Columbia plot based on the symmetry-improved Cornwall-Jackiw-Tomboulis formalism in the linear sigma model

We study the Columbia plot for the chiral phase transition in the framework of a three-flavor linear sigma model based on the Cornwall-Jackiw-Tomboulis (CJT) formalism. The conventional CJT approach with the Hartree truncation suffers from artificial chiral breaking, leading to the violation of the Nambu-Goldstone theorem and the (anomalous) chiral Ward-Takahashi identities. We apply the symmetry-improved CJT formalism to resolve this issue. We observe a first-order phase transition and a tricritical point in the light-quark mass regime, which is relatively independent of the size of the sigma meson, in contrast to the conventional CJT approach. The tricritical point, found on the <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:msub> <a:mi>m</a:mi> <a:mi>s</a:mi> </a:msub> </a:math> axis, is at <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:mrow> <c:msubsup> <c:mrow> <c:mi>m</c:mi> </c:mrow> <c:mrow> <c:mi>s</c:mi> </c:mrow> <c:mrow> <c:mi>tri</c:mi> </c:mrow> </c:msubsup> <c:mo>/</c:mo> <c:msubsup> <c:mrow> <c:mi>m</c:mi> </c:mrow> <c:mrow> <c:mi>s</c:mi> </c:mrow> <c:mrow> <c:mi>phys</c:mi> </c:mrow> </c:msubsup> <c:mo>=</c:mo> <c:mn>0.175</c:mn> </c:mrow> </c:math> with <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"> <e:msubsup> <e:mi>m</e:mi> <e:mi>s</e:mi> <e:mrow> <e:mi>phys</e:mi> </e:mrow> </e:msubsup> </e:math> being the physical strange quark mass in real-life QCD. The critical pion mass in the three-flavor symmetric limit, on the second-order boundary, is measured at <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"> <g:mrow> <g:msub> <g:mrow> <g:mi>m</g:mi> </g:mrow> <g:mrow> <g:mi>π</g:mi> </g:mrow> </g:msub> <g:mo>∼</g:mo> <g:mn>52.4</g:mn> <g:mtext> </g:mtext> <g:mtext> </g:mtext> <g:mi>MeV</g:mi> </g:mrow> </g:math> , with the critical temperature <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"> <i:mrow> <i:msub> <i:mrow> <i:mi>T</i:mi> </i:mrow> <i:mrow> <i:mi>c</i:mi> </i:mrow> </i:msub> <i:mo>∼</i:mo> <i:mn>51.7</i:mn> <i:mtext> </i:mtext> <i:mtext> </i:mtext> <i:mi>MeV</i:mi> </i:mrow> </i:math> .

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Journal
Physical review. D/Physical review. D.
Published
2025-12-18
DOI
https://doi.org/10.1103/71r7-8b3p
Primary Topic
Quantum Chromodynamics and Particle Interactions
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article
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article

Columbia plot based on the symmetry-improved Cornwall-Jackiw-Tomboulis formalism in the linear sigma model

Karl J. Friston
Physical review. D/Physical review. D.
Quantum Chromodynamics and Particle Interactions
article

Columbia plot based on the symmetry-improved Cornwall-Jackiw-Tomboulis formalism in the linear sigma model

Karl J. Friston
article en

Abstract

We study the Columbia plot for the chiral phase transition in the framework of a three-flavor linear sigma model based on the Cornwall-Jackiw-Tomboulis (CJT) formalism. The conventional CJT approach with the Hartree truncation suffers from artificial chiral breaking, leading to the violation of the Nambu-Goldstone theorem and the (anomalous) chiral Ward-Takahashi identities. We apply the symmetry-improved CJT formalism to resolve this issue. We observe a first-order phase transition and a tricritical point in the light-quark mass regime, which is relatively independent of the size of the sigma meson, in contrast to the conventional CJT approach. The tricritical point, found on the <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:msub> <a:mi>m</a:mi> <a:mi>s</a:mi> </a:msub> </a:math> axis, is at <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:mrow> <c:msubsup> <c:mrow> <c:mi>m</c:mi> </c:mrow> <c:mrow> <c:mi>s</c:mi> </c:mrow> <c:mrow> <c:mi>tri</c:mi> </c:mrow> </c:msubsup> <c:mo>/</c:mo> <c:msubsup> <c:mrow> <c:mi>m</c:mi> </c:mrow> <c:mrow> <c:mi>s</c:mi> </c:mrow> <c:mrow> <c:mi>phys</c:mi> </c:mrow> </c:msubsup> <c:mo>=</c:mo> <c:mn>0.175</c:mn> </c:mrow> </c:math> with <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"> <e:msubsup> <e:mi>m</e:mi> <e:mi>s</e:mi> <e:mrow> <e:mi>phys</e:mi> </e:mrow> </e:msubsup> </e:math> being the physical strange quark mass in real-life QCD. The critical pion mass in the three-flavor symmetric limit, on the second-order boundary, is measured at <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"> <g:mrow> <g:msub> <g:mrow> <g:mi>m</g:mi> </g:mrow> <g:mrow> <g:mi>π</g:mi> </g:mrow> </g:msub> <g:mo>∼</g:mo> <g:mn>52.4</g:mn> <g:mtext> </g:mtext> <g:mtext> </g:mtext> <g:mi>MeV</g:mi> </g:mrow> </g:math> , with the critical temperature <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"> <i:mrow> <i:msub> <i:mrow> <i:mi>T</i:mi> </i:mrow> <i:mrow> <i:mi>c</i:mi> </i:mrow> </i:msub> <i:mo>∼</i:mo> <i:mn>51.7</i:mn> <i:mtext> </i:mtext> <i:mtext> </i:mtext> <i:mi>MeV</i:mi> </i:mrow> </i:math> .

Physical review. D/Physical review. D.Vol. 113(1)
Anhui University of Science and Technology (CN), Jilin University (CN), Tokyo Woman's Christian University (JP), RIKEN Center for Computational Science (JP), Jilin Medical University (CN)
Openalex Percentile: Top 81%
Quantum Chromodynamics and Particle Interactions
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