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Proof of a universal lower bound on the shear viscosity to entropy density ratio
High Energy Physics - Theory · Submitted 11 Aug 2009
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Here, we prove the bound for any ghost-free extension of Einstein gravity and the field-theory dual thereof.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
It has been conjectured, on the basis of the gauge-gravity duality, that the ratio of the shear viscosity to the entropy density should be universally bounded from below by 1/ 4 pi in units of the Planck constant divided by the Boltzmann constant. Here, we prove the bound for any ghost-free extension of Einstein gravity and the field-theory dual thereof. Our proof is based on the fact that, for such an extension, any gravitational coupling can only increase from its Einstein value. Therefore, since the shear viscosity is a particular gravitational coupling, it is minimal for Einstein gravity. Meanwhile, we show that the entropy density can always be calibrated to its Einstein value. Our general principles are demonstrated for a pair of specific models, one with ghosts and one without.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | It has been conjectured, on the basis of the gauge-gravity duality, that the ratio of the shear viscosity to the entropy density should be universally bounded from below by 1/ 4 pi in units of the Planck constant divided by the Boltzmann constant. | background 1.00 | 0.03 | 0.07 | speculative 0.98 |
| s1 | Here, we prove the bound for any ghost-free extension of Einstein gravity and the field-theory dual thereof. | contribution 0.72 | 0.96 | 0.85 | asserted 1.00 |
| s2 | Our proof is based on the fact that, for such an extension, any gravitational coupling can only increase from its Einstein value. | method 0.88 | 0.56 | 0.08 | asserted 0.95 |
| s3 | Therefore, since the shear viscosity is a particular gravitational coupling, it is minimal for Einstein gravity. | result 0.54 | 0.74 | 0.32 | asserted 1.00 |
| s4 | Meanwhile, we show that the entropy density can always be calibrated to its Einstein value. | result 0.53 | 0.92 | 0.06 | asserted 1.00 |
| s5 | Our general principles are demonstrated for a pair of specific models, one with ghosts and one without. | method 0.51 | 0.90 | 0.03 | asserted 1.00 |
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The paper
Original abstract
It has been conjectured, on the basis of the gauge-gravity duality, that the ratio of the shear viscosity to the entropy density should be universally bounded from below by 1/ 4 pi in units of the Planck constant divided by the Boltzmann constant. Here, we prove the bound for any ghost-free extension of Einstein gravity and the field-theory dual thereof. Our proof is based on the fact that, for such an extension, any gravitational coupling can only increase from its Einstein value. Therefore, since the shear viscosity is a particular gravitational coupling, it is minimal for Einstein gravity. Meanwhile, we show that the entropy density can always be calibrated to its Einstein value. Our general principles are demonstrated for a pair of specific models, one with ghosts and one without.
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References
How the literature uses it
8 arXiv papers cite this in 15 sentences
Papers whose main result relates to this one's
States a conflicting result 2 papers
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In these theories therefore there is no lower bound for the shear viscosity to entropy density ratio, in contrast to the predictions coming from the AdS/CFT correspondence.
Viscosity to entropy density ratio: violation of the lower bound at small temperatures · 0.95
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The resulting ratio can take on values above or below 1/4\pi\ and is consistent with all the previous calculations, even though our reasoning is substantially different.
Papers citing it · 11 sentences without a confident label
Uses its method or tool 1 paper
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The most convenient way to evaluate it is, as explained in [ref] and reviewed in Appendix B, to use a particular choice of field redefinition.
Non-perturbative unitarity constraints on the ratio of shear viscosity to entropy density in UV complete theories with a gravity dual · Calculating the ratio $η/s$ · 0.97
Cites it as background 3 papers
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Let us recall the relevant discussion from [ref] .
Unitarity constraints on the ratio of shear viscosity to entropy density in higher derivative gravity · General arguments · 0.90
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A great progress alone this line appeared several months ago when the authors of [ref] gave a proof for the existence of a universal bound of $η/s$ for any ghost-free extension of Einstein theory.
The Quantum Viscosity Bound In Lovelock Gravity · Introduction · 0.81
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These findings led to a series of new works, see e.g. [ref] related to Lovelock gravity.
Shock waves and Birkhoff's theorem in Lovelock gravity · introduction · 0.85
What it cites · 14 sentences without a confident label
Uses the method or tool of 6 papers
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For a general theory$X$that extends Einstein gravity, the entropy is given by Wald's formula [ref] and can be expressed as a correction to the Einstein value: S_X = V_ r_h^p/4G_X = V_ r_h^p/4G_E+λδG + O[λ^2] .$
Black Hole Entropy is Noether Charge · Introduction · 0.93
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For a general theory$X$that extends Einstein gravity, the entropy is given by Wald's formula [ref] and can be expressed as a correction to the Einstein value: S_X = V_ r_h^p/4G_X = V_ r_h^p/4G_E+λδG + O[λ^2] .$
On Black Hole Entropy · Introduction · 0.93
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For a general theory$X$that extends Einstein gravity, the entropy is given by Wald's formula [ref] and can be expressed as a correction to the Einstein value: S_X = V_ r_h^p/4G_X = V_ r_h^p/4G_E+λδG + O[λ^2] .$
Some Properties of Noether Charge and a Proposal for Dynamical Black Hole Entropy · Introduction · 0.93
Cites as support 1 paper
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For a ghost-free theory, all of the couplings must remain positive at all energy scales [ref] ; meaning that the propagator can only increase relative to its Einstein value.
Predictive Power of Strong Coupling in Theories with Large Distance Modified Gravity · Introduction · 0.98
Cites as background 8 papers
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Kovtun, Son and Starinets (KSS) have proposed that the ratio of the shear viscosity $η$ to the entropy density $s$ should be universally bounded from below by $1/4π$ in units of the Planck constant divided by the Boltzmann constant $ħ/k_B$ [ref] .
Viscosity in Strongly Interacting Quantum Field Theories from Black Hole Physics · Introduction · 0.83
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The gauge–gravity duality [ref] provides a hydrodynamic description of strongly coupled field theories in terms of the hydrodynamics of a black brane in an asymptotically anti-de Sitter (AdS) spacetime [ref] .
Holography and hydrodynamics: diffusion on stretched horizons · Introduction · 0.98
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The gauge–gravity duality [ref] provides a hydrodynamic description of strongly coupled field theories in terms of the hydrodynamics of a black brane in an asymptotically anti-de Sitter (AdS) spacetime [ref] .
Large N Field Theories, String Theory and Gravity · Introduction · 0.98
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