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At high temperatures and densities the nuclear matter undergoes a phase transition to a new state of matter called quark gluon plasma (QGP). This new state of matter which existed in the universe after a few microsecond of the big bang can…

Nuclear Theory · Physics 2012-03-15 Jan-e Alam

Quantum chromodynamics (QCD) phase diagram is usually plotted as temperature (T) versus the chemical potential associated with the conserved baryon number (\mu_{B}). Two fundamental properties of QCD, related to confinement and chiral…

Nuclear Experiment · Physics 2011-07-06 Bedangadas Mohanty

We propose a scheme to determine the chemical potential and baryon number density of the hadron-quark phase transition in cold dense strong interaction matter (compact star matter). The hadron matter is described with the relativistic mean…

High Energy Physics - Phenomenology · Physics 2023-05-26 Zhan Bai , Yu-xin Liu

A charmed quark experiences drag and diffusion in the quark-gluon plasma, as well as strong interaction with the plasma surface. Our simulations indicate that charmed quarks created in heavy ion collisions will be trapped in the mixed phase…

High Energy Physics - Phenomenology · Physics 2007-05-23 Benjamin Svetitsky , Asher Uziel

We extend our proposal that major universality classes of hadronic matter can be understood, and in favorable cases calculated, directly in the microscopic quark variables, to allow for splitting between strange and light quark masses. A…

High Energy Physics - Phenomenology · Physics 2009-10-31 Thomas Schaefer , Frank Wilczek

The energy densities achieved during central collisions of large nuclei at Brookhaven's AGS may be high enough to allow the formation of quark--gluon plasma. Calculations based on relativistic nucleation theory suggest that rare events,…

Nuclear Theory · Physics 2009-09-25 J. I. Kapusta , R. Venugopalan , A. P. Vischer

The size of the average fluctuations of net baryon number and electric charge in a finite volume of hadronic matter differs widely between the confined and deconfined phases. These differences may be exploited as indicators of the formation…

High Energy Physics - Phenomenology · Physics 2009-10-09 Masayuki Asakawa , Ulrich Heinz , Berndt Muller

I use simple thermodynamic reasoning to argue that at temperatures of order a trillion kelvin, QCD, the theory which describes strongly interacting particles such as protons and neutrons under normal conditions, undergoes a phase transition…

Physics Education · Physics 2008-11-26 Simon Hands

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

Lattice QCD predicts a phase transition between hadronic matter and a system of deconfined quarks and gluons (the Quark Gluon Plasma) at high energy densities. Recent results from the Brookhaven Relativistic Heavy Ion Collider (RHIC)…

Nuclear Experiment · Physics 2007-05-23 Raimond Snellings

Lattice QCD predicts a phase transition between hadronic matter and a system of deconfined quarks and gluons (the Quark Gluon Plasma) at high energy densities. Recent results from the Brookhaven Relativistic Heavy Ion Collider (RHIC)…

High Energy Physics - Experiment · Physics 2007-05-23 Raimond Snellings

We study two-color QCD with two flavors of Wilson fermion as a function of quark chemical potential mu and temperature T. We find evidence of a superfluid phase at intermediate mu and low T where the quark number density and diquark…

High Energy Physics - Lattice · Physics 2012-10-26 Seamus Cotter , Jon-Ivar Skullerud , Pietro Giudice , Simon Hands , Seyong Kim , Dhagash Mehta

Our current knowledge of the quark-gluon plasma in thermodynamical equilibrium is reviewed. The phase diagram of strongly interacting matter is discussed, with emphasis on the quark-hadron phase transition and the color-superconducting…

Nuclear Theory · Physics 2014-11-18 Dirk H. Rischke

Matter described by Quantum Chromodynamics (QCD), the theory of strong interactions, may undergo phase transitions when its temperature and the chemical potentials are varied. QCD at finite temperature is studied in the laboratory by…

High Energy Physics - Phenomenology · Physics 2011-06-24 Sourendu Gupta , Xiaofeng Luo , Bedangadas Mohanty , Hans Georg Ritter , Nu Xu

In this paper we carry out a low-temperature scan of the phase diagram of dense two-color QCD with $N_f=2$ quarks. The study is conducted using lattice simulation with rooted staggered quarks. At small chemical potential we observe the…

High Energy Physics - Lattice · Physics 2016-12-19 V. V. Braguta , E. -M. Ilgenfritz , A. Yu. Kotov , A. V. Molochkov , A. A. Nikolaev

We consider the variation of the strange quark-chemical potential in the phase diagramme of nuclear matter, employing the order parameters and mass-scaled partition functions in each domain and enforcing flavour conservation. Assuming the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Apostolos D. Panagiotou , Panayotis G. Katsas

Lattice QCD results reveal that the critical parameters and the order of the quark-hadron phase transition are quite sensitive to the number of dynamical flavours and their masses included in the theory. Motivated by this result we develop…

High Energy Physics - Phenomenology · Physics 2007-05-23 B. K. Patra , K. K. Singh , C. P. Singh

We discuss two special limiting forms of QCD matter which may be produced at RHIC. We conclude from the available empirical evidence that an equilibrated, but strongly coupled Quark Gluon Plasma has been made in such collisions. We also…

Nuclear Theory · Physics 2009-10-09 Miklos Gyulassy , Larry McLerran

At high temperatures, strongly interacting matter becomes a plasma of deconfined quarks and gluons. In statistical QCD, deconfinement and the properties of the resulting quark-gluon plasma can be investigated by studying the in-medium…

High Energy Physics - Phenomenology · Physics 2009-11-11 Helmut Satz

We discuss the phase structure of quantum chromodynamics (QCD) with two colors and two flavors of light quarks. This is motivated by the increasing interest in the QCD phase diagram as follows: (1) The QCD critical point search has been…

High Energy Physics - Phenomenology · Physics 2010-06-09 Tomas Brauner , Kenji Fukushima , Yoshimasa Hidaka