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Entropy of Quantum Fields in de Sitter Space-time

General Relativity and Quantum Cosmology · Submitted 15 Jun 2013

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim The entropy of the quantum fields on this Hilbert space have been calculated which is finite and invariant for all inertial observers on the de Sitter hyperboloid.

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arXiv ID1306.3575 (version 3)
Pith IDNOMISCP4, Pith's permanent record of this paper and its review
CitationM.V. Takook. "Entropy of Quantum Fields in de Sitter Space-time." arXiv:1306.3575 (2013). https://pith.science/paper/NOMISCP4
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What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.19 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.16 · compares with prior results 0.06 · mentions code or data availability 0.01.

The abstract, sentence by sentence

arXiv listing abstract v3. Results and the main claim are underlined; .

The quantum states or Hilbert spaces for the quantum field theory in de Sitter space-time are studied on ambient space formalism. In this formalism, the quantum states are only depended $(1)$ on the topological character of the de Sitter space-time, {\it i.e.} $\R \times S^3$, and $(2)$ on the homogeneous spaces which are used for construction of the unitary irreducible representation of de Sitter group. A compact homogeneous space is chosen in this paper. The unique feature of this homogeneous space is that its total number of quantum states, ${\cal N}$, is finite although the Hilbert space has infinite dimensions. It is shown that ${\cal N}$ is a continuous function of the Hubble constant $H$ and the eigenvalue of the Casimir operators of de Sitter group. The entropy of the quantum fields on this Hilbert space have been calculated which is finite and invariant for all inertial observers on the de Sitter hyperboloid.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 The quantum states or Hilbert spaces for the quantum field theory in de Sitter space-time are studied on ambient space formalism. contribution 0.73 0.76 0.04 asserted 0.96
s1 In this formalism, the quantum states are only depended $(1)$ on the topological character of the de Sitter space-time, {\it i.e.} $\R \times S^3$, and $(2)$ on the homogeneous spaces which are used for construction of the unitary irreducible representation of de Sitter group. background 0.54 0.23 0.07 asserted 1.00
s2 A compact homogeneous space is chosen in this paper. method 0.77 0.90 0.03 asserted 0.99
s3 The unique feature of this homogeneous space is that its total number of quantum states, ${\cal N}$, is finite although the Hilbert space has infinite dimensions. result 0.53 0.81 0.16 asserted 1.00
s4 It is shown that ${\cal N}$ is a continuous function of the Hubble constant $H$ and the eigenvalue of the Casimir operators of de Sitter group. result 0.99 0.88 0.15 asserted 1.00
s5 The entropy of the quantum fields on this Hilbert space have been calculated which is finite and invariant for all inertial observers on the de Sitter hyperboloid. result 1.00 0.91 0.66 asserted 1.00

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 1.00.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

The quantum states or Hilbert spaces for the quantum field theory in de Sitter space-time are studied on ambient space formalism. In this formalism, the quantum states are only depended $(1)$ on the topological character of the de Sitter space-time, {\it i.e.} $\R \times S^3$, and $(2)$ on the homogeneous spaces which are used for construction of the unitary irreducible representation of de Sitter group. A compact homogeneous space is chosen in this paper. The unique feature of this homogeneous space is that its total number of quantum states, ${\cal N}$, is finite although the Hilbert space has infinite dimensions. It is shown that ${\cal N}$ is a continuous function of the Hubble constant $H$ and the eigenvalue of the Casimir operators of de Sitter group. The entropy of the quantum fields on this Hilbert space have been calculated which is finite and invariant for all inertial observers on the de Sitter hyperboloid.

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How the literature uses it

7 arXiv papers cite this in 14 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 10 sentences without a confident label

Cites it as support 2 papers
Cites it as background 1 paper

What it cites · 77 sentences without a confident label

Uses the method or tool of 4 papers
  • By using the Bros-Fourier transformation [ref] , the quantum field operator in this notation is given by: [equation] . +a^†(ξ_T,ν)[(x.ξ_T)_+^-3/2+iν +e^iπ(-3/2+iν)(x.ξ_T)_-^-3/2+iν] }dμ(ξ_T),where $(x·ξ)_+={[ 0 x·ξ≤0; (x·ξ) x·ξ>0; ] .$ [ref] .

    Fourier analysis and holomorphic decomposition on the one-sheeted hyperboloid · Massive scalar field: plane waves · 1.00

  • The annihilation operator $a(ξ,ν)$ is a homogeneous function with degree $-3/2+iν$ a̱(ζξ_T,ν)=ζ^-3/2+iνa(ξ_T,ν).Here $T$ stands for an orbital basis of $C^+$. $dμ_T(ξ)$ is an invariant measure defined by [equation] where $i_Ξw_C^+$ denotes the $3$-form on $C^+$ obtained from the contraction of the vector field $Ξ$ with the volume form [equation] Bros et al. have presented two orbital basis [ref] ; the hyperbolic-type sub-manifold $T_4=T_4^+ ∪T_4^-$ defined by Ṯ^±_4={ ξ∈C^+; ξ^4=±m_H},which is invariant under $SO(1,3)$ group, and the spherical-type submanifold $T_0$ defined by Ṯ_0={ ξ∈C^+; ξ^0=m_H>0, ξ⃗.ξ⃗+ (ξ^4)^2= m_H^2},which is invariant under $SO(4)$ group.

    Two-point Functions and Quantum Fields in de Sitter Universe · Massive scalar field: plane waves · 0.97

  • Gibbons and Hawking have suggested to use the following relation [ref] : ḏ(-E)=TdS,instead of the equation ([ref]), and then we obtain: E̱=μ/π arctan( H/μ)=μ/π arctan( 2πT/μ).In the null curvature limit we have $(H=0=T)$, E̱=μ/π ∑_n^∞(-1)^n/2n+1( 2πT/μ)^2n+1=2T-μ/3( 2πT/μ)^3+... .In this limit, we obtain $E=0$, which is a logical result!

    Les Houches Lectures on De Sitter Space · Entropy in de Sitter space-time · 0.84

Cites as support 3 papers
  • These two Hilbert spaces $H_T_0$ and $H_T_4$, are unitary equivalent [ref] .

    Two-point Functions and Quantum Fields in de Sitter Universe · Massive scalar field: plane waves · 0.99

  • From the group theoretical point of view it is proved that the second part cannot be described by a rank-$2$ symmetric tensor field in the ambient space notation or Dirac $6$-cone formalism [ref] .

    Linear Weyl Gravity in de Sitter Universe · Entropy in de Sitter space-time · 0.98

  • From the group theoretical point of view it is proved that the second part cannot be described by a rank-$2$ symmetric tensor field in the ambient space notation or Dirac $6$-cone formalism [ref] .

    Conformal linear gravity in de Sitter space · Entropy in de Sitter space-time · 0.98

Cites as background 18 papers

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