e_i\cdot \nabla^S_{e_i} s \bigr]

= \sum_{i=1}^n e_i\cdot e_i(f)s.

In particular, [D,f](gs) = g[D,f](s) for g\in C^{\infty}(X), so [D,f] is C^\infty(X)-linear and hence in DO_0(S,S). Thus D\in DO_1(S,S), and as D itself is not C^\infty(X)-linear, D is of order 1. \square


The above proof extends (by incorporating induction) to show that the composition of a k– and an m- order differential operator is a differential operator of order \leq k+m. Here, \nabla^S and c are differential operators of order 1 and 0, respectively.

We next show that D is elliptic.

Lemma (Symbol of a Dirac type operator)

Let D be a Dirac type operator and let \xi^\ast\in T^\ast X. Then the symbol \sigma_D(\xi^\ast) of D at \xi^\ast is given by

\sigma_D(\xi^\ast)(s) = \frac{1}{i} \xi\cdot s,

where \xi\in TX is the dual to \xi^\ast determined by the metric, i.e., such that \xi^\ast = g(\xi, \cdot).


Fix x\in X, and let U be an open neighborhood of x in X. Using g choose an orthonormal frame \{e_i\} of TX|_U with dual frame \{e^i\} for T^\ast X|_U. Being a bundle homomorphism \pi^\ast(S)\to \pi^\ast(S) (over \mathbb{R}), \sigma_D is \mathbb{R}-linear in the T^\ast X-ordinate. Thus it suffices to verify the proposition for e^j; that is, we wish to show that \sigma_D(e^j)(s) = \frac{1}{i} e_j\cdot s for s\in C^{\infty}(S|_U).

Choose a local chart \varphi: U\to \mathbb{R}^n such that \varphi(x)=0; let x_i=\text{pr}_i\circ \varphi: U\to \mathbb{R}. Note that \{e_i(x)\} is an orthonormal basis for T_xX. Let \frac{\partial}{\partial x_i} = d\varphi_x(e_i(x)); then {dx_j}_x(e_i(x)) = {d\text{pr}_j}|_0\circ d\varphi_x(e_i(x)) =  {d\text{pr}_j}|_0\bigl(\frac{\partial}{\partial x_i}\bigr) = \delta_{ji}, so {dx_j}_x = e^j(x).

Thus (see the Glossary below), as D is order 1, we have

\sigma_D(e^j)(s(x)) = \frac{1}{i} D(x_j s)(x)

= \frac{1}{i} (\sum_{i=1}^n e_i\cdot \nabla_{e_i}(x_j s))(x)

= \frac{1}{i} \sum_{i=1}^n e_i(x) \cdot \bigl[ {dx_j}_x(e_i(x)) s(x) + \underbrace{x_j(x)}_{=0}\nabla_{e_i}s(x)\bigr]

= \frac{1}{i} \sum_{i=1}^n e_i(x) \cdot \bigl[ \delta_{ji} s(x) + 0]

= \frac{1}{i} e_j(x)\cdot s(x),

as required. \square


A Dirac type operator is elliptic.


If \xi^\ast\in TX^\ast-X then \sigma_D(\xi^\ast) has inverse \sigma_D^{-1}(\xi^\ast)(s) = i \frac{1}{\xi^\ast} \cdot s . \square


Noting that \sigma_{D^2}(\xi) = \sigma_D(\xi)\sigma_D(\xi) (the product of linear maps), we observe that \sigma_{D^2}(\xi)s = -\xi\cdot \xi \cdot s = ||\xi||^2 s. Taking S=Cl(TX), this — apparently — implies that a Dirac type operator is, at the symbol level, the square root of the Laplacian.

\mathbb{Z}_2-grading and “a” Dirac Operator

A Dirac type operator is formally self-adjoint (so that its index is 0) if we impose the following further restrictions on the Clifford-module bundle.

Definition (Clifford-Compatible)

Let S\to X be a bundle of Clifford modules. We say that S is Clifford compatible if it is equipped with a metric \langle, \rangle and a covariant derivative \nabla^S such that

(1) \nabla^S is Riemannian, i.e., for all sections s, t\in C^\infty(S):

d\langle s, t\rangle = \langle \nabla^S s, t\rangle + \langle s, \nabla^S t \rangle, and

(2) for all vector fields V, W\in C^{\infty}(TX)\subset C^{\infty}(Cl(TX)) and for any section s\in C^\infty(S):

\nabla^S_V(W\cdot s) = \nabla^X_V W \cdot s + W\cdot \nabla^S_V s.

Definition (A Dirac operator)

A differential operator D: C^\infty(S)\to C^\infty(S) is a Dirac operator if

(1) D is a Dirac type operator, and

(2) S is Clifford compatible.


If X is oriented and D is a Dirac operator, then D is formally self-adjoint. That is,
\langle\langle Ds, t\rangle\rangle = \langle\langle s, Dt\rangle\rangle,
where \langle\langle s,t\rangle\rangle = \int_{X} \langle s, t \rangle (and the integration is with respect to the volume form on X).


Omitted 😦 \square

Consequently we have \text{index}(D)=0 (see Ning’s blog). To make use of the index, then, we introduce a Z_2-grading on Clifford module bundles.


Recall that a Clifford algebra is \mathbb{Z}-filtered — Cl_n=\cup_{i} {Cl_n^i} with Cl_n^i\cdot Cl_n^j\subset Cl_n^{i+j} — and \mathbb{Z}_2-graded — Cl_n={Cl_n}^{+}\oplus {Cl_n}^- (even and odd products).

A Clifford module bundle S is \mathbf{Z}_2-graded if it decomposes into a direct sum S=S^+\oplus S^- of vector bundles such that for each x\in X and v\in T_xX, one has v\cdot S_x^{\pm} \subset S_x^{\mp}.

Such a \mathbb{Z}_2-graded bundle is compatible if this decomposition is both orthogonal with respect to \, \langle, \rangle and parallel with respect to the covariant derivative \nabla^S, ie. \nabla^S S^{\pm} \subset S^{\pm}.


If X is oriented, the Clifford bundle Cl(TX) = Cl^+(TX) \oplus Cl^-(TX) is a \mathbb{Z}_2-graded compatible Clifford bundle. Some words which may be connected to verify this: Levi Civita connection, induced connection on F(TX), lift to principal spin bundle, induced covariant derivative on associated vector bundle, compatibility with the metric.

Examples of Dirac Operators

We now look at four examples of Dirac operators. The first two are familiar; here we reinterpret them in terms of Clifford modules.

Example 1: The De Rham Operator

Recall that the filtered algebra Cl(V^n,q) = \cup Cl^i(V,q) has associated graded algebra Gr(Cl(V,q))\cong \Lambda^\ast V. (See the Glossary below.)


Let f:\Lambda^\ast(\mathbb{R})\to Cl_n(\mathbb{R}) be the map defined by

v_1\wedge \ldots \wedge v_r\mapsto \frac{1}{r!} \sum_{\sigma\in \Sigma_r} \text{sign}(\sigma) v_{\sigma(1)}\cdot v_{\sigma(2)}\cdots v_{\sigma(r)}.

Then f is

(1) an isomorphism of vector spaces

(2) filtration preserving, i.e., f(\oplus_{i\leq r} \Lambda^i(\mathbb{R}))\subset {Cl_n}^r(\mathbb{R}), and

(3) O(n)-equivariant, i.e., f(A\omega) = A f(\omega) for \omega\in \Lambda^\ast(\mathbb{R}) and A\in O(n).


(1) and (2). Let e_1, \ldots, e_n is an orthonormal basis for \mathbb{R}^n. Since (by an equivalent definition of the exterior algebra) v_1\wedge \ldots \wedge v_r = \frac{1}{r!} \sum_{\sigma\in \Sigma_r} \text{sign}(\sigma) v_{\sigma(1)}\otimes v_{\sigma(2)}\otimes\ldots \otimes v_{\sigma(r)}, we see that f is induced by the map T(\mathbb{R}^n) \to Cl_n(\mathbb{R}) taking e_{i_1}\otimes \cdots\otimes  e_{i_r} to e_{i_1}\ldots e_{e_r} and descending to \Lambda^\ast(V); that is, f(e_{i_1}\wedge\ldots \wedge e_{i_r}) = e_{i_1}\cdots e_{i_r}. It follows that f is an isomorphism and preserves the grading.

(3) Using that Ae_1\wedge \ldots Ae_n = (\text{det} A) (e_1\wedge \ldots e_n), I feel like we need to be working with SO(n) here. Please comment! \square


The exterior algebra bundle over a(n oriented?) manifold \Lambda^\ast(T^\ast X) and the clifford bundles Cl(TX) are isomorphic as vector bundles.


Let F(TX) denote the principal O(n)-bundle associated to TX. By parts (1) and (3) of the lemma, the map f above induces a vector bundle isomorphism \Lambda^\ast(TX) = F(TX)\times_{O(n)} \Lambda^\ast(\mathbb{R}^n) \to F(TX)\times _{O(n)} Cl_n(\mathbb{R}) = Cl(TX). \square

Theorem 2.5.12 (Lawson, Michelsohn)

Under this bundle isomorphism \Lambda^\ast(T^\ast X) \cong Cl(TX), the de Rham operator d+d^\ast corresponds to the Dirac operator D.


Since we have already established (see Hailiang’s(?) blog post) that the Euler characteristic \chi(X) of X is equal to \text{Index}(d+d^\ast|_{\Omega^{\text{even}}}:\Omega^{\text{even}}\to \Omega^{\text{odd}}), the theorem (along with the grading-preserving property of f) implies we may also compute it as \text{Index}(D|_{C^\infty(Cl^+(TX))}: C^\infty(Cl^+(TX))\to C^\infty(Cl^-(TX))).

Example 2: The Signature Operator

We now look to reinterpret the signature operator in terms of Clifford bundles.

Recall (see Hailiang’s blog) in the case that n=2p and p is even, the Hodge star operator \ast: \Omega^p\to \Omega^{n-p} is an involution so we can decompose \Omega^p = \Omega^p_+\oplus \Omega^p_- into the +1 and -1 eigenspaces of \ast. We defined the signature operator D = d+d^\ast. Since D\ast = -\ast D, we saw that D took \Omega^p_{\pm} to \Omega^p_{\mp} and letting D_+=D|_{\Omega^p_+}, we found that \text{Index}(D_+) = \text{Sign}(X). The signature \text{sign}(X) of X was defined to be the signature of the quadratic form on \mathcal{H}^p given by (\alpha,\beta)\mapsto \int_X \alpha\wedge \beta.

In the case that p is odd, we had to modify the construction. We complexified, taking \Omega_\mathbb{C}^p = C^\infty(\Lambda^p(T^\ast X\otimes \mathbb{C})), and defined \tau = i\ast. Then the above paragraph went through with \tau replacing \ast and \Omega_\mathbb{C} replacing \Omega.

Let \{e_1, \ldots, e_n\} be an oriented orthonormal basis for \mathbb{R}^n. Let \omega = e_1\cdots e_n in Cl_n. Then by the lemma above and the corresponding properties of the volume form e_1\wedge\ldots \wedge e_n in \Lambda^\ast(\mathbb{R}^n), we obtain that \omega is a basis-independent section of Cl_n(\mathbb{R}).


(1) We have \omega^2 = \begin{cases} 1 \qquad n\equiv 0, \, 3 \mod 4\\  -1 \qquad n\equiv 1, \, 2 \mod 4  \end{cases}

(2) If n is even and v\in \mathbb{R}^n, then \omega \cdot v = -v \cdot \omega.


(1) We compute (e_1\cdots e_n)(e_1\cdots e_n) = (-1)^n(-1)^{n-1}\cdots (-1)^2 (-1)^1 = (-1)^{n(n+1)/2}. Writing n=4k+l for 0\leq l\leq 3, one finds that n(n+1)/2 is even if and only if l=0 or 3.

(2) It suffices to verify for v=e_i. We have (e_1\cdots e_n)\cdot e_i = (-1)^{n-i} e_1\cdots \hat{e}_i\cdots e_n and e_i \cdot (e_1\cdots e_n) = (-1)^i e_1\cdots \hat{e}_i\cdots e_n. (Here, a hat \hat{} indicates that the element be omitted from the product.) Since n is even, (-1)^{n-i}=(-1)^i. \square

Now, \omega acts on any Clifford module via v\mapsto w\cdot v, and by part (1) of the lemma this defines an involution in the case n\equiv 0, 3\mod 4; in the case n\equiv 1, 2\mod 4, i\omega defines an involution. Compare with the Hodge star operator recalled above. So define

\Gamma = \begin{cases} \omega \qquad n\equiv 0, \, 3 \mod 4,\\  i\omega \qquad n\equiv 1, \, 2 \mod 4;  \end{cases}

then \Gamma^2=\text{Id}. Thus if X is an oriented manifold and S is a Clifford module bundle of X, putting S^{\pm} = \{v\in S: \Gamma v = \pm v\}, we have

if n\equiv 0, 3 \mod 4: S = S^+\oplus S^-, or

if n\equiv 1,2 \mod 4: S_\mathbb{C} = S_\mathbb{C}^+\oplus S_\mathbb{C}^-


If n is even then S is \mathbb{Z}_2-graded, i.e., for x\in X and v\in T_xX, one has v\cdot S_x^{\pm} \subset S_x^{\mp}.


By part (2) of the lemma, for v\in T_xX we have \Gamma v = -\Gamma v.
Thus if e\in S_x^{\pm} (i.e. \Gamma e = \pm e) then v\cdot e = v\cdot (\pm \Gamma(e)) = \mp \Gamma(v\cdot e), so v\cdot e\in S^{\mp}. \square


If n is even and S is \mathbb{Z}_2-graded compatible, then the associated Dirac operator splits as
D = \left( \begin{array}{cc}0 & D^-\\ D^+ & 0\end{array}\right): C^\infty S^+\oplus C^\infty S^-\to  C^\infty S^+\oplus C^\infty S^-.
In particular, if S=Cl(TX), by Theorem 2.5.12 we have \text{Index}(D^+) = \text{Sign}(X).


Since S is \mathbb{Z}_2-graded and is compatible (so in particular, the covariant derivative preserves S^{\pm}), the Dirac operator
Ds = \sum e_i\cdot \nabla_{e_i}^S s
takes C^\infty(S^{\pm}) to C^\infty(S^{\mp}). \square

Example 3: twisted Dirac Operators

Preliminary: If S and E are vector bundles over X with covariant derivatives \nabla^S and \nabla^E, respectively, then the tensor product bundle S\otimes E\to X has covariant derivative
\nabla^S\otimes \nabla^E := \text{Id}_S\otimes \nabla^E + \nabla^S\otimes \text{Id}_E.

Fact: If S is a compatible \mathbb{Z}_2-graded Clifford module bundle and (E, g, \nabla^E) is a Riemannian bundle (see Property (1) of a compatible Clifford Bundle above for the definition), then S\otimes E is a compatible \mathbb{Z}_2-graded Clifford module bundle (with Clifford multiplication v\cdot(s\otimes e) = (v\cdot s)\otimes e for v\in Cl_n, s\in S, e\in E). In the case that S=Cl(TX_{\mathbb{C}}), we call the Dirac operator on S\otimes E a twisted Dirac operator.

Fact: (Apparently from topological K-theory) If the Index theorem holds for any twisted Signature operator then it holds for all elliptic differential operators.

Example 4: Spin Manifolds and The Atiyah-Singer Dirac Operator

Recall (see Prasit’s blog) that there is an isomorphism \varphi: Cl_{2l}(\mathbb{C}) \xrightarrow{\cong} M_{2^l}(\mathbb{C}). So since
\mathbb{C}^n is an M_n(\mathbb{C}) module, one has that \mathbb{C}^{2^l} is an Cl_{2l}(\mathbb{C})-module via a\cdot v = \varphi(a)v, for a\in Cl_{2l}(\mathbb{C}) and v\in \mathbb{C}^{2^l}. To avoid confusion, let us call \mathbb{C}^{2^l} with this module structure C.

Now, any M_{2^l}(\mathbb{C})-module is isomorphic to \oplus^{2^l} \mathbb{C}^{2^l}, so it follows that any Cl_{2l}(\mathbb{C})-module is isomorphic to \oplus^{2^l} C.

Let S be a Clifford module bundle. From the above paragraph we see that each fiber (a Cl_{2l}(\mathbb{C})-module) is isomorphic (via \varphi_x, say) to \oplus^{2^l} C_x, where C_x is a copy of C. We may then
ask if this splitting extends over the whole bundle; that is, is there a Clifford module bundle S\to X and a bundle isomorphism \varphi:S\to \oplus^{2^l} C which restricts fiberwise to an isomorphism S_x\cong \oplus^{2^l} C.

In turns out the answer is a resounding “Yes” if X is a spin manifold.

Definition (Spin Structure)

Let E\to X is an N-dimensional vector bundle. A spin structure on E is a principal \text{Spin}(N)-bundle P\to X together with a bundle isomorphism P\times_{\text{Spin}(N)} \mathbb{R}^N\to E. (Then E is the associated vector bundle for P). Using classifying space theory, we may reinterpret this
to say that a spin structure on E is a lift of the classifying map \varphi_E: X\to BGL_N(\mathbb{R}) to B\text{Spin}(N).

We may break up the existence of a spin structure into pieces as follows.

After choosing a metric on E, we may first reduce the structure group of E to O(n). (The only obstruction to doing so is the paracompactness of X.) So we’re left to lift a map \varphi_E: X\to BO(n) to B\text{Spin}(N).

Since B\text{Spin}(N) is the universal cover of BSO(N), we may first try to lift \varphi_E to BSO(n).

The short exact sequence of groups 1\to SO(N)\to O(N)\xrightarrow{\text{det}} \mathbb{Z}_2\to 1 induces a fibration of classifying spaces
X\xrightarrow{\varphi_E} BO(N)\to B\mathbb{Z}_2=K(\mathbb{Z}_2,1).

It turns out that the map X\to BO(N) lifts to BSO(N) if and only if the composite X\xrightarrow{\varphi_E} BO(N)\to B\mathbb{Z}_2=K(\mathbb{Z}_2,1) is nullhomotopic. Since [X, K(\mathbb{Z}_2,1)]\cong H^1(X;\mathbb{Z}_2), there is an element \omega_1(E)\in H^1(X;\mathbb{Z}_2) that vanishes if and only if \varphi_E lifts. We call \omega_1(E) the first Stiefel Whitney class of E.

Similarly, the map X\to BSO(N) lifts to B\text{Spin}(N) if and only if the composition X\to BSO(N)\to B K(\mathbb{Z}_2,1)=K(\mathbb{Z}_2,2) is nullhomotopic; we call the corresponding element in H^2(X;\mathbb{Z}_2)\cong [X, K(\mathbb{Z}_2,2)] (that vanishes iff X\to BSO(N) lifts) the second Stiefel Whitney class \omega_2(E) of E.

Definition (Spin manifold)

We will call an oriented manifold X (so \omega_1(TX)=0) a spin manifold if its tangent bundle TX admits a spin structure (i.e., \omega_2(TX)=0). It can be shown that this is equivalent to the existence of a trivialization of TX over the 2-skeleton of X. (Compare with the fact that X is orientable if and only if TX is trivializable over the 1-skeleton.)

Definition (The Atiyah-Singer Dirac Operator)

Suppose X^n has a spin structure with principal \text{Spin}(n)-bundle P (associated to TX). Since Cl_n(\mathbb{C}) acts on C on the left and \text{Spin}(n)={Cl_{n}}^+(\mathbb{C})\cap \langle S^{n-1}\rangle (where \langle S^{n-1}\rangle has general element x_1\cdot x_2\cdots x_k with x_i\in \mathbb{C}^n, x_i^2=1) is a subgroup of the group of units Cl_n^\times, we may define
the C-bundle associated to P by \mathbf{C} = P\times_{\text{Spin}(n)} C\to X. Since C is a Cl_n(\mathbb{C}) module, \mathbf{C} is a Clifford module bundle.

Some words: By lifting the Levi-Civita connection on P_{SO(n)} one obtains a connection on P_{\text{Spin}(n)}, and hence (see who’s blog?) a covariant derivative \nabla^\mathbf{C} on \mathbf{C} which makes it Clifford compatible
as a \mathbb{Z}_2 graded Clifford module bundle.

We may then define the Atiyah-Singer Dirac Operator by

Ds = \sum e_i\cdot \nabla_{e_i}^\mathbf{C} s.

Some more words:

If Ds=0 then s is called a harmonic spinor.

If X has positive scalar curvature, then D is injective. So if we have ways to compute the index (using the ASHI theorem, for example), we may be able to deduce that X does not admit a metric of positive scalar curvature.


(to include links to other blog posts)

Differential Operator (global definition)

If E and F are vector bundles over X (of the same dimension), we define the family of differential operators of order \leq m from E to F by

DO_m(E,F) = \{D\in \text{Hom}_{\mathbb{R}}(C^\infty E, C^\infty F):\, [D,f]\in DO_{m-1}(E,F) \, \forall f\in C^{\infty}(X)\}

with DO_{-1}(E,F)=\{0\}. In particular, DO_{0}(E,F) = \{C^{\infty}(X)\text{-linear bundle maps } C^\infty(E)\to C^\infty(F)\}.

Symbol of a differential operator

(cf. Juanita’s blog) We recall the definition of the symbol \sigma_D of an order-m differential operator D:C^\infty(E)\to C^\infty(F). Denote T^\ast X\xrightarrow{\pi} X, E\xrightarrow{p} X, so \pi^\ast(E)=\{(\xi^\ast,e)\in T^\ast X\times E:\, \pi(\xi^\ast)=x=p(e)\}. Let \xi^\ast\in T^\ast X. Let x\in X. The symbol \sigma_D(\xi^\ast) of D at x is the homomorphism E_x\to F_x defined by

\sigma_D(\xi^\ast)(s(x)) = \frac{1}{i} \frac{1}{m!} D(f^m s)(x)

where s\in C^\infty(E), and f\in C^\infty(X) is such that df_x = \xi^\ast(x).

Covariant Derivative

A covariant derivative \nabla on a vector bundle E\to X is a map \nabla: C^{\infty}(TX)\times C^{\infty}(E)\to C^{\infty}(E), (v,s)\mapsto \nabla^S_v s where \nabla_v^S is an \mathbb{R}-linear map C^\infty(E)\to C^{\infty}(E) satisfying the Leibnitz rule \nabla^S_v (fs) = v(f)s + f\nabla^S_v(s) for s\in C^\infty(E) and f\in C^\infty(X).

Graded Algebras

(cf Prasit’s blog) A k-algebra A is \mathbb{Z}-graded if A=\bigoplus_i A_i such that A_i A_j\subset A_{i+j}. A k-algebra is filtered over \mathbb{Z}
if A=\cup A^i such that A^i\subset A^{i+1} and A^i A^j \subset A^{i+j}. A graded algebra A=\bigoplus_i A_i defines a filtered algebra by taking A^i=A_0\oplus\ldots A_i, and conversely a filtered algebra A=\cup_i A^i defines a graded algebra by taking A_i=A^i/A^{i-1} (with A^{-1}=0).

Tensor Algebra and the Clifford Algebra

If V is a vector space, the tensor algebra TV = \mathbb{R}\oplus V\oplus V\otimes V\oplus\ldots \oplus V\oplus\ldots \oplus V has multiplication defined by concatenation, i.e., (x_1\otimes \ldots \otimes x_j)(y_1\otimes \ldots \otimes y_j) = x_1\otimes \ldots \otimes x_j \otimes y_1\otimes \ldots \otimes y_j. Thus TV is a graded algebra with (TV)_i = \underbrace{V\otimes \ldots \otimes V}_{\text{\emph{i}  times}}, and filtered with (TV)^i=\mathbb{R}\oplus \cdots \oplus  V\otimes\cdots \otimes V.

Recall that Cl(V,q)=\cup_i Cl^i(V,q) with Cl^i(V,q)=(TV)^i/{\langle v\otimes v = -q(v)\rangle}. (Here, q is a quadratic form; sometimes it is convenient to refer instead to the associated symmetric bilinear form \beta.) For any v\in V, q(v)\in \mathbb{R}=Cl^0(V,q) so q(v) maps to 0 under the quotient Gr_i(Cl(V,q))= Cl^i(V,q)/Cl^{i-1}(V,q). This sets up a natural identification between Gr_i(Cl(V,q)) and (\Lambda^\ast V)_i = \frac{(TV)_i}{\langle v\otimes v=0\rangle}. Whence the associated graded algebra for Cl(V,q) is isomorphic to \Lambda^\ast V. In particular, they are isomorphic as vector spaces, with dimension \sum_{k=0}^n \begin{pmatrix}n\\k\end{pmatrix}=2^n.

Clifford bundle

The Clifford bundle Cl(TX)\xrightarrow{\pi} X has fibers Cl(T_xX, g_x) \cong Cl_n(\mathbb{R}) (x\in X), where g is a Riemannian metric on X. (The latter isomorphism is given by identifying an orthonormal (with respect to g_x) basis for T_xX with the standard generators \{e_i\}.) Just as TX is the \mathbb{R}^n-bundle associated to the orthogonal frame bundle (of the tangent bundle) F(TX) over X, Cl(TX) is the associated Cl_n(\mathbb{R})-bundle to F(TX).

Written by aclightf

November 21, 2012 at 7:45 pm

Posted in Uncategorized

Clifford algebras and Spin groups

leave a comment »

Still lot of editing needed. the pdf file can be obtained here

As a provisional definition, clifford algebraover a field {k} can be defined as

\displaystyle Cl_{n}(k) = k[x_{1}, \ldots, x_{n}] /R


\displaystyle R = < x_{i}^{2} = -1, x_{i} x_{j} = - x_{j}x_{i} \forall i \neq j >

Easy to see that {Clifford} {Algebra} has dimension {2^{n}}. {Cl_{n}(k)} can also be thought of as

\displaystyle Cl_{n}(k) = TV / R

where {V = k^{n}} as vector space, {TV} is the tensor algebra, {R} is same as above, except that {x_{i}}‘s are standard basis for {V}. This observation leads to a more general definition of clifford algebra, where {V} is a vector space equipped with a symmetric bilinear form

Definition 1 Let {V} be a vector space with symmetric biliear form {\beta} and quadratic form {q = \beta(x,x)}. Then the clifford algebraover {V} can be defined as\displaystyle Cl(V, q) = TV / < x \otimes x + q(x)>

Remark 1 These are some of the properties that {CL(V, q)} enjoys

  1. There is a natural inclusion of {i: V \hookrightarrow Cl(V,q)}.
  2. If {q(x) = 0 \forall x \in V} then {Cl(V, q) = \bigwedge(V)} the exterior algebra
  3. Let {.} denote the clifford multiplication( induced by the tensor product of {TV}), then\displaystyle x . y + y . x = -2 \beta(x,y)
  4. Universal Property : Let {f: V \longrightarrow A}, where {A} is a {k}-algebra, such that {f(x)^{2} = -q(x)}, then there exists an unique map {F} such that {f = F \circ i}, that is the following diagram commutes\displaystyle \xymatrix@C-1pc{ V\ar[d]^{i} \ar[r]^{f}&A\\ Cl(V,q)\ar@{.>}[ur]_{F} }
  5. A map {\phi: ( V,q) \longrightarrow (V',q')}, such that {q'(\phi (x)) = q(x)}, extends to a {k}-algebra homomorphism\displaystyle \Phi: Cl(V,q) \longrightarrow Cl(V', q')Thus the orthogonal group {\mathbb{O}(n)} has an action on {Cl_{n}(\mathbb{R})}

Proposition 2 {Cl(v,q)} is a filtered algebra whose associate graded is {\bigwedge(V)}

Before proving the theorem, recall the following definition

Definition 3 If {A} is a {k}-algebra then a filtration {(A,\mathfrak{F} )} of {A} is sequence of subspaces\displaystyle F_{0}A \subset F_{1}A \subset \dots \subset A = \bigcup_{r}F_{r}A

The associate gradedof {(A, \mathfrak{F})} is defined as\displaystyle Gr(A, \mathfrak{F}) = \bigoplus_{r} F_{r}A/F_{r-1}A

Proof: Let {\pi} be the quotient map

\displaystyle \pi : TV \longrightarrow Cl(V,q)

Define, {G_{r} = V \otimes \ldots \otimes V} ({r} fold tensor product). Define filtration on {TV} by setting

\displaystyle F_{r}TV = \bigoplus_{i \leq r} G_{i}

Define filtration {\pi_{*}F_{r} TV} be the filtration on the clifford algebra. Note {x \otimes x = q(x) \in \pi_{*}F_{0}Cl(V, q)}. Hence, in the associated graded {x \otimes x = 0}. On the other hand the relation { x_{i}x_{j} = -x_{j} x_{i} } prevails in the associated graded. Hence the associate graded is isomorphic to {\bigwedge V}. \Box

Remark 2 {Cl(V,q)} is a { \mathbb{Z}/2}-graded algebra.\displaystyle Cl^{0}(V,q) = \pi_{*} TV^{even}

\displaystyle Cl^{1}(V,q) = \pi_{*} TV^{odd}

Definition 4 Recall,{S^{n-1} \subset V \hookrightarrow Cl(V,q)}. Define,\displaystyle Pin(n) = S^{n-1} \subset Cl^{\times}(V,q)(units)

and\displaystyle Spin(n) = S^{n-1} \cap Cl^{0}(V,q)

On {Cl(V,q)} we have an involution map, which is induced by the involution on {TV} given by,

\displaystyle \overline{x_{1} \otimes \ldots \otimes x_{r}} = (-1)^{r} x_{1} \otimes \ldots \otimes x_{r}

If {x \in S^{n-1} \subset Cl(V.q)} then

\displaystyle x .\overline{x} = - \beta (x,x )= q(x) = 1

Let {v \in V \subset Cl(V,q)} and {x \in Pin(n)}, then observe

\displaystyle q(-x.v.\overline{x}) = \beta(-x.v .\overline{x},-x.v.\overline{x}) = x.(-q(v)).x =- q(v).(-q(x)) = q(v)

Lemma 5 There exist short exact sequences\displaystyle 1 \longrightarrow \lbrace-1, +1 \rbrace \longrightarrow Pin(n) \xrightarrow{p}\mathbb{O}(n) \longrightarrow 1

and\displaystyle 1 \longrightarrow \lbrace-1, +1 \rbrace \longrightarrow Spin(n) \xrightarrow{p} \mathbb{SO}(n) \longrightarrow 1

where {p} is the map which sends\displaystyle x \mapsto ( v\mapsto-x.v.\overline{x)}

Let {k} be a field. Recall, tensor product of {k}-algebras {A} and {B} is a {k}-algebra, denoted by {A\otimes_{k}B } and multiplication is given by

\displaystyle (a \otimes b).(a' \otimes b')= aa' \otimes bb'

moreover if {M_{j}(A)} denotes the set of all {j \times j} matrices. Then we have the following isomorphism

\displaystyle M_{j}(A) \otimes M_{k}(B) \cong M_{jk}(A \otimes B)


\displaystyle Cl_{p,q}(k) = Cl(k^{p+q},x_{1}^{2}+ \ldots+ x_{p}^{2} - x_{p+1}^{2} - \dots x_{p+q}^{2} )

Remark 3 If {k = \mathbb{C}}, then\displaystyle Cl_{p,q}(\mathbb{C}) \cong Cl_{p+q,0}(\mathbb{C})

This follows from the fact that the quadratic forms {q_{p,q}(x)=x_{1}^{2}+ \ldots+ x_{p}^{2} - x_{p+1}^{2} - \dots x_{p+q}^{2}} and {q_{p+q,0}(x)=x_{1}^{2}+ \dots+ x_{p+q}^{2}} induces isomorphic innerproduct structure on {\mathbb{C}^{p+q}} where the isomorphism sends\displaystyle e_{t} \mapsto e_{t}: 0 \leq t \leq p

\displaystyle e_{t} \mapsto ie_{t}: p < t \leq p+q

Theorem 6 If {k= \mathbb{C}}, then we have the following isomorphisms

  1. {Cl_{0}(\mathbb{C}) = \mathbb{C}}
  2. {Cl_{1}(\mathbb{C}) = \mathbb{C} \times \mathbb{C}}
  3. {Cl_{2}(\mathbb{C}) = M_{2}(\mathbb{C})}
  4. {Cl_{n+2}(\mathbb{C}) = M_{2}(Cl_{n}(\mathbb{C}))}

Corollary 7 (Bott Periodicity) As a consequence of (iv) we have\displaystyle Cl_{n}(\mathbb{C}) = M_{2^{n}}(\mathbb{C})

if {n} even, and\displaystyle Cl_{n}(\mathbb{C}) = M_{2^{n}}(\mathbb{C}) \times M_{2^{n}}(\mathbb{C})

if {n} is odd.

To work out the case when the underlying field is {\mathbb{R}}. For any field {k} we have the following isomorphisms.

Lemma 8 For any field {k}

  1. {Cl_{n+2,0}(k) \cong Cl_{0,n}(k) \otimes Cl_{2,0}(k) .}
  2. { Cl_{o,n+2}(k) \cong Cl_{n,0}(k) \otimes Cl_{0,2}(k).}

Proof: Let {e_{i}} denote the standard basis of {k^{n+2}} and cannonical generatoring set of the Clifford algebra { Cl_{n+2,0}(k)}.

  1. To get the first isomorphism we simply produce a map given by sending\displaystyle e_{i} \mapsto e_{i} \otimes e_{i}e_{2} \forall 1\leq i \leq nand\displaystyle e_{n+1} \mapsto 1 \otimes e_{1}\displaystyle e_{n+2} \mapsto 1 \otimes e_{2}It is easy to check that the above map is an isomorphism.
  2. is similar to {(i)}.

\Box One can explicitly check some of the lower dimension cases( { n = 0, 1, 2}). Then one can repeatedly use the isomorphisms in previous lemma. One has to work upto dimension {8} when {k= \mathbb{R}}, before one sees the patern, which is called the Bott periodicity. TSome of the calculations are as follows calculations are as follows

  1. {Cl_{0,0}(\mathbb{R}) \cong \mathbb{R}}
  2. {Cl_{1,0}(\mathbb{R})\cong \mathbb{C}}
  3. {Cl_{0,1}(\mathbb{R}) \cong \mathbb{R} \times \mathbb{R}}
  4. {Cl_{2,0}(\mathbb{R}) \cong \mathbb{H}}
  5. {Cl_{0,2}(\mathbb{R}) \cong M_{2}(\mathbb{R})}
  6. {Cl_{3,0}(\mathbb{R}) \cong Cl_{0,1}(\mathbb{R}) \otimes Cl_{2,0}(\mathbb{R})\cong (\mathbb{R} \times \mathbb{R})\otimes \mathbb{H}\cong \mathbb{H}\times \mathbb{H} }
  7. {Cl_{4,0}(\mathbb{R}) \cong Cl_{0,2}(\mathbb{R}) \otimes Cl_{2,0}(\mathbb{R})\cong M_{2}(\mathbb{R})\otimes \mathbb{H}\cong M_{2}(\mathbb{H}) }
  8. In general one gets,
    {Cl_{n+4,0}(\mathbb{R}) \cong Cl_{0,n+2}(\mathbb{R}) \otimes Cl_{2,0} \cong Cl_{n,0}(\mathbb{R}) \otimes Cl_{0,2}(\mathbb{R}) \otimes Cl_{2,0}(\mathbb{R})}

Putting all these observations together we get

Theorem 9 The Bott periodicity in case of real number looks like\displaystyle Cl_{8k+r}(\mathbb{R}) = \left\lbrace \begin{array}{cccccc} M_{2^{4k}}(\mathbb{R})& r=0\\ M_{2^{4k}}(\mathbb{C})& r=1\\ M_{2^{4k}}(\mathbb{H})& r=2\\ M_{2^{4k}}(\mathbb{H}) \times M_{2^{4k}}(\mathbb{H})& r=3\\ M_{2^{4k+1}}(\mathbb{H})& r=4\\ M_{2^{4k+2}}(\mathbb{C})& r=5\\ M_{2^{4k+3}}(\mathbb{R})& r=6\\ M_{2^{4k+3}}(\mathbb{R}) \times M_{2^{4k+3}}(\mathbb{R})& r=7\\ \end{array} \right.

Lemma 10 As {k}-algebras {Cl_{n}^{0}(k) \cong Cl_{n-1}(k)} Proof:The isomorphism is given explicitly by the map induced by sending

\displaystyle e_{i} \mapsto e_{i}.e_{n}

Easy to check that this is an isomorphism of algebras. \Box

Written by prasit0605

October 27, 2012 at 6:41 pm

Posted in Uncategorized

Hermitian metrics and Kähler manifolds

leave a comment »

This post will be converted to WordPress soon; in the meantime, view it in PDF form as sections 3 and 4 here: ComplexManifolds

Written by Henry T. Horton

October 25, 2012 at 7:46 pm

Posted in Uncategorized

Complex manifolds and the Dolbeault complex

leave a comment »

This post will be converted to WordPress soon; in the meantime, view it in PDF form as sections 1 and 2 here: ComplexManifolds

Written by Henry T. Horton

October 23, 2012 at 6:28 pm

Posted in Uncategorized

Hodge star operator and Signature operator

leave a comment »

Let k=\mathbb{R} or \mathbb{C} and V be an inner product space with\{e_1,\cdot\cdot\cdot,e_n\} a fixed orthonormal basis,\Lambda^p V be the space of p form

Hodge Star Operator

Lemma 1  There is a unique map \ast:\Lambda^p V\rightarrow\Lambda^{n-p} V s.t. for any \alpha,\beta\in\Lambda^p V

\langle\alpha,\beta\rangle vol=\alpha\wedge\ast\beta

PROOF. (Uniqueness) suppose we have another map \ast', then

\alpha\land(\ast-\ast')\beta=\alpha\land\ast\beta-\alpha\land\ast'\beta=0 for every \alpha

 so (\ast-\ast')\beta=0 for every \beta,i.e.\ast=\ast'

(Existence) Fix an oriented orthonormal basis \{e_1,\cdot\cdot\cdot,e_n\}, for \sigma\in S_n

we define                            \ast(e_{\sigma(1)}\land\cdot\cdot\cdot\land e_{\sigma(n)})=\rm{sign}(\sigma)e_{\sigma(p+1)}\land\cdot\cdot\cdot\land e_{\sigma(n)}


We have      \ast(e_1\land\cdot\cdot\cdot\land e_p)=e_{p+1}\land\cdot\cdot\cdot \land e_{n}  and   \ast\ast=(-1)^{p(n-1)}

Suppose X^n is an oriented closed Riemannian Manifold,\alpha,\beta are pforms,define the l^2 inner product by


Using integration by parts and stokes theorem,we have the following equalities:

\langle d\alpha,\beta\rangle =\int_{X} d\alpha\land\ast\beta

= (-1)^p\int_{X} \alpha\land d\ast\beta

= (-1)^p\int_{X}\alpha\land (-1)^{(n-p-1)(p+1)}\ast\ast d\ast\beta

= \langle\alpha,(-1)^{n(p+1)+1}\ast d\ast\beta\rangle

hence we yield
Lemma 2 The formal adjoint of d is \delta=(-1)^{n(p+1)+1}\ast d \ast,i.e.\langle d\alpha,\beta\rangle=\langle\alpha,\delta\beta\rangle.

Exercise   Define \Delta=d\delta+\delta d,show that \ast\Delta=\Delta\ast
Corollary  \ast:\mathcal{H}^p\xrightarrow{\cong}\mathcal{H}^{n-p}

Harmonic Form and Signature

 If \tau:V\rightarrow V is an involution and charF\neq 2,then

V=V_+\oplus V_{-}

where V_{\pm} denote the \pm 1 eigenspace of \tau

If n=4k,p=2k,then \ast\ast=1

Theorem 1                                   \mbox{sign}(X)=\dim\mathcal{H}_{+}^p-\dim\mathcal{H}_{-}^p

PROOF using corollary,we could define the following nondegenerate  bilinear form:


Let \mathcal{H}_{\pm 1}^p be the \pm 1 eigenspace of \ast. For \alpha\in\mathcal{H}_{+}^p,\beta\in\mathcal{H}_{-}^p,we have:

I(\beta,\beta)=-I(\beta,\ast\beta)=-\langle\beta,\beta\rangle\leq 0

Hence there is a decomposation


and I is positive definite on \mathcal{H}_+\times\mathcal{H}_+ and negative definite on \mathcal{H}_-\times\mathcal{H}_-

Using Hodge-de Rham isomorphism          \mathcal{H}^p(X)\cong H^p(X,\mathbb{R})

the above non degenerate bilinear form is equivalent to the intersection form:

I':H^p(X,\mathbb{R})\times H^p(X,\mathbb{R})\rightarrow\mathbb{R},(\alpha,\beta)\mapsto\langle\alpha\cup\beta,[X]\rangle

So we have

\mbox{sign}(X)=\dim H_{+}^p-\dim H_{-}^p=\dim\mathcal{H}_{+}^p-\dim\mathcal{H}_{-}^p

Signature Operator

If n=2l,then \ast\ast=(-1)^{p(n-p)}=(-1)^p

Let \Omega^p=C^{\infty}(\Lambda^p T_{\mathbb{C}}^{\ast}X^{2l}) be the complex-valued p forms,define


we have                           \tau^2=Id     and       (d+\delta)\tau=-\tau(d+\delta)

 so if we write \Omega^{\ast}=\Omega_{+}^{\ast}\oplus\Omega_{-}^{\ast},where \Omega_{\pm 1}^{\ast} denotes the \pm 1-eigenspace of \tau,then D=d+\delta interchanges \Omega_{\pm 1}^{\ast}, due to its anti-commutitivity with \tau, i.e.:

D=d+\delta=\begin{bmatrix}  0 & D_{-} \\  D_{+} & 0  \end{bmatrix}: \Omega_{+}^{\ast}\oplus\Omega_{-}^{\ast}\rightarrow\Omega_{+}^{\ast}\oplus\Omega_{-}^{\ast}

Definition D_{+}:\Omega_{+}^{\ast}\rightarrow\Omega_{-}^{\ast} is called the  signature operator

Theorem 2                                        \mbox{Index}(D_{+})=\mbox{sign}(X)

PROOF  we have following facts:

  • (d+\delta)^2=\Delta is elliptic,hence d+\delta is elliptic,so are D_{+} and D_{-}. \dim (\mbox{ker} D_{+}) and \dim (\mbox{ker} D_{-}) are finite
  • D is self-adjoint,so (D_{+})^{\ast}=D_{-}
  • \mbox{ker} (d+\delta)=\mbox{ker}\Delta.so \mbox{ker} D_{\pm 1} consists of harmonic forms for the \pm 1 eigenvectors of \tau
  • \dim\mathcal{H}_{+}^p=\dim\mathcal{H}_{-}^{n-p} for p\neq l

Using these facts,we yield:     \mbox{Index} (D_{+}) = \dim (\mbox{ker} D_{+})-\dim(\mbox{coker} D_{+})

=\dim(\mbox{ker}D_{+})-\dim(\mbox{ker} D_{+}^{\ast})

=\dim(\mbox{ker}D_{+})-\dim(\mbox{ker} D_{-})

=\Sigma_p\dim\mathcal{H}_{+}^p-\Sigma_p \dim\mathcal{H}_{-}^p



Written by hailhu

October 21, 2012 at 4:13 pm

Posted in Uncategorized

%d bloggers like this: