English
Related papers

Related papers: Mapping the QCD Phase Diagram

200 papers

Cold three flavor quark matter at large (but not asymptotically large) densities may exist in a crystalline color superconducting phase. These phases are characterized by a gap parameter $\Delta$ that varies periodically in space, forming a…

High Energy Physics - Phenomenology · Physics 2010-05-27 Massimo Mannarelli , Rishi Sharma

The QCD phase diagram at finite temperature and density has attracted considerable interest over many decades now, not least because of its relevance for a better understanding of heavy-ion collision experiments. Models provide some insight…

High Energy Physics - Phenomenology · Physics 2017-04-05 Paul Springer , Jens Braun , Stefan Rechenberger , Fabian Rennecke

We present an overview of selected aspects of ultrarelativistic nucleus-nucleus collisions, a research program devoted to the study of strongly interacting matter at high energy densities and in particular to the characterization of the…

High Energy Physics - Phenomenology · Physics 2015-06-25 A. Andronic , P. Braun-Munzinger

A collection of the physical observables, related to the electromagnetic properties of a nucleon, to investigate the non--perturbative quantum fluctuations in the strong interaction vacuum state under the influence of at least one close by…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Ying

The presence of quark matter in neutron stars may affect several neutron star observables and the neutrino signal in core-collapse supernovae. These observables are sensitive to the phase of quark matter that is present in compact objects.…

Nuclear Theory · Physics 2009-11-11 Andrew W. Steiner

We present a novel framework for the equation of state of dense and hot Quantum Chromodynamics (QCD), which focuses on the region of the phase diagram relevant for neutron star mergers and core-collapse supernovae. The model combines…

High Energy Physics - Phenomenology · Physics 2023-11-09 Tuna Demircik , Christian Ecker , Matti Järvinen

I show an updated QCD phase diagram with recent developments from chiral effective theories and phenomenological models. Expected signals of a QCD critical point accessible in heavy-ion collisions are also discussed. In particular,…

High Energy Physics - Phenomenology · Physics 2009-11-18 Chihiro Sasaki

The QCD transition from a hadronic to a quark-gluon plasma phase is a cross-over at vanishing/small baryo-chemical potential, while at higher chemical potentials it is argued that it becomes of first order, ending with a critical end-point.…

High Energy Physics - Phenomenology · Physics 2020-12-30 M. Motta , W. M. Alberico , A. Beraudo , P. Costa , R. Stiele

After a very brief overview recollecting the `classic' parts of QCD, that is its application to describe hard processes and static properties of hadrons, I survey recent work -- some very recent -- on QCD at non-zero temperature and…

High Energy Physics - Phenomenology · Physics 2009-10-31 Frank Wilczek

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

Fluctuations provide a powerful tool for elucidating the nature of strongly-interacting matter in the QCD phase diagram. In heavy-ion-collision systems, the net-particle number fluctuations are captured at the moment of chemical freeze-out.…

Nuclear Theory · Physics 2023-03-15 Jamie M. Karthein

We use the linear sigma model with two flavors of quarks to study the phase diagram at finite temperature and baryon chemical potential as a function of the vacuum pion mass. Our calculations include thermal fluctuations of both the bosonic…

Nuclear Theory · Physics 2014-11-20 J. I. Kapusta , E. S. Bowman

Neither the chiral limit nor finite baryon density can be simulated directly in lattice QCD, which severely limits our understanding of the QCD phase diagram. In this review I collect results for the phase structure in an extended parameter…

High Energy Physics - Lattice · Physics 2019-12-11 Owe Philipsen

Employing an extended three flavor version of the NJL model we discuss in detail the phase diagram of quark matter. The presence of quark as well as of diquark condensates gives raise to a rich structure of the phase diagram. We study in…

High Energy Physics - Phenomenology · Physics 2009-11-07 F. Gastineau , R. nebauer , J. Aichelin

Important progress in understanding the behavior of hadronic matter at high density has been achieved recently, by adapting the techniques of condensed matter theory. At asymptotic densities, the combination of asymptotic freedom and BCS…

High Energy Physics - Phenomenology · Physics 2016-11-23 Krishna Rajagopal , Frank Wilczek

We study finite density QCD in an approximation in which the interaction between quarks is modelled on that induced by instantons. We sketch the mechanism by which chiral symmetry restoration at finite density occurs in this model. At all…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. Alford , K. Rajagopal , F. Wilczek

The QCD phase diagram may feature a critical end point at a temperature T and baryon chemical potential $\mu$ which is accessible in heavy ion collisions. The universal long wavelength fluctuations which develop near this Ising critical…

High Energy Physics - Phenomenology · Physics 2009-10-31 Boris Berdnikov , Krishna Rajagopal

Within a quasi-particle model for the equation of state of strongly interacting matter for two quark flavors we include phenomenologically features of the QCD critical point and discuss its impact on the equation of state. In particular, we…

High Energy Physics - Phenomenology · Physics 2009-04-14 M. Bluhm , B. Kampfer

We discuss the interplay between two first-principles calculations of QCD at high density: perturbative results in the weak-coupling regime and the recent lattice-QCD result at finite isospin density. By comparing these two results, we…

High Energy Physics - Phenomenology · Physics 2024-09-09 Yuki Fujimoto

We investigate color superconductivity on the lattice using the gap equation for the Cooper pair condensate. The weak coupling analysis is justified by choosing the physical size of the lattice to be smaller than the QCD scale, while…

High Energy Physics - Lattice · Physics 2023-06-28 Takeru Yokota , Yuta Ito , Hideo Matsufuru , Yusuke Namekawa , Jun Nishimura , Asato Tsuchiya , Shoichiro Tsutsui