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Chiral Symmetry Restoration at Nonzero Temperature in the SU(3) \times SU(3) Linear Sigma Model
Nuclear Theory · Submitted 4 Apr 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Taking the experimental values for the meson masses, however, the transition is crossover.
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The abstract, sentence by sentence
We study patterns of chiral symmetry breaking at zero temperature and its subsequent restoration at nonzero temperature within the $SU(3)_{r} \times SU(3)_{\ell}$ linear sigma model. Gap equations for the masses of the scalar and pseudoscalar mesons and the non-strange and strange quark condensates are systematically derived in the Hartree approximation via the Cornwall-Jackiw-Tomboulis formalism. In the chiral limit, the chiral symmetry restoring transition is found to be first order, as predicted by universality arguments. Taking the experimental values for the meson masses, however, the transition is crossover. The absence of the $U(1)_A$ anomaly is found to drive this transition closer to being first order. At large temperatures, the mixing angles between octet and singlet states approach ideal flavor mixing.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study patterns of chiral symmetry breaking at zero temperature and its subsequent restoration at nonzero temperature within the $SU(3)_{r} \times SU(3)_{\ell}$ linear sigma model. | contribution 0.98 | 0.85 | 0.07 | asserted 0.63 |
| s1 | Gap equations for the masses of the scalar and pseudoscalar mesons and the non-strange and strange quark condensates are systematically derived in the Hartree approximation via the Cornwall-Jackiw-Tomboulis formalism. | method 0.98 | 0.94 | 0.04 | asserted 1.00 |
| s2 | In the chiral limit, the chiral symmetry restoring transition is found to be first order, as predicted by universality arguments. | result 1.00 | 0.83 | 0.21 | asserted 1.00 |
| s3 | Taking the experimental values for the meson masses, however, the transition is crossover. | result 1.00 | 0.87 | 0.42 | asserted 1.00 |
| s4 | The absence of the $U(1)_A$ anomaly is found to drive this transition closer to being first order. | result 0.70 | 0.89 | 0.10 | asserted 1.00 |
| s5 | At large temperatures, the mixing angles between octet and singlet states approach ideal flavor mixing. | result 1.00 | 0.84 | 0.08 | asserted 1.00 |
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The paper
Original abstract
We study patterns of chiral symmetry breaking at zero temperature and its subsequent restoration at nonzero temperature within the $SU(3)_{r} \times SU(3)_{\ell}$ linear sigma model. Gap equations for the masses of the scalar and pseudoscalar mesons and the non-strange and strange quark condensates are systematically derived in the Hartree approximation via the Cornwall-Jackiw-Tomboulis formalism. In the chiral limit, the chiral symmetry restoring transition is found to be first order, as predicted by universality arguments. Taking the experimental values for the meson masses, however, the transition is crossover. The absence of the $U(1)_A$ anomaly is found to drive this transition closer to being first order. At large temperatures, the mixing angles between octet and singlet states approach ideal flavor mixing.
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References
How later papers used it
51 later papers cite it
4 later papers by other authors are listed below: 1 used its method or tool, 2 used its data or values and 1 compared its own results with it.
Uses its method or tool 1 of 5 papers with this label
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Used this paper's expressions, derived via the partially conserved axial current relation, for the expectation values and source terms.
QCD-Collapsed Domain Walls: QCD Phase Transition and Gravitational Wave Spectroscopy (2023) · 0.88 · paraphrased: the licence does not allow quoting
Uses its data or values 2 papers
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Used this paper's results as a rough guide to the expected values of the coupling constants.
Pseudoscalar Mesons in the SU(3) Linear Sigma Model with Gaussian Functional Approximation (2010) · 1.00 · paraphrased: the licence does not allow quoting
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Took the value of the light quark condensate from its relation to the pion decay constant as given by this paper.
Chiral matrix model of the semi-Quark Gluon Plasma in QCD (2016) · 0.94 · paraphrased: the licence does not allow quoting
Compares with it 1 of 3 papers with this label
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Said that the qualitative behavior of its own condensates is similar to what was obtained in the CJT approximation by this paper.
Functional Renormalization for Chiral and U_A(1) Symmetries at Finite Temperature (2012) · 1.00 · paraphrased: the licence does not allow quoting
How the literature uses it
44 arXiv papers cite this in 115 sentences
Papers whose main result relates to this one's
States the same result 1 paper
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The linear $\sigma$-model in $SU(3)\times SU(3)$ gives a crossover around $T_c\approx190$ MeV.
Papers citing it · 69 sentences without a confident label
Uses its method or tool 4 papers
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The further procedure in the mean field approximation is to determine $λ_1(m_0^2)$ via $m_σ$ and $m_π$ [ref] .
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Note that, following Refs. [ref] , we consistently ignore vacuum contributions in evaluating loop integrals throughout all LSM-related calculations.
Observational prospects for gravitational waves from hidden or dark chiral phase transitions · Basics of the CJT formalism · 0.85
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Using the partially conserved axial current relation, $⟨σ_x,y⟩$ and $h_x,y$ are given by [ref] [equation] where $f_π,K$ are the pion and kaon decay constants, respectively.
QCD-Collapsed Domain Walls: QCD Phase Transition and Gravitational Wave Spectroscopy · QCD PT with a non-zero $θ$ in the LSM$q$ model · 0.88
Uses its data or values 2 papers
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Here we may use Ref. [ref] results as a (rough) guide to the expected values of the coupling constants: to first approximation we expect $λ_1 ≃50, λ_2 ≃1.5$, and if we define $c = λ_3 f_π$, we find $λ_3 ≃50$.
Pseudoscalar Mesons in the SU(3) Linear Sigma Model with Gaussian Functional Approximation · The $SU(3)$ Linear Sigma Model · 1.00
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We take the value of the light quark condensate from its relation to the pion decay constant, $f_π= 93.$ MeV [ref] :
Chiral matrix model of the semi-Quark Gluon Plasma in QCD · Parameters of the chiral model in QCD · 0.94
Compares with it 3 papers
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The qualitative behave of the condensates shown here is similar to what obtained in the frame of CJT approximation [ref] .
Functional Renormalization for Chiral and U_A(1) Symmetries at Finite Temperature · Numerical results · 1.00
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These values agree approximately with those of a linear sigma model without a logarithmic coupling, as studied by Lenaghan, Rischke, and Schaffner-Bielich (LRS) in Ref. [ref] .
Chiral matrix model of the semi-Quark Gluon Plasma in QCD · Parameters of the chiral model in QCD · 1.00
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It is as good as example benchmarks' in the literature: [ref] (with $μ^2>0$) yields 0.20 and 2.84, respectively, and [ref] ($μ^2<0$) yields 1.22 and 4.64.
Hubble selection of the weak scale from QCD quantum critical point · QCD quantum critical points · 0.98
Cites it as support 2 papers
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Moreover, it is also expected that the phase transition for chiral restoration takes place for a similar temperature as the deconfined one, as supported by models, e.g. [ref] .
Introductory visual lecture on QCD at large-$N_{c}$: bound states, chiral models, and phase diagram · Brief description of QCD at nonzero temperature and densities at large-$N_c$ · 0.99
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Note that here we neglect vacuum contributions, which was previously demonstrated to not change the outcome qualitatively [ref] .
Observational prospects for gravitational waves from hidden or dark chiral phase transitions · The linear sigma model · 0.99
Cites it as background 23 papers
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The $SU_L(3)×SU_R(3)$ linear sigma model has been widely studied in mean field and CJT approximation in vacuum and at finite temperature [ref] .
Functional Renormalization for Chiral and U_A(1) Symmetries at Finite Temperature · Application of Functional Renormalization to the $SU(3)$ Linear Sigma Model · 1.00
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Taking into account vacuum fluctuations needs regularization schemes [ref] .
Effects of Renormalizing the chiral SU(2) Quark-Meson-Model · Regularization for the quark fields · 0.86
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All physical fields are arranged in the matrix $Φ$ [ref] [equation] where we consider the condensed $σ_n,s$ fields and the pions to determine the vacuum parameters $λ_1$, $λ_2$, $m_0^2$, c, $h_n$ and $h_s$ of the model, which are fixed at tree level [ref] , but change upon renormalization [ref] , see Sec.[ref].
Implications of the fermion vacuum term in the extended SU(3) Quark Meson model on compact stars properties · The SU(3) Quark Meson model · 0.86
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