For Differential Equations > s.a. fokker-planck
equation; Propagator; wave equations.
$ Def: For a second-order linear differential operator L, the symmetric 2-point function G satisfying
L G(x, x') = δ(x–x') ;
Notice that a given operator L has many Green functions, depending
on the boundary conditions imposed on the solution.
* Applications: Used to find solutions of the de Lφ = j, given the source j and the boundary conditions on the field φ, i.e., to propagate the field; It is thus also called propagator.
* Specific types of equations: For the Laplacian L = ∇2, the Green function is G(x, x') = 1 / |x – x'|; This applies to electrostatics and Newtonian gravity.
@ Specific types of equations: Haba JPA(04)ht, JMP(05)mp [strongly inhomogeneous media, singular coefficients]; Tyagi JPA(05) [Poisson, periodic boundary conditions]; Moroz JPA(06)mp [Helmholtz and Laplace, quasi-periodic]; Franklin a1202 [for Neumann boundary conditions].
@ For non-linear equations: Frasca MPLA(07)ht/07 [and quantum field theory applications]; Frasca IJMPA(08)-a0704 [short-time expansion].
> Online resources: see Wikipedia page.
For Classical Field Theory > s.a. gravitational radiation; huygens principle [tails].
* Interpretation: The Green function G(x, x') is the field produced at x by a unit-strength point source at a given point x'.
* In electrodynamics: It is used to write the electrostatic potential as
φ(x) = ∫V dv' ρ(x') G(x, x') + (1/4π) ∫∂(V) da' · (G ∇'φ – φ ∇'G) .
@ General references: Green 1828-a0807;
in Morse & Feschbach 53; Barton 89; Cornwall et al 11 [gauge theories, pinch technique]; in Alastuey et al 16.
@ In curved spacetime: Waylen PRS(78) [early universe, singular and regular terms]; Molnár CQG(01)gq [electrostatic, in Schwarzschild spacetime]; Higuchi & Lee PRD(08)-a0807, Higuchi et al PRD(09) [retarded, in de Sitter space]; Esposito & Roychowdhury IJGMP(09) [spin-1/2 and 3/2, de Sitter space]; Chu & Starkman PRD(11)-a1108 [scalar, photon and graviton retarded Green's functions in perturbed spacetimes, perturbation theory]; Kazinski a1211 [stationary, slowly-varying spacetime]; > s.a. klein-gordon fields in curved spacetime [Kerr spacetime].
@ Discrete: Xu & Yau JCTA(13) [Chung-Yau's discrete Green function]; Ray a1409 [exact Green functions on lattices].
For Other Classical Systems > see Kadanoff-Baym Equations [transport].
For Quantum Systems > s.a. feynman
propagator; green functions in quantum field theory; quantum
@ References: Tsaur & Wang AJP(06)jul [Schrödinger equation]; Miyazawa JPA(06) [1D, in terms of reflection coefficients]; Brouder et al PRL(09) [many-body degenerate systems].
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