1990
DOI: 10.1007/bf02102088
|View full text |Cite
|
Sign up to set email alerts
|

Local quasiequivalence and adiabatic vacuum states

Abstract: The problem of determining the physically relevant states acquires a new dimension in curved spacetime where there is, in general, no natural definition of a vacuum state. It is argued that there is a unique local quasiequivalence class of physically relevant states and it is shown how this class can be specified for the free Klein-Gordon field on a Robertson-Walker spacetime by using the concept of an adiabatic vacuum state. Any two adiabatic vacuum states of order two are locally quasiequivalent.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

7
210
0

Year Published

2002
2002
2016
2016

Publication Types

Select...
5
4

Relationship

0
9

Authors

Journals

citations
Cited by 102 publications
(219 citation statements)
references
References 18 publications
7
210
0
Order By: Relevance
“…Here this question of integrability of modes over the spectrum is settled by showing that the suitably chosen mode solutions remain well under control even at non positive spectral values. As an example of application and as a byproduct the explicit formula of the propagator of the field in the Fourier space is found, which generalizes one obtained in [5].…”
Section: Introductionsupporting
confidence: 65%
“…Here this question of integrability of modes over the spectrum is settled by showing that the suitably chosen mode solutions remain well under control even at non positive spectral values. As an example of application and as a byproduct the explicit formula of the propagator of the field in the Fourier space is found, which generalizes one obtained in [5].…”
Section: Introductionsupporting
confidence: 65%
“…those introduced by Parker [19] in order to minimise particle creation (see also [20] for a derivation of the expectation values of the stress tensor). Much work has been done also recently in order to make the definition of these states precise [21,22,23]. In order to write the two-points function of these states we follow the construction as in Parker [19].…”
Section: A Adiabatic States and Large Mass Expansionmentioning
confidence: 99%
“…noting from Lemma 3.2 of [4] that (n+1) k ∈ S −2n−2 and remembering that ω k := (k 2 /a 2 + m 2 ) 1/2 is the leading term in the asymptotic expansion of Ω (n) k for any n we find for (138) the principal symbol 1 4…”
Section: E2 Correction Of Theorem 324mentioning
confidence: 66%
“…E1) we restrict ourselves to the spatially compact case: Proof. The statement of the theorem is a consequence of Theorems 4.7 and 6.3 in [2] and Theorem 3.3 in [4]. For clarity's sake, however, we indicate the necessary corrections and modifications in the proof of Theorem 3.24.…”
Section: E2 Correction Of Theorem 324mentioning
confidence: 99%