Abstract:The solvable Bianchi I-VII groups which arise as homogeneity groups in cosmological models are analyzed in a uniform manner. The dual spaces (the equivalence classes of unitary irreducible representations) of these groups are computed explicitly. It is shown how parameterizations of the dual spaces can be chosen to obtain explicit Plancherel formulas. The Laplace operator ∆ arising from an arbitrary left invariant Riemannian metric on the group is considered, and its spectrum and eigenfunctions are given expli… Show more
“…Although the results of the previous section are explicit (if one follows closely the details in [7,8]), they are quite complicated. In certain particular cases it might be easier to rely on some direct treatment, as [2].…”
Section: The Connected Simply Connected Solvable Bianchi Groupsmentioning
confidence: 99%
“…Then the Lie bracket is [(α, β; γ), (α ′ , β ′ ; γ ′ )] = γM (α ′ , β ′ ) − γ ′ M (α, β); 0 . From now on we shall rely on results from [2], in which the authors found easier to apply directly Mackey's induced representation theory for semidirect product than the parametrization methods of Currey. The emphasis is on the orbit structure of the contragredient action M ⊥ of R on the dual R 2 ≡ R 2 .…”
Section: The Connected Simply Connected Solvable Bianchi Groupsmentioning
confidence: 99%
“…The (1-dimensional) algebraic submanifolds Σ , composed of one or several connected components, and its relevant measures dρ(σ) = ρ(σ)dσ, will be indicated below, via a parametrization, case by case. The generic classes of irreducible representations can all be realized on the Hilbert space H σ = L 2 (R) as To be more specific, one has to invoke the Bianchi classification [15,25] and results describing the parametrization spaces from [2]. It can be shown that two such semi-direct product Lie algebras given respectively by M where q = 0, −1 and p ≥ 0 , with corresponding group actions e tM IV = e t 0 te t e t , e tM V = e t 0 0 e t , e tM (q) VI = e t 0 0 e −qt , e tM (p) VII = e pt cos t −e pt sin t e pt sin t e pt cos t .…”
Section: The Connected Simply Connected Solvable Bianchi Groupsmentioning
confidence: 99%
“…The densities γ are indicated up to a strictly positive constant. Details, including more formulae and a picture of the orbits and of the cross-sections Σ , can be found in [2]; they help to understand the splittings. The results are roughly compatible with Currey's theory.…”
Section: The Connected Simply Connected Solvable Bianchi Groupsmentioning
In recent papers and books, a global quantization has been developed for unimodular groups of type I . It involves operator-valued symbols defined on the product between the group G and its unitary dual G , composed of equivalence classes of irreducible representations. For compact or for graded Lie groups, this has already been developed into a powerful pseudo-differential calculus. In the present article we extend the formalism to arbitrary locally compact groups of type I , making use of the Fourier theory of non-unimodular second countable groups. The unitary dual and its Plancherel measure being quite abstract in general, we put into evidence situations in which concrete forms are available. Kirillov theory and parametrizations of large parts of G allow rewriting the basic formulae in a manageable form. Some examples of completely solvable groups are worked out. * 2010 Mathematics Subject Classification: Primary 46L65, 47G30, Secondary 22D10, 22D25.
“…Although the results of the previous section are explicit (if one follows closely the details in [7,8]), they are quite complicated. In certain particular cases it might be easier to rely on some direct treatment, as [2].…”
Section: The Connected Simply Connected Solvable Bianchi Groupsmentioning
confidence: 99%
“…Then the Lie bracket is [(α, β; γ), (α ′ , β ′ ; γ ′ )] = γM (α ′ , β ′ ) − γ ′ M (α, β); 0 . From now on we shall rely on results from [2], in which the authors found easier to apply directly Mackey's induced representation theory for semidirect product than the parametrization methods of Currey. The emphasis is on the orbit structure of the contragredient action M ⊥ of R on the dual R 2 ≡ R 2 .…”
Section: The Connected Simply Connected Solvable Bianchi Groupsmentioning
confidence: 99%
“…The (1-dimensional) algebraic submanifolds Σ , composed of one or several connected components, and its relevant measures dρ(σ) = ρ(σ)dσ, will be indicated below, via a parametrization, case by case. The generic classes of irreducible representations can all be realized on the Hilbert space H σ = L 2 (R) as To be more specific, one has to invoke the Bianchi classification [15,25] and results describing the parametrization spaces from [2]. It can be shown that two such semi-direct product Lie algebras given respectively by M where q = 0, −1 and p ≥ 0 , with corresponding group actions e tM IV = e t 0 te t e t , e tM V = e t 0 0 e t , e tM (q) VI = e t 0 0 e −qt , e tM (p) VII = e pt cos t −e pt sin t e pt sin t e pt cos t .…”
Section: The Connected Simply Connected Solvable Bianchi Groupsmentioning
confidence: 99%
“…The densities γ are indicated up to a strictly positive constant. Details, including more formulae and a picture of the orbits and of the cross-sections Σ , can be found in [2]; they help to understand the splittings. The results are roughly compatible with Currey's theory.…”
Section: The Connected Simply Connected Solvable Bianchi Groupsmentioning
In recent papers and books, a global quantization has been developed for unimodular groups of type I . It involves operator-valued symbols defined on the product between the group G and its unitary dual G , composed of equivalence classes of irreducible representations. For compact or for graded Lie groups, this has already been developed into a powerful pseudo-differential calculus. In the present article we extend the formalism to arbitrary locally compact groups of type I , making use of the Fourier theory of non-unimodular second countable groups. The unitary dual and its Plancherel measure being quite abstract in general, we put into evidence situations in which concrete forms are available. Kirillov theory and parametrizations of large parts of G allow rewriting the basic formulae in a manageable form. Some examples of completely solvable groups are worked out. * 2010 Mathematics Subject Classification: Primary 46L65, 47G30, Secondary 22D10, 22D25.
“…The set of spacetimes with homogeneous Cauchy hypersurfaces encompasses the well known Bianchi spacetimes [19]. Hadamard states were recently constructed on these spacetimes by the authors of [20]. We will briefly comment on examples of spacetimes whose Cauchy hypersurfaces are compact and homogeneous.…”
Abstract. We construct states on the algebra of the Klein-Gordon field that minimize the energy density in homogeneous and in inhomogeneous spacetimes, both with compact Cauchy hypersurfaces. The energy density is measured by geodesic observers and smeared over a spacelike slab of spacetime, entirely containing a Cauchy hypersurface and extended in time. We further show that these states are Hadamard states. The present construction generalizes the construction of States of Low Energy in Robertson-Walker spacetimes presented by Olbermann [1].
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.
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