Bogoliubov Transformations  

In General [> s.a. quantum field theory in curved spacetime].
* Idea: A transformation between one set of pure frequency modes (c.o.n.s. of solutions of a field equation, or Fock space structure for a quantum field theory) to another, in particular wrt two timelike (Killing) vector fields in quantum field theory (in curved spacetime).
$ Def: If the set of modes {ui} is associated with operators ai and ai, and {vi} with bi and bi, then

ai = j (ji bj + ji* bj) ,   bj = i (ji* aiji* ai) ,

where the coefficients are given by ij = (vi, uj), ij = –(vi, uj*), or

ui = j (ji* vjji vj*) ,   vj = i (ji ui + ji ui*) .

* Properties of the coefficients: For a Bosonic field we get, from orthonormality of modes and preservation of commutation relations, respectively,

k (ik jk* – ik jk*) = ij ,   k (ik jkik jk) = 0 .

* Fock spaces: The two Fock spaces are different if bij 0, and v-positive frequency modes contain u-negative frequency ones; e.g.,  0v | Nui | 0 = j |ji|2.

References
@ General: Bogoliubov JETP(58); Boonserm & Visser a0801 [bounds on coefficients].
@ In curved spacetime: Parker PR(69); Lapedes JMP(78); Ruijsenaars AP(78); Woodhouse PRS(81); in Birrell & Davies 82; Bombelli & Wyrozumski CQG(89).


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