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We first introduce the conceptual basis of critical behaviour in strongly interacting matter, with colour deconfinement as QCD analog of the insulator-conductor transition and chiral symmetry restoration as special case of the associated…

High Energy Physics - Phenomenology · Physics 2016-09-06 Helmut Satz

Despite quantum chromodynamics (QCD) being established as the theory of the strong interaction and its many successes since then, significant challenges in our understanding of hadron physics remain. The lack of a full understanding for how…

High Energy Physics - Lattice · Physics 2024-02-09 Andrew D. Hanlon

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

The QCD cross-over line in the temperature ($T$) -- baryo-chemical potential ($\mu_B$) plane has been computed by several lattice groups by calculating the chiral order parameter and its susceptibility at finite values of $\mu_B$. In this…

The phase transition calculations are utilized for an in-depth understanding of the thermodynamics of the deconfinement transition to perform the best analysis of the QCD phase diagram. The phenomenological justifications for a mathematical…

Nuclear Theory · Physics 2023-03-07 Mahboubeh Shahrbaf

The quark-hadron transition that happens in ultra-relativistic heavy-ion collisions is expected to be influenced by the effects of rotation and magnetic field, both present due to the geometry of a generic non-head-on impact. We augment the…

High Energy Physics - Phenomenology · Physics 2023-10-12 Gaurav Mukherjee , D. Dutta , D. K. Mishra

After decades of painstaking research, the field of heavy ion physics has reached an exciting new era. Evidence is mounting that we can create a high temperature, high density, strongly interacting ``bulk matter'' state in the laboratory --…

Nuclear Experiment · Physics 2017-08-23 Mark D. Baker

I report the results of a series of works on the phase diagram of theories with a different number of colors and/or quarks in a different representation than in QCD. Similarities as well as differences as compared to the real world are…

High Energy Physics - Phenomenology · Physics 2011-06-15 Tomas Brauner

At sufficiently high temperature and density, quantum chromodynamics (QCD) predicts phase transition from the hadronic phase to the quark-gluon plasma phase. Lattice QCD is the most useful tool to investigate this critical phenomenon, which…

High Energy Physics - Phenomenology · Physics 2017-08-23 Xiang-Qian Luo , Eric B. Gregory , Shuo-Hong Guo , Helmut Kroger

Starting from Wilson's action, we calculate strong coupling series for the Polyakov loop susceptibility in lattice gauge theories for various small N_\tau in the thermodynamic limit. Analysing the series with Pad\'e approximants, we…

High Energy Physics - Lattice · Physics 2015-05-14 Jens Langelage , Owe Philipsen

The theory of Quantum Chromo Dynamics (QCD) reproduces the strong interaction at distances much shorter than the size of the nucleon. At larger distance scales, the generation of hadron masses and confinement cannot yet be derived from…

High Energy Physics - Experiment · Physics 2019-08-13 J. G. Messchendorp

Rich experimental data have been collected in heavy-ion collisions at high energies to study the properties of strongly interacting matter. As the theory of strong interactions, QCD, predicts asymptotic freedom, the created matter at…

Nuclear Experiment · Physics 2015-06-03 Anar Rustamov

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

It is generally known for $\mathrm{U}(N)$ gauge theory at finite temperature that phase transitions are manifested by taking the large-$N$ limit. Since the large-$N$ theory undergoes two thermodynamic phase transitions, a nontrivial…

High Energy Physics - Theory · Physics 2024-05-01 Hiromasa Watanabe

This course consists of two lectures. In the first lecture I discuss why a non perturbative formulation of QCD is needed, and I show that lattice formulation copes with this need, even if it mainly produces numerical results. In the second…

High Energy Physics - Lattice · Physics 2009-11-07 A. Di Giacomo

The quantum chromodynamics (QCD) phase diagram, which reveals the state of strongly interacting matter at different temperatures and densities, is key to answering open questions in physics, ranging from the behavior of particles in neutron…

When quarks and gluons are led to form a dense medium, like in high energy or/and heavy-ion collisions, it is interesting to ask the question which are the relevant degrees of freedom that Quantum Chromodynamics predict. The present notes…

High Energy Physics - Phenomenology · Physics 2007-05-23 Robi Peschanski

I discuss the phase structure of strongly interacting matter at high temperatures and densities, as predicted by statistical QCD, and consider in particular the nature of the transition of hot hadronic matter to a plasma of deconfined…

High Energy Physics - Phenomenology · Physics 2007-05-23 H. Satz

The cosmological QCD phase transition is studied in terms of the color confinement at finite temperature using the dual Higgs theory of QCD. The confinement force is largely reduced at high temperature, which leads to the swelling of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Hideo Suganuma , Hiroko Ichie , Hideko Monden , Shoichi Sasaki , Manabu Orito , Tadahiro Yamamoto , Toshitaka Kajino