Abstract:The methods of mode decomposition and Fourier analysis of classical and quantum fields on curved spacetimes previously available mainly for the scalar field on Friedman-Robertson-Walker (FRW) spacetimes are extended to arbitrary vector bundle fields on general spatially homogeneous spacetimes. This is done by developing a rigorous unified framework which incorporates mode decomposition, harmonic analysis and Fourier analysis. The limits of applicability and uniqueness of mode decomposition by separation of the… Show more
“…In the second part of the second section, we will specify the introduced notions to the case of a spatially flat FRW background. That is, based on former results by Lüders & Roberts [37] and Schlemmer [46] on the mode decomposition of homogeneous and isotropic states as well as their renormalization, as described by Eltzner & Gottschalk [18], we explicitly calculate the renormalized quantized EMT for homogeneous and isotropic Hadamard (HIH) states in terms of a plane wave mode decomposition − note that a similar mode decomposition for states of spin-0 and spin-1 fields on homogeneous spacetimes was recently achieved by Avetisyan [1] and Avetisyan & Verch [2].…”
In this paper we try to answer the question whether the quantized free scalar field on a spatially flat Friedmann-Robertson-Walker (FRW) spacetime is a matter model that can induce a Chaplygin gas equation of state. For this purpose we first describe how one can obtain every possible homogeneous and isotropic Hadamard (HIH) state once any such state is given. We also identify a condition on the scale factor sufficient to entail the existence of a simple HIH state − this state is constructed explicitly and can thence be used as a starting point for constructing all HIH states. Furthermore, we employ these results to show that on an FRW spacetime with nonpositive constant scalar curvature there is, with one exception, no Chaplygin gas equation of state compatible with any HIH state. Finally, we argue that the semi-classical Einstein equation and the Chaplygin gas equation of state can presumably not be consistently solved for the quantized free scalar field.
“…In the second part of the second section, we will specify the introduced notions to the case of a spatially flat FRW background. That is, based on former results by Lüders & Roberts [37] and Schlemmer [46] on the mode decomposition of homogeneous and isotropic states as well as their renormalization, as described by Eltzner & Gottschalk [18], we explicitly calculate the renormalized quantized EMT for homogeneous and isotropic Hadamard (HIH) states in terms of a plane wave mode decomposition − note that a similar mode decomposition for states of spin-0 and spin-1 fields on homogeneous spacetimes was recently achieved by Avetisyan [1] and Avetisyan & Verch [2].…”
In this paper we try to answer the question whether the quantized free scalar field on a spatially flat Friedmann-Robertson-Walker (FRW) spacetime is a matter model that can induce a Chaplygin gas equation of state. For this purpose we first describe how one can obtain every possible homogeneous and isotropic Hadamard (HIH) state once any such state is given. We also identify a condition on the scale factor sufficient to entail the existence of a simple HIH state − this state is constructed explicitly and can thence be used as a starting point for constructing all HIH states. Furthermore, we employ these results to show that on an FRW spacetime with nonpositive constant scalar curvature there is, with one exception, no Chaplygin gas equation of state compatible with any HIH state. Finally, we argue that the semi-classical Einstein equation and the Chaplygin gas equation of state can presumably not be consistently solved for the quantized free scalar field.
“…This construction has been generalised to encompass almost equilibrium states in [Ku08] and expanding spacetimes with less symmetry in [TB13]. Noteworthy in this context is the thorough analysis of the mode expansion presented in [Av14].…”
Section: Let O ⊂ R N Be An Open Set and Vmentioning
“…where x = (t, x), y = (t ′ , y) while j = 1, 2 is introduced to distinguish between the values m 1 and m 2 of the mass, which are our starting and arrival point respectively. Here each ψ k is an eigenfunction of the positive elliptic operator K, that is Kψ k = λ 2 k ψ k , λ k ∈ R and dµ(k) is a suitable spectral measure -see [Ave14]. At the same time each T k,j (t) obeys to the ODE:…”
Section: The Adiabatic Limit On Static Spacetimes -Sufficient Conditionsmentioning
We consider real scalar field theories whose dynamics is ruled by normally hyperbolic operators differing only by a smooth potential V . By means of an extension of the standard definition of Møller operator, we construct an isomorphism between the associated spaces of smooth solutions and between the associated algebras of observables. On the one hand such isomorphism is non-canonical since it depends on the choice of a smooth time-dependant cut-off function. On the other hand, given any quasi-free Hadamard state for a theory with a given V , such isomorphism allows for the construction of another quasi-free Hadamard state for a different potential. The resulting state preserves also the invariance under the action of any isometry, whose associated Killing field commutes with the vector field built out of the normal vectors to a family of Cauchy surfaces, foliating the underlying manifold. Eventually we discuss a sufficient condition to remove on static spacetimes the dependence on the cut-off via a suitable adiabatic limit.Keywords: quantum field theory on curved backgrounds, Hadamard sates, Møller operator MSC: 81T20, 81T05
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.