pith. sign in

arxiv: 2602.24170 · v3 · submitted 2026-02-27 · ✦ hep-ph · hep-ex· hep-lat

Kaons in hot and dense QCD

Pith reviewed 2026-05-15 18:51 UTC · model grok-4.3

classification ✦ hep-ph hep-exhep-lat
keywords QCD sum ruleskaon in-medium propertieschiral symmetry restorationhot dense QCDheavy-ion collisionscritical onset densityWeinberg-Tomozawa interaction
0
0 comments X

The pith

QCD sum rules extract a critical baryon density where K- masses and properties signal the onset of chiral symmetry restoration in hot dense matter.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper applies QCD sum rules to track how the masses, decay constants, and self-energies of charged kaons evolve across the full temperature-density plane relevant to heavy-ion collisions. It shows that kaon masses fall steadily with rising density and temperature while a charge-dependent mass splitting grows, both effects pointing to progressive partial restoration of chiral symmetry. The authors identify a critical onset density ρ_c(T) beyond which the K- modifications become pronounced enough to mark the approach to the chirally restored phase. This provides a concrete, calculable indicator that experiments can test without claiming to locate the exact QCD critical point. The vacuum results match known kaon properties to better than one percent, lending support to the medium extrapolations.

Core claim

Using Borel-transformed QCD sum rules that incorporate temperature- and density-dependent quark, gluon, and mixed condensates, the calculation yields effective masses m_{K±} that decrease monotonically with baryon density ρ and temperature T. A mass splitting Δm = m_{K-} − m_{K+} arises from the opposite signs of the Weinberg-Tomozawa vector interaction and reaches roughly 0.35 GeV near 3.2 times saturation density at zero temperature. The same framework simultaneously determines the pseudoscalar decay constants and vector self-energy for both charge states. The central result is the extraction of a critical onset density ρ_c(T) defined as the threshold at which these in-medium changes in K-

What carries the argument

Borel-transformed two-point correlation functions for the charged kaon doublet in nuclear medium, with temperature- and density-dependent condensates supplied as input parameters.

If this is right

  • Kaon effective masses decrease steadily with increasing baryon density and temperature.
  • A charge-dependent mass splitting develops in baryonic matter and is partially suppressed by thermal effects.
  • The critical onset density ρ_c(T) marks the point where K- modifications indicate the approach to the chirally restored phase.
  • Vacuum masses and decay constants reproduce Particle Data Group values at the sub-percent level.
  • ρ_c(T) functions as an indicator rather than a precise location of the QCD critical point.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The predicted mass splitting could alter kaon production and flow patterns measured in heavy-ion collisions at facilities probing densities above saturation.
  • Similar sum-rule treatments applied to other strange mesons might map how chiral restoration affects the full spectrum of light hadrons.
  • If the condensate parametrizations are refined with lattice input, the extracted ρ_c values could serve as quantitative benchmarks for effective models of the QCD phase diagram.

Load-bearing premise

The chosen parametrizations of the quark, gluon, and mixed condensates as functions of temperature and density must remain accurate across the entire (T, ρ) plane studied.

What would settle it

Observation of no significant mass drop or mass splitting for K- mesons in heavy-ion data near the predicted ρ_c at low temperature would contradict the claimed onset of chiral restoration effects.

Figures

Figures reproduced from arXiv: 2602.24170 by A. T\"urkan, G. Bozk{\i}r, K. Azizi, N. Er.

Figure 1
Figure 1. Figure 1: FIG. 1. Dependence of the vacuum masses of [PITH_FULL_IMAGE:figures/full_fig_p006_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Density dependence of the modified masses of [PITH_FULL_IMAGE:figures/full_fig_p007_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. The modified masses of [PITH_FULL_IMAGE:figures/full_fig_p008_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Density and temperature dependence of the in-medium masses of the [PITH_FULL_IMAGE:figures/full_fig_p008_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. Density dependence of the in-medium decay constants of [PITH_FULL_IMAGE:figures/full_fig_p009_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. Temperature dependence of the in-medium decay constants of [PITH_FULL_IMAGE:figures/full_fig_p010_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7. Evolution of the in-medium mass difference [PITH_FULL_IMAGE:figures/full_fig_p011_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8. Temperature dependence of the mass splitting [PITH_FULL_IMAGE:figures/full_fig_p011_8.png] view at source ↗
read the original abstract

We present a systematic QCD sum-rule analysis of the in-medium properties of the charged kaon doublet $K^{\pm}$ over the full $(T,\rho)$ plane relevant to current and forthcoming heavy-ion experiments. Working within the QCD sum-rule framework and incorporating temperature-and density-dependent quark, gluon, and mixed condensates, we derive Borel-transformed sum rules for the effective masses $m_{K^{\pm}}$, the pseudoscalar decay constants $f_{K^{\pm}}$, and the vector self-energy $\Sigma_{v}$ of both charged states simultaneously. Our vacuum results, $m_{K^{-}} = 494.6^{+4.9}_{-6.9}$~MeV and $f_{K^{-}} = 157.3^{+4.1}_{-2.9}$~MeV (with near-degenerate $K^{+}$ values), are in excellent agreement with Particle Data Group values at the sub-percent level. In the medium, $m_{K^{\pm}}$ decreases monotonically with increasing baryon density and temperature, signalling progressive partial restoration of chiral symmetry. A pronounced mass splitting $\Delta m = m_{K^{-}} - m_{K^{+}}$ develops in baryonic matter, driven by the opposite sign of the Weinberg--Tomozawa vector interaction for the two charge states; it reaches $|\Delta m| \sim 0.35$~GeV near $\rho \simeq 3.2\,\rho_{\rm sat}$ at $T = 0$ and is partially quenched by thermal fluctuations. A central outcome of this study is the extraction of the critical onset density $\rho_c$, defined as the threshold beyond which the in-medium modifications of $K^{-}$ properties signal the onset of the transition toward the chirally restored phase. We stress that $\rho_c(T)$ should not be interpreted as a precise determination of the QCD critical point-a task beyond the reach of any current effective framework-but rather as an indicator ....

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 1 minor

Summary. The manuscript performs a QCD sum-rule analysis of the in-medium properties of charged kaons K± across the (T,ρ) plane, deriving Borel-transformed sum rules for effective masses m_{K±}, pseudoscalar decay constants f_{K±}, and vector self-energy Σ_v using temperature- and density-dependent quark, gluon, and mixed condensates. Vacuum results match PDG values at the sub-percent level (e.g., m_{K^-} = 494.6^{+4.9}_{-6.9} MeV), while medium results show monotonic mass decrease, charge-dependent splitting Δm reaching ~0.35 GeV near 3.2 ρ_sat at T=0, and extraction of a critical onset density ρ_c(T) defined as the threshold where K^- modifications signal the approach to chiral restoration.

Significance. If the medium sum-rule analysis proves robust, the work provides a systematic exploration of kaon properties over the full (T,ρ) range relevant to heavy-ion collisions, with the extracted ρ_c serving as a practical indicator (explicitly not claimed as the QCD critical point) for the onset of partial chiral restoration. The simultaneous treatment of both charge states and inclusion of thermal quenching of the splitting are strengths.

major comments (2)
  1. [Results section (ρ_c extraction)] The extraction of ρ_c (defined in the abstract and results as the density beyond which K^- modifications signal chiral restoration) is controlled by the imported T/ρ-dependent forms of the light-quark, gluon, and mixed condensates. No systematic variation of these external parametrizations or propagation of their uncertainties into the reported ρ_c value is performed, rendering the numerical threshold sensitive to the choice of inputs.
  2. [Formalism and results sections] The Borel mass M² and continuum threshold s0 (free parameters in the sum-rule setup) are stated to remain stable across the (T,ρ) plane, yet no explicit windows, stability tests, or error budgets for the medium extrapolations are provided, which directly affects verification of the ρ_c onset.
minor comments (1)
  1. [Abstract] The abstract reports vacuum values for K^- but only states 'near-degenerate K+ values' without quoting the K+ numbers; explicit listing would improve clarity.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the thorough review and constructive feedback on our QCD sum-rule analysis of in-medium kaon properties. We address each major comment below and have revised the manuscript to strengthen the presentation of uncertainties and stability criteria.

read point-by-point responses
  1. Referee: The extraction of ρ_c (defined in the abstract and results as the density beyond which K^- modifications signal chiral restoration) is controlled by the imported T/ρ-dependent forms of the light-quark, gluon, and mixed condensates. No systematic variation of these external parametrizations or propagation of their uncertainties into the reported ρ_c value is performed, rendering the numerical threshold sensitive to the choice of inputs.

    Authors: We agree that ρ_c is sensitive to the adopted condensate parametrizations. In the revised manuscript we have added an explicit discussion of this dependence, including results for two alternative sets of T/ρ-dependent condensates drawn from the literature. We now quote a conservative uncertainty band on ρ_c(T) that incorporates the spread between these parametrizations, while noting that a exhaustive global scan lies beyond the scope of the present work. revision: yes

  2. Referee: The Borel mass M² and continuum threshold s0 (free parameters in the sum-rule setup) are stated to remain stable across the (T,ρ) plane, yet no explicit windows, stability tests, or error budgets for the medium extrapolations are provided, which directly affects verification of the ρ_c onset.

    Authors: We acknowledge that explicit documentation of the Borel windows and stability tests was insufficient. The revised manuscript now includes a dedicated subsection with tables listing the M² and s0 windows employed at representative (T,ρ) points, together with stability plots that demonstrate the extracted masses remain flat within those windows. We have also added error budgets obtained by varying M² and s0 within their allowed ranges for both vacuum and medium cases. revision: yes

Circularity Check

0 steps flagged

No significant circularity in derivation of in-medium kaon properties or ρ_c

full rationale

The paper performs a standard QCD sum-rule calculation that takes external T/ρ-dependent condensate parametrizations as inputs, constructs Borel-transformed sum rules for m_{K±}, f_{K±} and Σ_v, reproduces vacuum PDG values to sub-percent accuracy as validation, and then computes the medium evolution. ρ_c is identified numerically as the density at which the computed modifications become large. This is a forward computation from independent inputs rather than any self-definitional loop, fitted-input-renamed-as-prediction, or load-bearing self-citation chain. The explicit caveat that ρ_c is only an indicator, not a determination of the critical point, further confirms the result does not reduce to its inputs by construction.

Axiom & Free-Parameter Ledger

2 free parameters · 2 axioms · 0 invented entities

The central results rest on standard QCD sum-rule machinery plus external parametrizations for the medium dependence of condensates; no new particles or forces are introduced.

free parameters (2)
  • Borel mass M^2
    Stability window chosen to suppress higher-dimensional operators while keeping continuum contribution small
  • continuum threshold s0
    Adjusted to reproduce vacuum kaon mass and decay constant
axioms (2)
  • domain assumption Temperature and density dependence of quark, gluon, and mixed condensates follows specific functional forms taken from prior literature
    These forms are inserted directly into the operator product expansion without independent derivation in the present work
  • domain assumption The Weinberg-Tomozawa term provides the leading vector interaction responsible for K+ versus K- splitting
    Standard chiral effective theory input used to interpret the sign difference in self-energies

pith-pipeline@v0.9.0 · 5671 in / 1428 out tokens · 31794 ms · 2026-05-15T18:51:30.196266+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Reference graph

Works this paper leans on

53 extracted references · 53 canonical work pages

  1. [1]

    Hatsuda and T

    T. Hatsuda and T. Kunihiro, ”QCD phenomenology based on a chiral effective Lagrangian”, Phys. Rept.247, 221-367 (1994). 15

  2. [2]

    Fukushima and T

    K. Fukushima and T. Hatsuda, ”The phase diagram of dense QCD”, Rept. Prog. Phys.74, 014001 (2011)

  3. [3]

    R. S. Hayano and T. Hatsuda, ”Hadron properties in the nuclear medium”, Rev. Mod. Phys.82, 2949 (2010)

  4. [4]

    G. Baym, T. Hatsuda, T. Kojo, P. D. Powell, Y. Song and T. Takatsuka, ”From hadrons to quarks in neutron stars: a review”, Rept. Prog. Phys.81no.5, 056902 (2018)

  5. [5]

    Y. Aoki, G. Endrodi, Z. Fodor, S. D. Katz and K. K. Szabo, ”The order of the quantum chromodynamics transition predicted by the standard model of particle physics”, Nature443, 675-678 (2006)

  6. [6]

    Bazavov, H

    A. Bazavov, H. T. Ding, P. Hegde, O. Kaczmarek, F. Karsch, E. Laermann, Y. Maezawa, S. Mukherjee, H. Ohno and P. Petreczky,et al. ”The QCD Equation of State toO (𝜇 6 𝐵)from Lattice QCD”, Phys. Rev. D95no.5, 054504 (2017)

  7. [7]

    M. F. M. Lutz, A. Steiner and W. Weise, ”Kaons and strange quarks in dense matter”, Phys. Lett. B278, 29-33 (1992)

  8. [8]

    J. M. Lattimer and M. Prakash, ”The Equation of State of Hot, Dense Matter and Neutron Stars”, Phys. Rept.621, 127-164 (2016)

  9. [9]

    Mishra, E

    A. Mishra, E. L. Bratkovskaya, J. Schaffner-Bielich, S. Schramm and H. St¨ocker, ”Kaons and antikaons in hot and dense hadronic matter”, Phys. Rev. C70, 044904 (2004)

  10. [10]

    T. Song, T. Hatsuda and S. H. Lee, ”QCD sum rule for open strange meson𝐾 ± 1 in nuclear matter”, Phys. Lett. B792, 160-169 (2019)

  11. [11]

    Tang Huan-Huan and Peng Guang-Xiong, ”A New Calculation of the In-Medium Quark Condensate at Finite Density and Temperature”, Commun. Theor. Phys.,56, 1071-1074 (2011)

  12. [12]

    A. Gal, E. V. Hungerford and D. J. Millener, ”Strangeness in nuclear physics”, Rev. Mod. Phys.88no.3, 035004 (2016)

  13. [13]

    G. E. Brown, C. M. Ko, Z. G. Wu, and L. H. Xia, ‘Kaon production from hot and dense matter formed in heavy-ion collisions”, Phys. Rev. C43, 1881-1892 (1991)

  14. [14]

    Cassing and E.L

    W. Cassing and E.L. Bratkovskaya, ”Hadronic and electromagnetic probes of hot and dense nuclear matter”, Phys. Rept.308, 65-233 (1999)

  15. [15]

    Mishustin, Jakob Bondorf, ”In-medium kaon production at the mean-field level”, Nucl

    J¨ urgen Schaffner-Bielich, Igor N. Mishustin, Jakob Bondorf, ”In-medium kaon production at the mean-field level”, Nucl. Phys. A625, 325-346 (1997)

  16. [16]

    M. F. M. Lutz, S. Klimt and W. Weise, ”Meson properties at finite temperature and baryon density”, Nucl. Phys. A542, 521-558 (1992)

  17. [17]

    Brown, G. E. and Rho, Mannque, ”Scaling effective Lagrangians in a dense medium”, Phys. Rev. Lett.66, 2720–2723 (1991)

  18. [18]

    Tol ´os, Laura and Ramos, Angels and Polls, Artur, ”Antikaon nuclear potential in hot and dense matter”, Phys. Rev. C65,054907 (2002)

  19. [19]

    Kaplan and A.E

    D.B. Kaplan and A.E. Nelson, ”Strange goings on in dense nucleonic matter”, Phys. Lett. B175, 57-63 (1986)

  20. [20]

    Costa, M

    P. Costa, M. C. Ruivo, Y. L. Kalinovsky and C. A. de Sousa, ”Pseudoscalar mesons in hot, dense matter”, Phys. Rev. C70, 025204 (2004)

  21. [21]

    Bozkır, A

    G. Bozkır, A. T¨ urkan and K. Azizi, ”Properties of kaon at non-zero temperature and baryon chemical potential”, Eur. Phys. J. A59no.11, 267 (2023)

  22. [22]

    Er and K

    N. Er and K. Azizi, ”Spectroscopic parameters and electromagnetic form factor of kaon in vacuum and a dense medium”, Eur. Phys. J. C 82no.5, 397 (2022)

  23. [23]

    Kumar, ”Heavy Scalar, Vector and Axial-Vector Mesons in Hot and Dense Nuclear Medium”, Adv

    A. Kumar, ”Heavy Scalar, Vector and Axial-Vector Mesons in Hot and Dense Nuclear Medium”, Adv. High Energy Phys.2014, 549726 (2014)

  24. [24]

    T. D. Cohen, R. J. Furnstahl, D. K. Griegel and X. m. Jin, ”QCD sum rules and applications to nuclear physics”, Prog. Part. Nucl. Phys. 35, 221-298 (1995)

  25. [25]

    Chanfray, ”Hadrons in dense and hot matter: Implications of chiral symmetry restoration”, Nucl

    G. Chanfray, ”Hadrons in dense and hot matter: Implications of chiral symmetry restoration”, Nucl. Phys. A685, 328-345 (2001)

  26. [26]

    Cabrera, D

    D. Cabrera, D. Fernandez-Fraile and A. Gomez Nicola, ”Chiral Symmetry and light resonances in hot and dense matter”, Eur. Phys. J. C 61, 879-892 (2009)

  27. [27]

    Ilner, D

    A. Ilner, D. Cabrera, P. Srisawad and E. Bratkovskaya, ”Properties of strange vector mesons in dense and hot matter”, Nucl. Phys. A927, 249-265 (2014)

  28. [28]

    R. Rapp, J. Wambach and H. van Hees, ”The Chiral Restoration Transition of QCD and Low Mass Dileptons”, Landolt-Bornstein23, 134 (2010)

  29. [29]

    Kumar and A

    R. Kumar and A. Kumar, ”Open strange meson𝐾 ± 1 in hot and dense nuclear matter”, SciPost Phys. Proc., 055 (2022)

  30. [30]

    Cassing, A

    W. Cassing, A. Palmese, P. Moreau, and E. L. Bratkovskaya, ”Chiral symmetry restoration versus deconfinement in heavy-ion collisions at high baryon density”, Phys. Rev. C93, 014902 (2016)

  31. [31]

    Ahmad, N

    Z. Ahmad, N. Chahal, A. Kumar and S. Dutt, ”Impact of Finite Volume on Kaon, Antikaon, and𝜙Meson Masses and Decay Widths in Asymmetric Strange Hadronic Matter”, Prog. Theo. Exp. Phys.2025no.1, 013B03 (2025)

  32. [32]

    Kahangirwe, S

    M. Kahangirwe, S. A. Bass, E. Bratkovskaya, J. Jahan, P. Moreau, P. Parotto, D. Price, C. Ratti, O. Soloveva and M. Stephanov, ”Finite density QCD equation of state: Critical point and lattice-based T’ expansion”, Phys. Rev. D109no.9, 094046 (2024)

  33. [33]

    Costa and R

    P. Costa and R. C. Pereira, ”Phase Diagram, Scalar-Pseudoscalar Meson Behavior and Restoration of Symmetries in (2 + 1) Polyakov- Nambu-Jona-Lasinio Model”, Symmetry11no.4, 507-538 (2019)

  34. [34]

    Moreau, A

    P. Moreau, A. Palmese, W. Cassing, E. Seifert, T. Steinert, E.L. Bratkovskaya, ”Evidence for chiral symmetry restoration in heavy-ion collisions”, Nucl. Phys. A967, 836-839 (2017)

  35. [35]

    H. T. Ding, F. Karsch and S. Mukherjee, ”Thermodynamics of strong-interaction matter from Lattice QCD”, Int. J. Mod. Phys. E24 no.10, 1530007 (2015)

  36. [36]

    Borsanyi, Z

    S. Borsanyi, Z. Fodor, J. N. Guenther, R. Kara, S. D. Katz, P. Parotto, A. Pasztor, C. Ratti and K. K. Szabo, ”QCD Crossover at Finite Chemical Potential from Lattice Simulations”, Phys. Rev. Lett.125(2020) no.5, 052001

  37. [37]

    L. Y. Glozman, ”Chiral spin symmetry and hot/dense QCD”, Prog. Part. Nucl. Phys.131, 104049 (2023)

  38. [38]

    Kornakov [HADES], ”Measurements and understanding of fundamental properties of hot and dense nuclear matter with HADES”, J

    G. Kornakov [HADES], ”Measurements and understanding of fundamental properties of hot and dense nuclear matter with HADES”, J. Phys. Conf. Ser.1024no.1, 012006 (2018)

  39. [39]

    Adamczewski-Muschet al.[HADES], ”Strong absorption of hadrons with hidden and open strangeness in nuclear matter”, Phys

    J. Adamczewski-Muschet al.[HADES], ”Strong absorption of hadrons with hidden and open strangeness in nuclear matter”, Phys. Rev. Lett.123no.2, 022002 (2019)

  40. [40]

    Ablyazimovet al.[CBM], ”Challenges in QCD matter physics –The scientific programme of the Compressed Baryonic Matter experiment at FAIR”, Eur

    T. Ablyazimovet al.[CBM], ”Challenges in QCD matter physics –The scientific programme of the Compressed Baryonic Matter experiment at FAIR”, Eur. Phys. J. A53no.3, 60 (2017). 16

  41. [41]

    Adamet al.[STAR], ”Beam energy dependence of net-Λfluctuations measured by the STAR experiment at the BNL Relativistic Heavy Ion Collider”, Phys

    J. Adamet al.[STAR], ”Beam energy dependence of net-Λfluctuations measured by the STAR experiment at the BNL Relativistic Heavy Ion Collider”, Phys. Rev. C102no.2, 024903 (2020)

  42. [42]

    Acharyaet al.[NA61/SHINE], ”Measurements of𝜋 ±,𝐾 ±,𝑝and ¯𝑝spectra in 7Be+9Be collisions at beam momenta from 19𝐴to 150𝐴 GeV/𝑐with the NA61/SHINE spectrometer at the CERN SPS”, Eur

    A. Acharyaet al.[NA61/SHINE], ”Measurements of𝜋 ±,𝐾 ±,𝑝and ¯𝑝spectra in 7Be+9Be collisions at beam momenta from 19𝐴to 150𝐴 GeV/𝑐with the NA61/SHINE spectrometer at the CERN SPS”, Eur. Phys. J. C81no.1, 73 (2021)

  43. [43]

    D. B. Kaplan, and A. E. Nelson, ”Kaon condensation in dense matter”, Nucl. Phys. A.479, 273-284 (1988)

  44. [44]

    M. G. Alford, K. Rajagopal and F. Wilczek, ”QCD at finite baryon density: Nucleon droplets and color superconductivity”, Phys. Lett. B 422, 247-256 (1998)

  45. [45]

    Fukushima and C

    K. Fukushima and C. Sasaki, ”The phase diagram of nuclear and quark matter at high baryon density”, Prog. Part. Nucl. Phys.72, 99-154 (2013)

  46. [46]

    T¨ urkan, G

    A. T¨ urkan, G. Bozkır and K. Azizi, ”Properties of spin-1/2 heavy baryons at nonzero temperature”, Phys. Rev. D104no.9, 094029 (2021)

  47. [47]

    Navas, and others (Particle Data Group), ”Review of Particle Physics”, Phys

    S. Navas, and others (Particle Data Group), ”Review of Particle Physics”, Phys. Rev. D110, 030001 (2024)

  48. [48]

    X. S. Fang, C. M. Ko, G. E. Brown, and V. Koch, ”Medium effects on kaon and antikaon spectra in heavy-ion collisionsy”, Phys. Rev. C 47no.4, 1678–1682 (2022)

  49. [49]

    Loewe, ”Pions at Finite Temperature from QCD Sum Rules”, Phys.Lett

    C.A.Dominguez, M.S.Fetea and M. Loewe, ”Pions at Finite Temperature from QCD Sum Rules”, Phys.Lett. B387, 151-154 (1996)

  50. [50]

    B. J. Schaefer and J. Wambach, ”Renormalization group approach towards the QCD phase diagram”, Phys. Part. Nucl.39, 1025-1032 (2008)

  51. [51]

    Buballa, ”NJL model analysis of quark matter at large density”, Phys

    M. Buballa, ”NJL model analysis of quark matter at large density”, Phys. Rept.407, 205-376 (2005)

  52. [52]

    B. J. Schaefer, M. Wagner and J. Wambach, ”Thermodynamics of (2+1)-flavor QCD: Confronting Models with Lattice Studies,” Phys. Rev. D81, 074013 (2010)

  53. [53]

    Antonin, ”Production des baryons multi- ´etranges au LHC dans les collisions proton-proton avec l’exp´erience ALICE”, Ph.D

    M. Antonin, ”Production des baryons multi- ´etranges au LHC dans les collisions proton-proton avec l’exp´erience ALICE”, Ph.D. Thesis, Universit´e de Strasbourg, CERN-THESIS-2011-263 (2011)