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Holographic Approach to Finite Temperature QCD: The Case of Scalar Glueballs and Scalar Mesons
High Energy Physics - Phenomenology · Submitted 8 Sep 2009
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim A consistent holographic description of in-medium effects on hadron properties should include the Hawking-Page transition, which separates the phase with the Anti-de Sitter metric at small temperatures from the phase with Anti-de Sitter-Black Hole metric at high temperatures.
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The abstract, sentence by sentence
We study scalar glueballs and scalar mesons at $T \neq 0$ in the soft wall holographic QCD model. We find that, using the Anti-de Sitter-Black Hole metric for all values of the temperature, the masses of the hadronic states decrease and the widths become broader when T increases, and there are temperatures for which the states disappear from the scalar glueball and scalar meson spectral functions. However, the values of the temperatures in correspondence of which such phenomena occur are low, of the order of 40-60 MeV. A consistent holographic description of in-medium effects on hadron properties should include the Hawking-Page transition, which separates the phase with the Anti-de Sitter metric at small temperatures from the phase with Anti-de Sitter-Black Hole metric at high temperatures.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study scalar glueballs and scalar mesons at $T \neq 0$ in the soft wall holographic QCD model. | contribution 1.00 | 0.90 | 0.04 | asserted 0.81 |
| s1 | We find that, using the Anti-de Sitter-Black Hole metric for all values of the temperature, the masses of the hadronic states decrease and the widths become broader when T increases, and there are temperatures for which the states disappear from the scalar glueball and scalar meson spectral functions. | result 1.00 | 0.95 | 0.64 | asserted 1.00 |
| s2 | However, the values of the temperatures in correspondence of which such phenomena occur are low, of the order of 40-60 MeV. | result 0.69 | 0.84 | 0.14 | asserted 1.00 |
| s3 | A consistent holographic description of in-medium effects on hadron properties should include the Hawking-Page transition, which separates the phase with the Anti-de Sitter metric at small temperatures from the phase with Anti-de Sitter-Black Hole metric at high temperatures. | limitation 0.36 | 0.15 | 0.25 | asserted 0.93 |
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The paper
Original abstract
We study scalar glueballs and scalar mesons at $T \neq 0$ in the soft wall holographic QCD model. We find that, using the Anti-de Sitter-Black Hole metric for all values of the temperature, the masses of the hadronic states decrease and the widths become broader when T increases, and there are temperatures for which the states disappear from the scalar glueball and scalar meson spectral functions. However, the values of the temperatures in correspondence of which such phenomena occur are low, of the order of 40-60 MeV. A consistent holographic description of in-medium effects on hadron properties should include the Hawking-Page transition, which separates the phase with the Anti-de Sitter metric at small temperatures from the phase with Anti-de Sitter-Black Hole metric at high temperatures.
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References
How the literature uses it
39 arXiv papers cite this in 69 sentences
Papers citing it · 35 sentences without a confident label
Contests it 1 paper
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Further studies in [ref] on refinements of this model found, however, unrealistic melting temperatures much below the QCD deconfinement scale $𝒪([150]MeV)$.
A quantum information perspective on meson melting · Insights from holographic models · contest 0.78
Builds on it 4 papers
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In this section, we will describe the extension of the predictive AdS/QCD model [ref] to a thermodynamic model by simply considering the black hole metric [ref] .
Thermal Mass Spectra of Vector and Axial-Vector Mesons in Predictive Soft-Wall AdS/QCD Model · Predictive AdS/QCD Model at Finite Temperature · 0.99
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This mimics the scenario considered in [ref] , but we include the full back-reaction of the scalar field and take the Gibbons-Hawking term into account.
The Dynamics and Thermodynamics of Soft-Wall AdS/QCD · Deconfinement Temperature · 0.86
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This mimics the scenario considered in [ref] , but we include the full back-reaction of the scalar field and take the Gibbons-Hawking term into account.
The Thermodynamics of a 5D Gravity-Dilaton-Tachyon Solution · Deconfinement Temperature · 0.93
Uses its method or tool 4 papers
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However, fortunately, as was discussed in [ref] , if it is possible to tackle the problem of obtaining masses by considering that the horizon is at a long distance from the border, and modes dual to hadrons decrease to zero far from the horizon, then it is also possible to solve ([ref]) considering normalized modes and using the usual tools to solve Sturm-Liouville problems.
Effects of beta function on mass and melting temperature for scalar glueballs in AdS/QCD models at finite temperature · Model at finite temperature · 0.87
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In order to extract the dependence of glueball masses on the temperature and chemical potential, we have fitted each peak with a deformed Breit-Wigner function [ref] :
In-medium hadronic spectral functions through the soft-wall holographic model of QCD · Scalar glueball spectral function · 1.00
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To quantitatively extract the temperature and chemical potential dependence of the lightest oddball mass, we fit the peak in the spectral function $ρ(ω^2)$ using a Breit-Wigner-like expression [ref] :
Holographic Oddballs · Oddballs in medium · 1.00
Uses its data or values 2 papers
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In Ref. [ref] , the scalar glueball and light scalar mesons spectral have been studied in the soft-wall model and the highest temperature for which the meson state can exist was found to be about $40-60$.
Thermal Mass Spectra of Scalar and Pseudo-Scalar Mesons in IR-improved Soft-Wall AdS/QCD Model with Finite Chemical Potential · Introduction · 0.89
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In [ref] , the melting temperature of the scalar glueball from the spectral functions is about $40-60$ MeV, while the deconfinement temperature of the soft wall model is about $190$ MeV [ref] .
Holography at work for nuclear and hadron physics · Glueballs · 0.90
Compares with it 4 papers
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This criterion gives the same dissociation temperature at $μ=0$ found in [ref] , namely $T∼0.116c$.
In-medium hadronic spectral functions through the soft-wall holographic model of QCD · Scalar glueball spectral function · 0.81
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However, the melting temperature in this model is higher than in previous holographic meson melting models, which find all sharp peaks disappearing at temperatures of 30-60 MeV [ref] .
Chiral transition and meson melting within improved holographic soft wall models · Temperature effects · 1.00
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Similar results were recently obtained for scalar [ref] and vector [ref] mesons in the soft-wall model.
Glueballs at finite temperature from AdS/QCD · Final comments · 0.88
Cites it as background 14 papers
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The spectral function in the soft-wall model was calculated for vector mesons in [ref] and for scalar glueballs and scalar mesons in [ref] .
Vector meson quasinormal modes in a finite-temperature AdS/QCD model · Introduction · 0.87
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The investigation of hadron dissociation in a thermal medium in the framework of holography was carried out, for instance, in Refs. [ref] , see also references therein.
Melting of heavy vector mesons and quasinormal modes in a finite density plasma from holography · Introduction · 0.93
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The thermal spectral functions for both mesons and glueballs have been studied in the soft-wall model, and the meson melting properties such as the in-medium mass shift have also been investigated [ref] .
Chiral transition and meson melting with finite chemical potential in an improved soft-wall AdS/QCD Model · Introduction · 0.89
What it cites · 2 sentences without a confident label
Compares with 1 paper
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It is qualitatively analogous to the behaviour of the scalar glueball mass and width observed in lattice studies [ref] : however, the temperature scale is very different.
A Quenched Study of SU(3) Glueballs at Finite Temperature · Scalar glueball at $T ≠0$: soft wall model with AdS-BH metric · 1.00
Cites as background 1 paper
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The theoretical tools used to describe these phenomena are lattice QCD, QCD Sum Rules, effective QCD theories and models of QCD [ref] .
Heavy quarkonium correlators at finite temperature: QCD sum rule approach · Introduction · 0.83
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