Global Beam Energy Scan Global Beam Energy Scan

Slides:



Advertisements
Similar presentations
Hydrodynamical description of first order phase transitions Vladimir Skokov (GSI, Darmstadt) in collaboration with D. N. Voskresensky Strongly Interacting.
Advertisements

Mass, Quark-number, Energy Dependence of v 2 and v 4 in Relativistic Nucleus- Nucleus Collisions Yan Lu University of Science and Technology of China Many.
Supported by DOE 11/22/2011 QGP viscosity at RHIC and LHC energies 1 Huichao Song 宋慧超 Seminar at the Interdisciplinary Center for Theoretical Study, USTC.
The Physics of Dense Nuclear Matter
Nuclear matter 1) Introduction 2) Nuclear matter in the ground state 3) Hot and dense nuclear matter 4) State equation of nuclear matter 5) Phase diagram.
Bucharest emulsion group along the time Who we are.
17-Nov-2004G.S.F.Stephans Exploring the Phase Diagram of Strongly Interacting Matter Exploring the Phase Diagram: The RHIC Contribution  RHIC is currently.
Experimental Results for Fluctuations And Correlations as a Signature of QCD Phase Transitions in Heavy Ion Collisions Gary Westfall Michigan State University,
Relativistic Heavy Ions Experiment I. The QCD Phasediagram.
5-12 April 2008 Winter Workshop on Nuclear Dynamics STAR Particle production at RHIC Aneta Iordanova for the STAR collaboration.
Thermal Photons and Dileptons Workshop BNL, August 20-22, 2014 Itzhak Tserruya Dilepton Experiments – Overview (From √s NN = 2 GeV up to 7 TeV)
March 1, 2003University of Rochester - Graduate Student Days1 Nuclear Physics at the University of Rochester Steven Manly Grad. Student Days March 1, 2003.
Supriya Das SQM 2006, 26th March 2006, UCLA 1 Event By Event Fluctuation in K/  ratio atRHIC Supriya Das § VECC, Kolkata (for STAR Collaboration) § Present.
QCD Phase Boundary and the Critical Point B. Mohanty (1), X.F. Luo (2,3), H.G. Ritter (3) and N. Xu (3) (1)VECC, Kolkata, , India (2)Modern Physics.
Christina Markert Physics Workshop UT Austin November Christina Markert The ‘Little Bang in the Laboratory’ – Accelorator Physics. Big Bang Quarks.
The Project NICA/MPD at JINR (Dubna) Search for the Mixed Phase of Strongly Interacting Matter at Nuclotron-based Ion Collider FAcility (1  1.5)·10 27.
1 NA49/NA61: results and plans on beam energy and system size scan at the CERN SPS Onset of deconfinement: - NA49 evidence - NA61 systematic study Critical.
1 QM2006 D.I.Lowenstein RHIC : The Path Forward Presented to Quark Matter 2006 Shanghai, PRC Derek I. Lowenstein Brookhaven National Laboratory November.
RESEARCH POSTER PRESENTATION DESIGN © The RHIC Beam Energy Scan (BES) was proposed to search for the possible critical.
1 Plans for JINR participation at FAIR JINR Contributions: ● Accelerator Complex ● Condensed Baryonic Matter ● Antiproton Physics ● Spin Physics Physics.
Summer Student Practice, Dubna, 2009 Analysis of UrQMD Data Obtained for Relativistic Au+Au Collisions at 17.3 GeV for STAR detector F. Nemulodi, M.W.
Roy A. Lacey (SUNY Stony Brook ) C ompressed B aryonic at the AGS: A Review !! C ompressed B aryonic M atter at the AGS: A Review !!
A.N.Sissakian, A.S.Sorin Very High Multiplicity Physics Seventh International Workshop JINR, Dubna, September 18, 2007 Status of the project NICA/MPD at.
1 Jeffery T. Mitchell – Quark Matter /17/12 The RHIC Beam Energy Scan Program: Results from the PHENIX Experiment Jeffery T. Mitchell Brookhaven.
HIGGS BOSON – ON YOUR OWN T. Csörgő 1 | 17 T. Csörgő Wigner RCP, Budapest, Hungary wigner.mta.hu.
Hadron Collider Physics 2012, 12/Nov/2012, KyotoShinIchi Esumi, Univ. of Tsukuba1 Heavy Ion results from RHIC-BNL ShinIchi Esumi Univ. of Tsukuba Contents.
Report from India Topical Conference on Hadron Collider Physics XIII Jan 14-20, TIFR, India Naohito Saito RIKEN/ RIKEN BNL Research Center.
QuarkNet 2006 Lets go smash some Atoms! Peripheral Collision:Central Collision Head-On Collision: Largest # of Nucleons Participate Glancing Collision:
International Accelerator Facility for Beams of Ions and Antiprotons at Darmstadt Construction of FAIR Phase-1 December 2005 J. Eschke, GSI Construction.
C H I C Charm in Heavy Ion SPS 1.J/  – Suppression in A+A 2.CHIC – Physics motivations 3.CHIC – Experimental aspects 1F. Fleuret - LLR.
1 Guannan Xie Nuclear Modification Factor of D 0 Mesons in Au+Au Collisions at √s NN = 200 GeV Lawrence Berkeley National Laboratory University of Science.
A.G. Olshevskiy 104 th Session of the JINR Scientific Council.
1 M. Gazdzicki Frankfurt, Kielce Observation of the onset of deconfinement and Search for the critical point Past and future of the ion physics at the.
1 Heavy-Ion Physics at J-PARC Shoji Nagamiya RIKEN / KEK / JAEA January 20, 2016 Tokai 1) Motivation 2) J-PARC vs. FAIR.
NA61 ION PROGRAM M. RYBCZYŃSKI for the NA61 Collaboration Institute of Physics, Jan Kochanowski University Kielce, Poland.
1 Furture of heavy ion collisions: → Fluctuations: → M.G., Frankfurt, Kielce, Why event-by-event fluctuations? Towards ideal detectors Experimental.
1 M. Gazdzicki, Frankfurt, Kielce for the NA61 Collaboration Onset of Deconfinement and Critical Point: Nucleus-Nucleus Program of NA61/SHINE Fundamentals.
Quark Gluon Plasma Researches at RHIC/LHC Fuqiang Wang Purdue University Tsukuba Global Science Week 2016 Session #6 "Universe Evolution and Matter Origin"
History, status and future of multi-particle production in
Perspectives for Heavy-Ion Collisions at Future Facilities
Prospects for Flow Measurements at Low Energies
(SHINE – SPS Heavy Ion and Neutrino Experiment)
CBM and the nuclear matter EOS
The 'Little Bang’ in the Laboratory - Physics at the LHC
? ? Nucleus-nucleus collisions in NA61/SHINE
A heavy-ion experiment at the future facility at GSI
25 Years of Dilepton Experiments
Veksler and Baldin Laboratory
RHIC-BES program as a path towards future HIC(sPHENIX/J-parc)
Search for the critical point of strongly interacting matter
of secondary light ion beams
of secondary light ion beams
NA61/SHINE: status and energy scans with Pb+Pb collisions
Are Flow Measurements at RHIC reliable?
Collective Dynamics at RHIC
NUCLEUS-NUCLEUS COLLISION Centrality Determination For NICA/MPD
Current and Future Status of Heavy Ion Physics
Current Heavy Ion Physics Experiments and Results Survey
Introduction Results Methods Conclusions
Project "Nuclotron M" / NICA
Many Thanks to Organizers!
Summary Model Data from RHIC experiments Introduction
What have we learned from Monte Carlo models? HIJING
The Study of Elliptic Flow for PID Hadron at RHIC-PHENIX
Multiplicity Dependence of Charged Particle, φ Meson and Multi-strange Particle Production in p+p Collisions at
What have we learned from Anisotropic Flow at RHIC ?
Relativistic Heavy Ion Collisions 相对论重离子碰撞
Relativistic heavy ion collisions
Claudia Höhne, GSI Darmstadt
JLEIC Accelerator R&D Meeting
Presentation transcript:

Global Beam Energy Scan Global Beam Energy Scan BNL AGS CERN SPS BNL RHIC CERN LHC E895 NA61 STAR ALICE rich experimental data: on Pb+Pb and p+p interactions from several GeV to several TeV Global Beam Energy Scan is well advanced ! M. Gazdzicki, Frankfurt, Kielce

Basic goals: -study properties of strongly interacting matter, -in particular, what are its phases and how do transitions between them look like, Basic assumptions (consistent with data): -strongly interacting matter (a large system close to equilibrium) is created at the early stage of collisions, -its energy density increases with collision energy Basic drawback: -absence of SM (QCD) predictions

Popular phase diagram of strongly interacting matter

Global Beam Energy Scan is mostly - the by-product of the global race to construct larger and more powerful accelerators and - the product of dedicated programs at the already constructed facilities. The systematic results in full energy range only for Pb+Pb (Au+Au) collisions, significantly poorer data for p+p and light ion interactions.

accelerator, laboratory Brief history of beam energy scan programs important energy limit data taking accelerator, laboratory 1970-1990 Synchrophasotron, JINR, Dubna, up to 5A GeV 1975-1993: Bevalac, LBL, Berkeley, up to ≈2A GeV 1990-now: SIS, GSI, Darmstadt, up to ≈2A GeV 1996-1997: AGS, BNL, Brookhaven, up to ≈10A GeV 1998-2002: SPS, CERN, Geneva, up to ≈200A GeV 2009-2011: RHIC, BNL, Brookhaven down to ≈30A GeV 2011-2015: SPS, CERN, Geneva, up to ≈200A GeV All energies (kinetic ...-AGS, total SPS-...) in the fixed target system

Bevalac, LBL, Berkeley (1975-1993) Ar+KCL at 1.8A GeV

Bevalac, LBL, Berkeley (1975-1993) Bevelac ≡ Bevatron (1954) + SuperHILAC (1971) Key experiments: Nagamiya's spectrometer: PRC 24, 971 (81) Streamer Chamber: PRL 45, 874 (80) Plastic Ball/Wall: PL 142B, 141 (84) EOS: PRL 75, 2662 (95)

Bevalac, LBL, Berkeley (1975-1993) central Ar+KCl Kinetic energy: 0.25A - 2.1A GeV Ion beams: from p to Au Targets: various nuclei Results on multi-fragmentation and hadron production 2-5 k events per reaction

SIS-18, GSI, Darmstadt (1990-now) Ni+Ni at 1.95A GeV

SIS-18, GSI, Darmstadt (1990-now) SIS = Heavy Ion Synchrotron, 18 Tm Key experiments: FOPI: PLB 612, 173 (05) KaoS: J.Phys. G31, S693 (05) ALADIN PRL 94, 162701 (05) HADES PR C84, 014902 (11) Kinetic energy: 0.05A - 2.0A GeV Ion beams: from p to Au Targets: from p to Au

SIS-18, GSI, Darmstadt (1990-now)

AGS, BNL, Brookhaven (1996-1997) Au+Au at 4A GeV Alternating Gradient Synchrotron (1954) + AGS Booster (1991) Au+Au at 4A GeV The EOS Time Projection Chamber was the first TPC used in heavy ion experiments: first in EOS at Bevelac and then in E895 at AGS

AGS, BNL, Brookhaven (1996-1997) Key experiments: E866, E917 (E802, E859): PLB 490, 53 (00) E895: PRL 88, 102301 (02) Kinetic energy: 1.96A, 4.00A, 5.93A, 7.94A (10.74A) GeV Ion beams: Au Targets: Au

AGS, BNL, Brookhaven (1996-1997) central Au+Au

AGS, BNL, Brookhaven (1996-1997) central Au+Au

SPS, CERN, Geneva (1998-2002) Super Proton Synchrotron (1976), ions since (1986)

SPS, CERN, Geneva (1998-2002) Key experiments: NA49: PR C77, 024903 (02) NA57: PL B595, 68 (04) NA45: NP A727, 97 (03) Energy: 20A, 30A, 40A, 80A (158A) GeV Ion beams: Pb (0, S) Targets: Pb (S, Cu)

SPS, CERN, Geneva (1998-2002) central Pb+Pb

SPS, CERN, Geneva (1998-2002) central Pb+Pb (Au+Au)

RHIC, BNL, Brookhaven (2009-2011) Relativistic Heavy Ion Collider (2000) Au+Au at 7.6 GeV (30A GeV)

RHIC, BNL, Brookhaven (2009-2011) Key experiments: STAR: PR C81, 024911 (10) PHENIX: J. Phys. G38, 124146 (11) Energy: 7.7, 9.2, 11.5, 19.6, 27.0, 39.0 (62, 200) GeV (N+N c.m.s. energy) Ions: Au + Au

RHIC, BNL, Brookhaven (2009-2011) Au+Au at 39 GeV

SPS, CERN, Geneva (2011-2015) Be+Be at 158A GeV

SPS, CERN, Geneva (2011-2015) Only one experiment: NA61/SHINE: PR C84, 034604 (11) Energy: 13A, 20A, 30A, 40A, 80A (158A) GeV Ion beams: (p), Be, Ar and Xe Targets: (p), Be, Ca and La

SPS, CERN, Geneva (2011-2015) Be+Be at 150A GeV UNCORRECTED

Present and future heavy ion experimental programs LHC RHIC energy accelerator/exps (GeV) accelerator/exps 1 SIS-18/HADES SIS-100/HADES-CBM SPS NICA 10 SPS/NA61 NICA/MPD SIS-18 SIS-100 100 RHIC/STAR,PHENIX 1000 LHC/ALICE,ATLAS,CMS

NICA, JINR, Dubna (2017-...) Experiments: MPD, SPD: NICA = Nuclotron based Ion Collider fAcility Experiments: MPD, SPD: Energy: 4-11 GeV (N+N c.m.s. energy), Beams: from p to Au

Nuclotron, JINR, Dubna (2015-...) Experiment: BM@N Energy: up to 6A GeV, Beams: from p to Au

SIS-100, FAIR, Darmstadt (2019-...) Experiments: HADES, CBM: Energy: up to 14A GeV, Beams: from p to Au

Do we need energy scan at LHC, CERN, Geneva ? Experiments: ALICE, CMS, ATLAS: Energy: 400 – 5400 GeV Beams: from p to Au

Do we need energy scan at LHC, CERN, Geneva ? central Pb+Pb (Au+Au) Smooth evolution of hadron production properties from the top SPS to the almost top LHC energy There is no strong motivation for a beam energy scan at LHC. However would be desirable to close the large gap between the top RHIC and LHC energies.