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Quantum Field Theory and Gravity: Conceptual and Mathematical ...

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190 C. Bär <strong>and</strong> N. Ginoux<br />

3.2. Differential operators <strong>and</strong> Green’s functions<br />

A differential operator of order (at most) k on a vector bundle S → M over<br />

K = R or K = C is a linear map P : C ∞ (M,S) → C ∞ (M,S) which in local<br />

coordinates x =(x 1 ,...,x m )ofM <strong>and</strong> with respect to a local trivialization<br />

looks like<br />

P = ∑<br />

A α (x) ∂α<br />

∂x . α<br />

|α|≤k<br />

Here C ∞ (M,S) denotes the space of smooth sections of S → M, α =<br />

(α 1 ,...,α m ) ∈ N 0 ×···×N 0 runs over multi-indices, |α| = ∑ m<br />

j=1 α j <strong>and</strong><br />

∂ α<br />

∂<br />

= |α|<br />

∂x α ∂(x 1 ) α 1 ···∂(x m ) .Theprincipal symbol σ αm P of P associates to each<br />

covector ξ ∈ Tx ∗ M a linear map σ P (ξ) :S x → S x . Locally, it is given by<br />

σ P (ξ) = ∑<br />

A α (x)ξ α ,<br />

|α|=k<br />

where ξ α = ξ α 1<br />

1 ···ξα m m <strong>and</strong> ξ = ∑ j ξ jdx j .IfP <strong>and</strong> Q are two differential<br />

operators of order k <strong>and</strong> l respectively, then Q ◦ P is a differential operator<br />

of order k + l <strong>and</strong><br />

σ Q◦P (ξ) =σ Q (ξ) ◦ σ P (ξ).<br />

For any linear differential operator P : C ∞ (M,S) → C ∞ (M,S) thereisa<br />

unique formally dual operator P ∗ : C ∞ (M,S ∗ ) → C ∞ (M,S ∗ )ofthesame<br />

order characterized by ∫ ∫<br />

〈ϕ, P ψ〉 dV = 〈P ∗ ϕ, ψ〉 dV<br />

M<br />

M<br />

for all ψ ∈ C ∞ (M,S) <strong>and</strong>ϕ ∈ C ∞ (M,S ∗ ) with supp(ϕ) ∩ supp(ψ) compact.<br />

Here 〈·, ·〉 : S ∗ ⊗ S → K denotes the canonical pairing, i.e., the evaluation of<br />

a linear form in Sx ∗ on an element of S x ,wherex ∈ M. Wehaveσ P ∗(ξ) =<br />

(−1) k σ P (ξ) ∗ where k is the order of P .<br />

Definition 3.5. Let a vector bundle S → M be endowed with a non-degenerate<br />

inner product 〈· , ·〉. A linear differential operator P on S is called formally<br />

self-adjoint if <strong>and</strong> only if<br />

∫<br />

∫<br />

〈Pϕ,ψ〉 dV = 〈ϕ, P ψ〉 dV<br />

M<br />

holds for all ϕ, ψ ∈ C ∞ (M,S) with supp(ϕ) ∩ supp(ψ) compact.<br />

Similarly, we call P formally skew-adjoint if instead<br />

∫<br />

∫<br />

〈Pϕ,ψ〉 dV = − 〈ϕ, P ψ〉 dV .<br />

M<br />

We recall the definition of advanced <strong>and</strong> retarded Green’s operators for<br />

a linear differential operator.<br />

Definition 3.6. Let P be a linear differential operator acting on the sections<br />

of a vector bundle S over a Lorentzian manifold M. Anadvanced Green’s<br />

operator for P on M is a linear map<br />

G + : Cc<br />

∞ (M,S) → C ∞ (M,S)<br />

M<br />

M

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