Searching for the QCD critical end point using multipoint Padé approximations

Using the multipoint Padé approach, we locate Lee-Yang edge singularities of the quantum chromodynamics (QCD) pressure in the complex baryon chemical potential plane. These singularities are extracted from singularities in the net baryon-number density calculated in <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:msub> <a:mi>N</a:mi> <a:mi>f</a:mi> </a:msub> <a:mo>=</a:mo> <a:mn>2</a:mn> <a:mo>+</a:mo> <a:mn>1</a:mn> </a:math> lattice QCD at physical quark mass and purely imaginary chemical potential. Taking an appropriate scaling ansatz in the vicinity of the conjectured QCD critical end point, we extrapolate the singularities on <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:msub> <c:mi>N</c:mi> <c:mi>τ</c:mi> </c:msub> <c:mo>=</c:mo> <c:mn>6</c:mn> </c:math> lattices to pure real baryon chemical potential to estimate the position of the critical end point (CEP). We find <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"> <e:msup> <e:mi>T</e:mi> <e:mi>CEP</e:mi> </e:msup> <e:mo>=</e:mo> <e:mn>10</e:mn> <e:msubsup> <e:mn>2</e:mn> <e:mrow> <e:mo>−</e:mo> <e:mn>23</e:mn> </e:mrow> <e:mrow> <e:mo>+</e:mo> <e:mn>11</e:mn> </e:mrow> </e:msubsup> <e:mtext> </e:mtext> <e:mtext> </e:mtext> <e:mi>MeV</e:mi> </e:math> and <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"> <g:msubsup> <g:mi>μ</g:mi> <g:mi>B</g:mi> <g:mi>CEP</g:mi> </g:msubsup> <g:mo>=</g:mo> <g:mn>42</g:mn> <g:msubsup> <g:mn>8</g:mn> <g:mrow> <g:mo>−</g:mo> <g:mn>74</g:mn> </g:mrow> <g:mrow> <g:mo>+</g:mo> <g:mn>162</g:mn> </g:mrow> </g:msubsup> <g:mtext> </g:mtext> <g:mtext> </g:mtext> <g:mi>MeV</g:mi> </g:math> , which compares well with recent estimates in the literature. For the slope of the transition line at the critical point we find <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"> <i:mo>−</i:mo> <i:mn>0.16</i:mn> <i:mo stretchy="false">(</i:mo> <i:mn>20</i:mn> <i:mo stretchy="false">)</i:mo> </i:math> .

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Journal
Physical review. D/Physical review. D.
Published
2025-10-14
DOI
https://doi.org/10.1103/y6kg-ry8x
Citations
7
Primary Topic
Quantum Chromodynamics and Particle Interactions
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article
Field-Weighted Citation Impact
13.09
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article

Searching for the QCD critical end point using multipoint Padé approximations

Francesco Di Renzo, P. Dimopoulos, Jishnu Goswami, Simran Singh et al.
7 citations
Physical review. D/Physical review. D.
Quantum Chromodynamics and Particle Interactions
13.09
article

Searching for the QCD critical end point using multipoint Padé approximations

Francesco Di Renzo, P. Dimopoulos, Jishnu Goswami, Simran Singh, Kevin Zambello, Christian Schmidt, D. Clarke
article en
7 citations

Abstract

Using the multipoint Padé approach, we locate Lee-Yang edge singularities of the quantum chromodynamics (QCD) pressure in the complex baryon chemical potential plane. These singularities are extracted from singularities in the net baryon-number density calculated in <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:msub> <a:mi>N</a:mi> <a:mi>f</a:mi> </a:msub> <a:mo>=</a:mo> <a:mn>2</a:mn> <a:mo>+</a:mo> <a:mn>1</a:mn> </a:math> lattice QCD at physical quark mass and purely imaginary chemical potential. Taking an appropriate scaling ansatz in the vicinity of the conjectured QCD critical end point, we extrapolate the singularities on <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:msub> <c:mi>N</c:mi> <c:mi>τ</c:mi> </c:msub> <c:mo>=</c:mo> <c:mn>6</c:mn> </c:math> lattices to pure real baryon chemical potential to estimate the position of the critical end point (CEP). We find <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"> <e:msup> <e:mi>T</e:mi> <e:mi>CEP</e:mi> </e:msup> <e:mo>=</e:mo> <e:mn>10</e:mn> <e:msubsup> <e:mn>2</e:mn> <e:mrow> <e:mo>−</e:mo> <e:mn>23</e:mn> </e:mrow> <e:mrow> <e:mo>+</e:mo> <e:mn>11</e:mn> </e:mrow> </e:msubsup> <e:mtext> </e:mtext> <e:mtext> </e:mtext> <e:mi>MeV</e:mi> </e:math> and <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"> <g:msubsup> <g:mi>μ</g:mi> <g:mi>B</g:mi> <g:mi>CEP</g:mi> </g:msubsup> <g:mo>=</g:mo> <g:mn>42</g:mn> <g:msubsup> <g:mn>8</g:mn> <g:mrow> <g:mo>−</g:mo> <g:mn>74</g:mn> </g:mrow> <g:mrow> <g:mo>+</g:mo> <g:mn>162</g:mn> </g:mrow> </g:msubsup> <g:mtext> </g:mtext> <g:mtext> </g:mtext> <g:mi>MeV</g:mi> </g:math> , which compares well with recent estimates in the literature. For the slope of the transition line at the critical point we find <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"> <i:mo>−</i:mo> <i:mn>0.16</i:mn> <i:mo stretchy="false">(</i:mo> <i:mn>20</i:mn> <i:mo stretchy="false">)</i:mo> </i:math> .

Physical review. D/Physical review. D.Vol. 112(9)
University of Pisa (IT), University of Parma (IT), Bielefeld University (DE), University of Utah (US), RIKEN Center for Computational Science (JP), Istituto Nazionale di Fisica Nucleare, Sezione di Pisa (IT), Istituto Nazionale di Fisica Nucleare, Gruppo Collegato di Parma
Openalex Percentile: Top 1%
Quantum Chromodynamics and Particle Interactions
13.09
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