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Using two-color lattice QCD with Wilson fermions, we report a study of the finite baryon number density system with two-flavors. First we investigate the Polyakov line and thermodynamical uantities in the $(\kappa,\mu)$ plane, where…

High Energy Physics - Lattice · Physics 2016-09-01 Shin Muroya , Atsushi Nakamura , Chiho Nonaka

Instantons generate strong non-perturbative interactions between quarks. In the vacuum, these interactions lead to chiral symmetry breaking and generate constituent quark masses on the order of 300-400 MeV. The observation that the same…

High Energy Physics - Phenomenology · Physics 2009-10-31 R. Rapp , T. Schaefer , E. V. Shuryak , M. Velkovsky

The exploration of the QCD phase diagram is the goal of many experiments in the world. The low net baryon density region is relatively well studied, while the one corresponding to higher net densities still contains multiple unrevealed…

Nuclear Experiment · Physics 2022-09-20 Maria Stefaniak

We review recent results on QCD at finite temperature and non-vanishing baryon number density. We focus on observables which are of immediate interest to experimental searches for the Quark Gluon Plasma, i.e. the phase transition…

High Energy Physics - Lattice · Physics 2015-06-25 Frithjof Karsch

Strongly interacting matter exhibits new phases under extreme conditions. Matter was exposed to such extremes not only in the Early Universe, but also today in the cores of neutron stars, as well as in laboratory experiments at a much…

Nuclear Theory · Physics 2025-12-10 Szabolcs Borsanyi , Paolo Parotto

I review recent developments in finite temperature lattice QCD which are useful for the study of heavy-ion collisions. I pay particular attention to studies of the equation of state and the light they throw on conformal symmetry and the…

Nuclear Theory · Physics 2008-11-26 Sourendu Gupta

As part of an ongoing effort to characterize the high temperature phase of QCD, in a numerical simulation using the staggered fermion scheme, we measure the quark baryon density in the vicinity of a fixed test quark at high temperature and…

High Energy Physics - Lattice · Physics 2008-11-26 Claude Bernard , Thomas A. DeGrand , Carleton DeTar , Steven Gottlieb , Alex Krasnitz , Robert L. Sugar , Douglas Toussaint

The possibility of kaon condensation in high-density symmetric nuclear matter is investigated including both s- and p-wave kaon-baryon interactions within the relativistic mean-field (RMF) theory. Above a certain density, we have a…

Nuclear Theory · Physics 2010-02-17 Tomoyuki Maruyama , Takumi Muto , Toshitaka Tatsumi , Kazuo Tsushima , Anthony W. Thomas

Recent progress in understanding general properties of high energy scattering near the unitarity limit, where high density gluon components of the wavefunction are dominant, is reviewed. The similarity of the QCD problem and that of…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. H. Mueller

We investigate the properties of QCD axion at low temperature and moderate density in the Nambu-Jona-Lasinio model with instanton induced interactions by simultaneously considering the scalar and pseudo-scalar condensates in both…

High Energy Physics - Phenomenology · Physics 2025-01-22 Zhao Zhang , Wenhao Zhao

Baryonic matter at high density and low temperature is a color superconductor. In real world, this state of matter may naturally appear inside compact stars. A construction of a hybrid compact star with two flavor color superconducting…

High Energy Physics - Phenomenology · Physics 2007-05-23 Igor Shovkovy , Matthias Hanauske , Mei Huang

Cold and dense matter is expected to be in a color-superconducting state. Here we review two calculations, relevant for fundamental properties and applications of color superconductivity, respectively: the weak-coupling QCD calculation of…

High Energy Physics - Phenomenology · Physics 2025-11-11 Andreas Schmitt

The structure of $K^-$-condensed hypernuclei, which may be produced in the laboratory in strangeness-conserving processes, is investigated using an effective chiral Lagrangian for the kaon-baryon interaction, combined with a nonrelativistic…

Nuclear Theory · Physics 2008-11-26 Takumi Muto

We discuss how the co-existence of hyperons, antikaon condensate and color superconducting quark matter in neutron star interior influences the gross properties of compact stars such as, the equation of state and mass-radius relationship.…

Astrophysics · Physics 2009-11-10 Sarmistha Banik , Debades Bandyopadhyay

The core of neutron-star matter is supposed to be at a much higher density than the normal nuclear matter density for which various possibilities have been suggested such as, for example, meson or hyperon condensation and/or deconfined…

High Energy Astrophysical Phenomena · Physics 2011-10-07 Kyungmin Kim , Hyun Kyu Lee , Mannque Rho

We study the phase diagram of a hadronic chiral flavor-SU(3) model. Heavy baryon resonances can induce a phase structure that matches current results from lattice-QCD calculations at finite temperature and baryon density. Furthermore, we…

Nuclear Theory · Physics 2008-11-26 D. Zschiesche , G. Zeeb , S. Schramm

A compact star with superconducting quark core, the hadron crust and the mixed phase between the two is considered. The quark meson coupling model for hadron matter and the color flavor locked quark model for quark matter is used in order…

Astrophysics · Physics 2009-11-11 P. K. Panda , H. S. Nataraj

Matter at high density and low temperature is expected to be a color superconductor, which is a degenerate Fermi gas of quarks with a condensate of Cooper pairs near the Fermi surface that induces color Meissner effects. At the highest…

High Energy Physics - Phenomenology · Physics 2008-12-18 Mark G. Alford , Krishna Rajagopal , Thomas Schaefer , Andreas Schmitt

Substantial experimental and theoretical efforts worldwide are devoted to explore the phase diagram of strongly interacting matter. At LHC and top RHIC energies, QCD matter is studied at very high temperatures and nearly vanishing…

Nuclear Experiment · Physics 2017-03-30 CBM Collaboration , T. Ablyazimov , A. Abuhoza , R. P. Adak , M. Adamczyk , K. Agarwal , M. M. Aggarwal , Z. Ahammed , F. Ahmad , N. Ahmad , S. Ahmad , A. Akindinov , P. Akishin , E. Akishina , T. Akishina , V. Akishina , A. Akram , M. Al-Turany , I. Alekseev , E. Alexandrov , I. Alexandrov , S. Amar-Youcef , M. Anđelić , O. Andreeva , C. Andrei , A. Andronic , Yu. Anisimov , H. Appelshäuser , D. Argintaru , E. Atkin , S. Avdeev , R. Averbeck , M. D. Azmi , V. Baban , M. Bach , E. Badura , S. Bähr , T. Balog , M. Balzer , E. Bao , N. Baranova , T. Barczyk , D. Bartoş , S. Bashir , M. Baszczyk , O. Batenkov , V. Baublis , M. Baznat , J. Becker , K. -H. Becker , S. Belogurov , D. Belyakov , J. Bendarouach , I. Berceanu , A. Bercuci , A. Berdnikov , Y. Berdnikov , R. Berendes , G. Berezin , C. Bergmann , D. Bertini , O. Bertini , C. Beşliu , O. Bezshyyko , P. P. Bhaduri , A. Bhasin , A. K. Bhati , B. Bhattacharjee , A. Bhattacharyya , T. K. Bhattacharyya , S. Biswas , T. Blank , D. Blau , V. Blinov , C. Blume , Yu. Bocharov , J. Book , T. Breitner , U. Brüning , J. Brzychczyk , A. Bubak , H. Büsching , T. Bus , V. Butuzov , A. Bychkov , A. Byszuk , Xu Cai , M. Cálin , Ping Cao , G. Caragheorgheopol , I. Carević , V. Cătănescu , A. Chakrabarti , S. Chattopadhyay , A. Chaus , Hongfang Chen , LuYao Chen , Jianping Cheng , V. Chepurnov , H. Cherif , A. Chernogorov , M. I. Ciobanu , G. Claus , F. Constantin , M. Csanád , N. D'Ascenzo , Supriya Das , Susovan Das , J. de Cuveland , B. Debnath , D. Dementiev , Wendi Deng , Zhi Deng , H. Deppe , I. Deppner , O. Derenovskaya , C. A. Deveaux , M. Deveaux , K. Dey , M. Dey , P. Dillenseger , V. Dobyrn , D. Doering , Sheng Dong , A. Dorokhov , M. Dreschmann , A. Drozd , A. K. Dubey , S. Dubnichka , Z. Dubnichkova , M. Dürr , L. Dutka , M. Dželalija , V. V. Elsha , D. Emschermann , H. Engel , V. Eremin , T. Eşanu , J. Eschke , D. Eschweiler , Huanhuan Fan , Xingming Fan , M. Farooq , O. Fateev , Shengqin Feng , S. P. D. Figuli , I. Filozova , D. Finogeev , P. Fischer , H. Flemming , J. Förtsch , U. Frankenfeld , V. Friese , E. Friske , I. Fröhlich , J. Frühauf , J. Gajda , T. Galatyuk , G. Gangopadhyay , C. García Chávez , J. Gebelein , P. Ghosh , S. K. Ghosh , S. Gläßel , M. Goffe , L. Golinka-Bezshyyko , V. Golovatyuk , S. Golovnya , V. Golovtsov , M. Golubeva , D. Golubkov , A. Gómez Ramírez , S. Gorbunov , S. Gorokhov , D. Gottschalk , P. Gryboś , A. Grzeszczuk , F. Guber , K. Gudima , M. Gumiński , A. Gupta , Yu. Gusakov , Dong Han , H. Hartmann , Shue He , J. Hehner , N. Heine , A. Herghelegiu , N. Herrmann , B. Heß , J. M. Heuser , A. Himmi , C. Höhne , R. Holzmann , Dongdong Hu , Guangming Huang , Xinjie Huang , D. Hutter , A. Ierusalimov , E. -M. Ilgenfritz , M. Irfan , D. Ivanischev , M. Ivanov , P. Ivanov , Valery Ivanov , Victor Ivanov , Vladimir Ivanov , A. Ivashkin , K. Jaaskelainen , H. Jahan , V. Jain , V. Jakovlev , T. Janson , Di Jiang , A. Jipa , I. Kadenko , P. Kähler , B. Kämpfer , V. Kalinin , J. Kallunkathariyil , K. -H. Kampert , E. Kaptur , R. Karabowicz , O. Karavichev , T. Karavicheva , D. Karmanov , V. Karnaukhov , E. Karpechev , K. Kasiński , G. Kasprowicz , M. Kaur , A. Kazantsev , U. Kebschull , G. Kekelidze , M. M. Khan , S. A. Khan , A. Khanzadeev , F. Khasanov , A. Khvorostukhin , V. Kirakosyan , M. Kirejczyk , A. Kiryakov , M. Kiš , I. Kisel , P. Kisel , S. Kiselev , T. Kiss , P. Klaus , R. Kłeczek , Ch. Klein-Bösing , V. Kleipa , V. Klochkov , P. Kmon , K. Koch , L. Kochenda , P. Koczoń , W. Koenig , M. Kohn , B. W. Kolb , A. Kolosova , B. Komkov , M. Korolev , I. Korolko , R. Kotte , A. Kovalchuk , S. Kowalski , M. Koziel , G. Kozlov , V. Kozlov , V. Kramarenko , P. Kravtsov , E. Krebs , C. Kreidl , I. Kres , D. Kresan , G. Kretschmar , M. Krieger , A. V. Kryanev , E. Kryshen , M. Kuc , W. Kucewicz , V. Kucher , L. Kudin , A. Kugler , Ajit Kumar , Ashwini Kumar , L. Kumar , J. Kunkel , A. Kurepin , N. Kurepin , A. Kurilkin , P. Kurilkin , V. Kushpil , S. Kuznetsov , V. Kyva , V. Ladygin , C. Lara , P. Larionov , A. Laso García , E. Lavrik , I. Lazanu , A. Lebedev , S. Lebedev , E. Lebedeva , J. Lehnert , J. Lehrbach , Y. Leifels , F. Lemke , Cheng Li , Qiyan Li , Xin Li , Yuanjing Li , V. Lindenstruth , B. Linnik , Feng Liu , I. Lobanov , E. Lobanova , S. Löchner , P. -A. Loizeau , S. A. Lone , J. A. Lucio Martínez , Xiaofeng Luo , A. Lymanets , Pengfei Lyu , A. Maevskaya , S. Mahajan , D. P. Mahapatra , T. Mahmoud , P. Maj , Z. Majka , A. Malakhov , E. Malankin , D. Malkevich , O. Malyatina , H. Malygina , M. M. Mandal , S. Mandal , V. Manko , S. Manz , A. M. Marin Garcia , J. Markert , S. Masciocchi , T. Matulewicz , L. Meder , M. Merkin , V. Mialkovski , J. Michel , N. Miftakhov , L. Mik , K. Mikhailov , V. Mikhaylov , B. Milanović , V. Militsija , D. Miskowiec , I. Momot , T. Morhardt , S. Morozov , W. F. J. Müller , C. Müntz , S. Mukherjee , C. E. Muńoz Castillo , Yu. Murin , R. Najman , C. Nandi , E. Nandy , L. Naumann , T. Nayak , A. Nedosekin , V. S. Negi , W. Niebur , V. Nikulin , D. Normanov , A. Oancea , Kunsu Oh , Yu. Onishchuk , G. Ososkov , P. Otfinowski , E. Ovcharenko , S. Pal , I. Panasenko , N. R. Panda , S. Parzhitskiy , V. Patel , C. Pauly , M. Penschuck , D. Peshekhonov , V. Peshekhonov , V. Petráček , M. Petri , M. Petriş , A. Petrovici , M. Petrovici , A. Petrovskiy , O. Petukhov , D. Pfeifer , K. Piasecki , J. Pieper , J. Pietraszko , R. Płaneta , V. Plotnikov , V. Plujko , J. Pluta , A. Pop , V. Pospisil , K. Poźniak , A. Prakash , S. K. Prasad , M. Prokudin , I. Pshenichnov , M. Pugach , V. Pugatch , S. Querchfeld , S. Rabtsun , L. Radulescu , S. Raha , F. Rami , R. Raniwala , S. Raniwala , A. Raportirenko , J. Rautenberg , J. Rauza , R. Ray , S. Razin , P. Reichelt , S. Reinecke , A. Reinefeld , A. Reshetin , C. Ristea , O. Ristea , A. Rodriguez Rodriguez , F. Roether , R. Romaniuk , A. Rost , E. Rostchin , I. Rostovtseva , Amitava Roy , Ankhi Roy , J. Rożynek , Yu. Ryabov , A. Sadovsky , R. Sahoo , P. K. Sahu , S. K. Sahu , J. Saini , S. Samanta , S. S. Sambyal , V. Samsonov , J. Sánchez Rosado , O. Sander , S. Sarangi , T. Satława , S. Sau , V. Saveliev , S. Schatral , C. Schiaua , F. Schintke , C. J. Schmidt , H. R. Schmidt , K. Schmidt , J. Scholten , K. Schweda , F. Seck , S. Seddiki , I. Selyuzhenkov , A. Semennikov , A. Senger , P. Senger , A. Shabanov , A. Shabunov , Ming Shao , A. D. Sheremetiev , Shusu Shi , N. Shumeiko , V. Shumikhin , I. Sibiryak , B. Sikora , A. Simakov , C. Simon , C. Simons , R. N. Singaraju , A. K. Singh , B. K. Singh , C. P. Singh , V. Singhal , M. Singla , P. Sitzmann , K. Siwek-Wilczyńska , L. Škoda , I. Skwira-Chalot , I. Som , Guofeng Song , Jihye Song , Z. Sosin , D. Soyk , P. Staszel , M. Strikhanov , S. Strohauer , J. Stroth , C. Sturm , R. Sultanov , Yongjie Sun , D. Svirida , O. Svoboda , A. Szabó , R. Szczygieł , R. Talukdar , Zebo Tang , M. Tanha , J. Tarasiuk , O. Tarassenkova , M. -G. Târzilă , M. Teklishyn , T. Tischler , P. Tlustý , T. Tölyhi , A. Toia , N. Topil'skaya , M. Träger , S. Tripathy , I. Tsakov , Yu. Tsyupa , A. Turowiecki , N. G. Tuturas , F. Uhlig , E. Usenko , I. Valin , D. Varga , I. Vassiliev , O. Vasylyev , E. Verbitskaya , W. Verhoeven , A. Veshikov , R. Visinka , Y. P. Viyogi , S. Volkov , A. Volochniuk , A. Vorobiev , Aleksey Voronin , Alexander Voronin , V. Vovchenko , M. Vznuzdaev , Dong Wang , Xi-Wei Wang , Yaping Wang , Yi Wang , M. Weber , C. Wendisch , J. P. Wessels , M. Wiebusch , J. Wiechula , D. Wielanek , A. Wieloch , A. Wilms , N. Winckler , M. Winter , K. Wiśniewski , Gy. Wolf , Sanguk Won , Ke-Jun Wu , J. Wüstenfeld , Changzhou Xiang , Nu Xu , Junfeng Yang , Rongxing Yang , Zhongbao Yin , In-Kwon Yoo , B. Yuldashev , I. Yushmanov , W. Zabołotny , Yu. Zaitsev , N. I. Zamiatin , Yu. Zanevsky , M. Zhalov , Yifei Zhang , Yu Zhang , Lei Zhao , Jiajun Zheng , Sheng Zheng , Daicui Zhou , Jing Zhou , Xianglei Zhu , A. Zinchenko , W. Zipper , M. Żoładź , P. Zrelov , V. Zryuev , P. Zumbruch , M. Zyzak

Using variational methods, we numerically investigate the matrix model for the two-color QCD coupled to a single quark (matrix-QCD$_{2,1}$) in the limit of ultra-strong Yang-Mills coupling ($g =\infty$). The spectrum of the model has…

High Energy Physics - Theory · Physics 2024-06-11 Nirmalendu Acharyya , Prasanjit Aich , Arkajyoti Bandyopadhyay , Sachindeo Vaidya