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Some Aspects of the de Sitter/CFT Correspondence
High Energy Physics - Theory · Submitted 26 Jun 2001
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Requiring the pressure to be positive yields an upper bound for the black hole mass, given by the mass of the Nariai solution.
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The abstract, sentence by sentence
We discuss several aspects of the proposed correspondence between quantum gravity on de Sitter spaces and Euclidean conformal field theories. The central charge appearing in the asymptotic symmetry algebra of three-dimensional de Sitter space is derived both from the conformal anomaly and the transformation law of the CFT stress tensor when going from dS_3 in planar coordinates to dS_3 with cosmological horizon. The two-point correlator for CFT operators coupling to bulk scalars is obtained in static coordinates, corresponding to a CFT on a cylinder. Correlation functions are also computed for CFTs on two-dimensional hyperbolic space. We furthermore determine the energy momentum tensor and the Casimir energy of the conformal field theory dual to the Schwarzschild-de Sitter solution in five dimensions. Requiring the pressure to be positive yields an upper bound for the black hole mass, given by the mass of the Nariai solution. Beyond that bound, which is similar to the one found by Strominger requiring the conformal weights of CFT operators to be real, one encounters naked singularities.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We discuss several aspects of the proposed correspondence between quantum gravity on de Sitter spaces and Euclidean conformal field theories. | contribution 0.68 | 0.70 | 0.09 | asserted 0.47 |
| s1 | The central charge appearing in the asymptotic symmetry algebra of three-dimensional de Sitter space is derived both from the conformal anomaly and the transformation law of the CFT stress tensor when going from dS_3 in planar coordinates to dS_3 with cosmological horizon. | result 0.80 | 0.90 | 0.20 | asserted 1.00 |
| s2 | The two-point correlator for CFT operators coupling to bulk scalars is obtained in static coordinates, corresponding to a CFT on a cylinder. | result 0.76 | 0.92 | 0.05 | asserted 1.00 |
| s3 | Correlation functions are also computed for CFTs on two-dimensional hyperbolic space. | result 0.67 | 0.89 | 0.04 | asserted 1.00 |
| s4 | We furthermore determine the energy momentum tensor and the Casimir energy of the conformal field theory dual to the Schwarzschild-de Sitter solution in five dimensions. | result 0.66 | 0.94 | 0.11 | asserted 1.00 |
| s5 | Requiring the pressure to be positive yields an upper bound for the black hole mass, given by the mass of the Nariai solution. | result 0.99 | 0.86 | 0.18 | asserted 1.00 |
| s6 | Beyond that bound, which is similar to the one found by Strominger requiring the conformal weights of CFT operators to be real, one encounters naked singularities. | interpretation 0.53 | 0.55 | 0.22 | asserted 0.99 |
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The paper
Original abstract
We discuss several aspects of the proposed correspondence between quantum gravity on de Sitter spaces and Euclidean conformal field theories. The central charge appearing in the asymptotic symmetry algebra of three-dimensional de Sitter space is derived both from the conformal anomaly and the transformation law of the CFT stress tensor when going from dS_3 in planar coordinates to dS_3 with cosmological horizon. The two-point correlator for CFT operators coupling to bulk scalars is obtained in static coordinates, corresponding to a CFT on a cylinder. Correlation functions are also computed for CFTs on two-dimensional hyperbolic space. We furthermore determine the energy momentum tensor and the Casimir energy of the conformal field theory dual to the Schwarzschild-de Sitter solution in five dimensions. Requiring the pressure to be positive yields an upper bound for the black hole mass, given by the mass of the Nariai solution. Beyond that bound, which is similar to the one found by Strominger requiring the conformal weights of CFT operators to be real, one encounters naked singularities.
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20 arXiv papers cite this in 36 sentences
Papers citing it · 20 sentences without a confident label
Compares with it 3 papers
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This average is given by [equation] finally obtaining [equation] Thereby, the central charge in the large $q-$limit corresponds [equation] exactly as has been previously derived in the dS$_3$/CFT$_2$ correspondence [ref] .
de Sitter Entanglement and Conformal Description of the Cosmological Horizon · dS$_3$ holography from $4$ dimensions · 0.93
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As we shall see, the total central charge of the two boundaries reproduces exactly the central charge derived in the context of the dS$_3$/CFT$_2$ correspondence [ref] .
Liouville description of conical defects in dS$_4$, Gibbons-Hawking entropy as modular entropy, and dS$_3$ holography · Introduction · 0.90
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The value of the central charge agrees with [ref] and is imaginary for the dual CFT of dS$_3$, as mentioned above.
Aspects of dS/CFT Holography · Central Charge in dS$_3$ · 0.95
Cites it as background 13 papers
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According to the dS/CFT correspondence [ref] , its precursors [ref] and refinements [ref] , the microscopic degrees of freedom giving rise to the dS entropy are encoded within a dual Euclidean conformal field theory located at the boundary of global dS space.
De Sitter Space and Entanglement · The problem of de Sitter entropy · 0.87
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In comparison to AdS/CFT's brane-dynamical constructuring [ref] and prosperous developing [ref] , dS/CFT [ref] especially dS/CFTe has never been implemented/invented top-downly and has been only rarely(relative to AdS/CFT) explored in string communities due to the difficulty of de Sitter vaccum's brane-constructuring [ref] .
Emergent time axis from statistic/gravity dualities · Basic ideals on emergent space-time · 0.87
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Some papers have proposed the dS/CFT correspondence, which describes that quantum gravity in de Sitter space is dual to CFT living on the past and future boundaries of de Sitter space [ref] , where the masses of the stable scalar make the conformal weights become complex, hence the boundary CFT is non-unitary.
Pole-skipping in two-dimensional de Sitter spacetime and double-scaled SYK model · Introduction · 0.90
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