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Hadron Resonance Mass Spectrum and Lattice QCD Thermodynamics
High Energy Physics - Phenomenology · Submitted 13 Mar 2003
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that the value of T_c for different quark masses agrees with lines of constant energy density in a hadron resonance gas.
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The abstract, sentence by sentence
We confront lattice QCD results on the transition from the hadronic phase to the quark--gluon plasma with hadron resonance gas and percolation models. We argue that for T < T_c the equation of state derived from Monte--Carlo simulations of (2+1) quark--flavor QCD can be well described by a hadron resonance gas. We examine the quark mass dependence of the hadron spectrum on the lattice and discuss its description in terms of the MIT bag model. This is used to formulate a resonance gas model for arbitrary quark masses which can be compared to lattice calculations. We finally apply this model to analyze the quark mass dependence of the critical temperature obtained in lattice calculations. We show that the value of T_c for different quark masses agrees with lines of constant energy density in a hadron resonance gas. For large quark masses a corresponding contribution from a glueball resonance gas is required.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We confront lattice QCD results on the transition from the hadronic phase to the quark--gluon plasma with hadron resonance gas and percolation models. | contribution 0.80 | 0.78 | 0.07 | asserted 0.81 |
| s1 | We argue that for T < T_c the equation of state derived from Monte--Carlo simulations of (2+1) quark--flavor QCD can be well described by a hadron resonance gas. | result 0.55 | 0.47 | 0.29 | hedged possibility 0.66 |
| s2 | We examine the quark mass dependence of the hadron spectrum on the lattice and discuss its description in terms of the MIT bag model. | method 0.51 | 0.74 | 0.04 | unclear 0.73 |
| s3 | This is used to formulate a resonance gas model for arbitrary quark masses which can be compared to lattice calculations. | method 0.81 | 0.83 | 0.06 | asserted 0.94 |
| s4 | We finally apply this model to analyze the quark mass dependence of the critical temperature obtained in lattice calculations. | contribution 0.75 | 0.89 | 0.09 | asserted 0.79 |
| s5 | We show that the value of T_c for different quark masses agrees with lines of constant energy density in a hadron resonance gas. | result 0.96 | 0.90 | 0.52 | asserted 1.00 |
| s6 | For large quark masses a corresponding contribution from a glueball resonance gas is required. | result 0.64 | 0.74 | 0.12 | asserted 0.90 |
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The paper
Original abstract
We confront lattice QCD results on the transition from the hadronic phase to the quark--gluon plasma with hadron resonance gas and percolation models. We argue that for T < T_c the equation of state derived from Monte--Carlo simulations of (2+1) quark--flavor QCD can be well described by a hadron resonance gas. We examine the quark mass dependence of the hadron spectrum on the lattice and discuss its description in terms of the MIT bag model. This is used to formulate a resonance gas model for arbitrary quark masses which can be compared to lattice calculations. We finally apply this model to analyze the quark mass dependence of the critical temperature obtained in lattice calculations. We show that the value of T_c for different quark masses agrees with lines of constant energy density in a hadron resonance gas. For large quark masses a corresponding contribution from a glueball resonance gas is required.
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References
How the literature uses it
43 arXiv papers cite this in 48 sentences
Papers whose main result relates to this one's
States the same result 1 paper
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Furthermore, it is shown that the quark mass dependence of the transition temperature can be understood in terms of lines of constant energy density in a resonance gas.
Lattice QCD at non-zero chemical potential and the resonance gas model · 0.90
Papers citing it · 31 sentences without a confident label
Compares with it 4 papers
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Furthermore, the peculiar shape of the non-diagonal correlator near $T_c$ (sharp dip and subsequent slow rise towards zero) can be interpreted when comparing it to the separate contributions of mesonic and baryonic states in a hadron resonance gas (HRG) calculation [ref] .
Are there hadronic bound states above the QCD transition temperature? · Results and conclusions · 0.86
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A similar picture one can see in the dependence of $T_c$ on the $mass(PS) ≈2m_q$ in [ref] .
Theory of the deconfinement process in QCD · The deconfining temperature $T_c$ for different hadronic systems · 0.92
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In particular we here study [equation] These ratios can also be calculated from the hadron resonance gas (HRG) [ref] , and we here use these results for a comparison with our data in the low temperature/confined regime.
Quark number susceptibilities at finite chemical potential from fugacity expansion · Quark number related observables from fugacity expansion · 0.92
Cites it as background 13 papers
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This approach is commonly known as the Hadron Resonance Gas (HRG) model [ref] .
Constraining the hadronic spectrum through QCD thermodynamics on the lattice · Introduction · 0.95
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Such investigations were carried out in the past by various authors, see [ref] and references therein, where the reader may find more details and results.
Limits on hadron spectrum from bulk medium properties · Introduction · 1.00
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The focus of this study is on the latter approach, which generally assumes that strongly interacting QCD matter attains thermal and chemical equilibrium at hadronization and models it as a hadron resonance gas (statistical thermal) [ref] .
Rapidity scan approach for net-baryon cumulants with a statistical thermal model · Introduction · 0.82
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