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Flavor-Mixing Effects on the QCD Phase Diagram at non-vanishing Isospin Chemical Potential: One or Two Phase Transitions?
High Energy Physics - Phenomenology · Submitted 13 Mar 2003
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We find that already for rather moderate values of the coupling strength in the flavor-mixing channel the recent findings of two seperate phase transitions do not persist.
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The abstract, sentence by sentence
We investigate effects of a fixed nonzero isospin chemical potential on the mu_B-T phase diagram of strongly interacting matter using a Nambu--Jona-Lasinio-type four fermion interaction. We focus on the influence of a flavor-mixing interaction induced by instantons. We find that already for rather moderate values of the coupling strength in the flavor-mixing channel the recent findings of two seperate phase transitions do not persist.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We investigate effects of a fixed nonzero isospin chemical potential on the mu_B-T phase diagram of strongly interacting matter using a Nambu--Jona-Lasinio-type four fermion interaction. | contribution 0.79 | 0.91 | 0.03 | asserted 0.75 |
| s1 | We focus on the influence of a flavor-mixing interaction induced by instantons. | contribution 0.91 | 0.41 | 0.03 | unclear 0.51 |
| s2 | We find that already for rather moderate values of the coupling strength in the flavor-mixing channel the recent findings of two seperate phase transitions do not persist. | result 1.00 | 0.95 | 0.90 | asserted 1.00 |
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The paper
Original abstract
We investigate effects of a fixed nonzero isospin chemical potential on the mu_B-T phase diagram of strongly interacting matter using a Nambu--Jona-Lasinio-type four fermion interaction. We focus on the influence of a flavor-mixing interaction induced by instantons. We find that already for rather moderate values of the coupling strength in the flavor-mixing channel the recent findings of two seperate phase transitions do not persist.
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References
How the literature uses it
17 arXiv papers cite this in 39 sentences
Papers citing it · 23 sentences without a confident label
Uses its method or tool 2 papers
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We follow the prescription of Ref. [ref] where they have considered a general NJL Lagrangian with arbitrary interaction strengths for $U(1)_A$ symmetric and breaking interactions, [equation] where the kinetic term is [equation] and the interactions are given by, [equation] with $L_1$ being symmetric under $U(1)_A$ but $L_2$ is not. $τ⃗$ represents Pauli matrices.
Studying explicit $U(1)_A$ symmetry breaking in hot and magnetised two flavour non-local NJL model constrained using lattice results · Formalism · 0.92
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For later convenience, following [ref] we parameterize the two coupling $G_1$ and $G_2$ in terms of a common $G$ and a parameter $α$ as [equation] so that $α=0$ describes the limit of decoupled quarks, while for $α=0.5$ we have $G_1 = G_2$ and the maximal coupling is realized.
Color-superconductivity and inhomogeneous chiral symmetry breaking in isospin-asymmetric quark matter · Model · 0.94
Uses its data or values 2 papers
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Following [ref] a good choice is $m_u = m_d = m = 6 MeV$, the cutoff $Λ= 590 MeV$ and $G_0Λ^2 = 2.435$.
Magnetic-Field Induced Critical Endpoint · Effective Potential · 0.96
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An alternative estimate for this parameter can be obtained from the $η- η'$ mass splitting within the 3-flavor NJL model [ref] , which leads to $α≃0.2$ [ref] .
Neutral pseudoscalar and vector meson masses under strong magnetic fields in an extended NJL model: mixing effects · Model parametrization and mean field results · 0.86
Compares with it 1 paper
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This agrees well with [ref] .
Magnetic-Field Induced Critical Endpoint · Chiral Phase Structure and Isospin Breaking · 0.95
Cites it as background 8 papers
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If one considers non-zero isospin chemical potential ($μ_I$ [ref] ) or/and magnetic field ($eB$ [ref] ), the independent appearance of both the $u$ and $d$ quark condensates in the $u$ and $d$ constituent masses becomes important.
Studying explicit $U(1)_A$ symmetry breaking in hot and magnetised two flavour non-local NJL model constrained using lattice results · Introduction · 0.86
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In addition to LQCD, these phases are also found using chiral perturbation theory ($χ$PT) [ref] , Hard Thermal Loop perturbation theory (HTLPt) [ref] , the Nambu-Jona-Lasinio (NJL) model [ref] and its Polyakov loop (PNJL) extended version [ref] , the quark meson model (QMM) [ref] and other low energy effective models exploiting functional RG studies [ref] .
QCD equation of state at finite isospin density from the linear sigma model with quarks: The cold case · Introduction · 0.86
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The formalism of the two-flavor NJL model at finite isospin density has been a subject of considerable scrutiny in the literature [ref] .
Describing the speed of sound peak of isospin-asymmetric cold strongly interacting matter using effective models · The NJL model at finite isospin chemical potential · 1.00
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