Critical vs. spurious fluctuations in the search for the QCD critical point
|
|
- Gervase Warren
- 5 years ago
- Views:
Transcription
1 Critical vs. spurious fluctuations in the search for the QCD critical point Maurício Hippert Eduardo S. Fraga Edivaldo M. Santos Instituto de Física - Universidade Federal do Rio de Janeiro June 16, 2016 Maurício Hippert (IF-UFRJ) Critical vs. spurious fluctuations June 16, / 13
2 Outline 1 Motivation 2 Effective model 3 Limitations 4 Results 5 Final remarks Maurício Hippert (IF-UFRJ) Critical vs. spurious fluctuations June 16, / 13
3 Motivation The QCD critical point T, GeV QGP 0.1 crossover critical point hadron gas vacuum nuclear matter quark matter phases CFL 0 1 µ B, GeV Figure: A semiquantitative representation of the QCD phase diagram. Ref.: M. Stephanov (2006). Can heavy ion collisions reach the neighborhood of the critical point? Is it there? What would its signatures be? Maurício Hippert (IF-UFRJ) Critical vs. spurious fluctuations June 16, / 13
4 Motivation Experimental signatures Theory ξ : long range fluctuations (pions, protons...). Statistical moments of observables (e.g. ( N) 3 ) as signatures in HICs (focus: multiplicity). Reality (HICs) Spurious contributions, finite size/duration: ξ... Do signatures survive, even in a simplified model? Need to test basic realistic ingredients! Mission: Test signatures under the most optimistic scenario Maurício Hippert (IF-UFRJ) Critical vs. spurious fluctuations June 16, / 13
5 Effective model Critical fluctuations Critical mode Classical treatment with homogeneous approximation a Ω[σ 0 ] = V ( ) Ω[σ0 ] P σ0 [σ 0 ] exp, (1) T ( m 2 σ 2 σ2 0+ λ 3 3 σ3 0 + λ ) 4 4 σ4 0 +, (2) with m σ ξ 1, λ 3 T (T ξ) 3/2, λ 4 (T ξ) 1. a Stephanov, Rajagopal, Shuryak (1999); Stephanov (2009); Tsypin (1996). Distribution changes at the CEP change in cumulants! Maurício Hippert (IF-UFRJ) Critical vs. spurious fluctuations June 16, / 13
6 Effective model Framework Interaction Mass correction δm 2 π = 2G δσ 0, δm p = g δσ 0 (G 300MeV, g 10). (3) Fluctuations of σ change m, change distribution of particles. Freeze-out near the CEP possible observation. Correlated fluctuations of observables signal. Analytically, expansion in δσ 0 followed by average. Framework for Monte Carlo simulations! Background can be added! Maurício Hippert (IF-UFRJ) Critical vs. spurious fluctuations June 16, / 13
7 Limitations HICs background contributions In HICs, not everything is under control 1 Gaussian temperature fluctuations (σ T = 5%) 2 Geometrical fluctuations (below) Geometric fluctuations Impact parameter distribution Overlap area. Assumption V(b) = C A(b). R Fix R p = 6.8 fm for 0 5% centrality. b Analytically, expansion of p i = α i R p +δr p. Maurício Hippert (IF-UFRJ) Critical vs. spurious fluctuations June 16, / 13
8 Limitations HICs inherent limitations Also, no thermodynamic limit or equilibrium. Critical Slowing Down ξ ξ (fm) t/τ A = 1.9 A = 0.9 A = 0.2 Equilibration is slow near the critical point. ξ does not reach its equilibrium value. Speed-of-light limit Berdnikov, Rajagopal (2000), MH, Fraga, Santos (2015). Maurício Hippert (IF-UFRJ) Critical vs. spurious fluctuations June 16, / 13
9 Results Signatures of pions Signal in ( N π ) 2 / N π. Excellent agreement with analytic calculations! Signal (%) ξ/ξ Pure - Analytic 25 Pure - Simulation 20 BG - Analytic (V) BG - Simulation (V+T) ξ (fm) MH, Fraga, Santos (2015). Maurício Hippert (IF-UFRJ) Critical vs. spurious fluctuations June 16, / 13
10 Final remarks Final remarks Conclusions: Theoretical expectations vs. reality! Simplified model + noise visible signatures? Background contributions can be very relevant. Perspectives: Other signatures to be tested (soon, higher-order and proton). More background/limitations. Parameter estimation: τ, V p? Dynamics beyond ξ(t). Resonance decay contributions. Maurício Hippert (IF-UFRJ) Critical vs. spurious fluctuations June 16, / 13
11 Final remarks In progress: higher-order signatures Our code is ready for higher-order moments (skewness and kurtosis). Should yield stronger signals. Results coming soon. Without spurious contributions: Temperature and volume fluctuations included: ξ ѵ ξ ѵ ¾ ½º ¾º½ ¾º ¾º º º Ë(N) Ã(N) ½º ½º¾ ½ ½º ¾º½ ¾º ¾º º º Ë(N) Ã(N) X X0 X0 ¼ ¹¾ ¹ X X0 X0 ¼º ¼º ¼º ¼º¾ ¼ ¹¼º¾ ¹ ¹¼º ¹¼º ¹ ¼ ½ ¾ (ξ/ξ0) 2 ¹¼º ¼ ½ ¾ (ξ/ξ0) 2 Maurício Hippert (IF-UFRJ) Critical vs. spurious fluctuations June 16, / 13
12 Final remarks Ë Ò Ð ±µ In progress: acceptance effects Acceptance effects can also be introduced. For now only approximate results. Signal (%) ξ/ξ GeV GeV GeV GeV ξ (fm) ξ/ξ0 ¼ ¼º¾ ¼º ¼º ½ ½º¾ ½º ½º ¾ ¾¼ η < 0.1 ½ η < 0.2 η < 0.3 η < 0.5 ½¼ η < 1.0 η < 2.0 ¼ ¹ ¼ ¼º ½ ½º ¾ ¾º º ξ ѵ Preliminary: MH, Fraga, in preparation. Maurício Hippert (IF-UFRJ) Critical vs. spurious fluctuations June 16, / 13
13 Final remarks Acknowledgements Thanks! Thanks also to FAPERJ and CNPq for financial support. Maurício Hippert (IF-UFRJ) Critical vs. spurious fluctuations June 16, / 13
A simple framework for multiplicity fluctuations near the QCD critical point
A simple framework for multiplicity fluctuations near the QCD critical point Maurício Hippert Eduardo S. Fraga INT - October 11, 2016 Maurício Hippert (IF-UFRJ) INT Program INT-16-3 October 2016 1 / 26
More informationFluctuations and the QCD Critical Point
Fluctuations and the QCD Critical Point M. Stephanov UIC M. Stephanov (UIC) Fluctuations and the QCD Critical Point Weizmann 2017 1 / 15 Outline 1 QCD phase diagram, critical point and fluctuations Critical
More informationQCD critical point, fluctuations and hydrodynamics
QCD critical point, fluctuations and hydrodynamics M. Stephanov M. Stephanov QCD critical point, fluctuations and hydro Oxford 2017 1 / 32 History Cagniard de la Tour (1822): discovered continuos transition
More informationPhase diagram of QCD: the critical point
Phase diagram of QCD: the critical point p. 1/1 Phase diagram of QCD: the critical point M. Stephanov U. of Illinois at Chicago Phase diagram of QCD: the critical point p. 2/1 Phase Diagram of QCD Basic
More informationFluctuations and QCD phase structure
Fluctuations and QCD phase structure Guo-yun Shao ( 邵国运 ) Xi an Jiaotong University Outline: Motivation Methods to describe fluctuations of conserved charges in heavy-ion collisions Numerical results and
More informationBaryon Number Fluctuations in Energy Scan Program at RHIC
Baryon Number Fluctuations in Energy Scan Program at RHIC Masakiyo Kitazawa (Osaka U.) MK, Asakawa, arxiv:1107.2755 (to appear in PRC) HIRSCHEGG2012, 18, Jan, 2012, Hirschegg Energy Scan Program @ RHIC
More informationFluctuations of Conserved Charges
Fluctuations of Conserved Charges Theory, Experiment, and Lattice Masakiyo Kitazawa (Osaka U.) KEK, 2014/Jan./20 QCD @ nonzero T Theory (Motivation) QCD @ nonzero T Lattice Heavy Ion Collisions QCD @ nonzero
More informationFluctuations of conserved charges and freeze-out conditions in heavy ion collisions
Freeze-out parameters Fluctuations of conserved charges and freeze-out conditions in heavy ion collisions Claudia Ratti University of Houston, Texas (USA) S. Borsanyi, Z. Fodor, S. Katz, S. Krieg, C. R.,
More informationDynamics of net-baryon density correlations near the QCD critical point
Dynamics of net-baryon density correlations near the QCD critical point Marcus Bluhm and Marlene Nahrgang The work of M.B. is funded by the European Union s Horizon 22 research and innovation programme
More informationInitial Condition Fluctuations for Heavy Ion Collisions
Initial Condition Fluctuations for Heavy Ion Collisions Philipe de Almeida Mota Takeshi Kodama (Ph.D. Advisor) Instituto de Física UFRJ, Rio de Janeiro, Brasil Max Planck Institut Frankfurt, Germany February
More informationThe critical point of QCD: what measurements can one make?
The critical point of QCD: what measurements can one make? Sourendu Gupta ILGTI: TIFR Strong Interactions 2010 TIFR, Mumbai February 10, 2010 Lattice measurements The critical point NLS at finite µ B Experimental
More informationThe Beam Energy Scan at RHIC
2013 ICNT Program @ FRIB, MSU July 31, 2013 The Beam Energy Scan at RHIC Jinfeng Liao Indiana University, Physics Dept. & CEEM RIKEN BNL Research Center 1 Outline Brief Intro: High Energy Heavy Ion Collisions
More informationKibble-Zurek dynamics and off-equilibrium scaling of critical cumulants in the QCD phase diagram
Kibble-Zurek dynamics and off-equilibrium scaling of critical cumulants in the QCD phase diagram Raju Venugopalan BNL/Heidelberg arxiv:1310.1600 [cond-mat.stat-mech] Heidelberg Seminar, June 8 th, 2016
More informationExperimental Approach to the QCD Phase Diagram & Search for the Critical Point
Experimental Approach to the QCD Phase Diagram & Search for the Critical Point / LBNL, Berkeley The John Cramer Symposium University of Washington, Seattle, September 10-11, 2009 Outline : QCD phase diagram
More informationThe QCD phase diagram from the lattice
The QCD phase diagram from the lattice Sourendu Gupta ILGTI: TIFR ICPAGQP Student Day Doan Paula, Goa December 5, 2010 Zero baryon density Background Exact SU(2) flavour symmetry Exact SU(3) flavour symmetry
More informationThe QCD phase diagram from the lattice
The QCD phase diagram from the lattice Sourendu Gupta ILGTI: TIFR CBM Meeting VECC Kolkata July 31, 2010 Zero baryon density Background Exact SU(2) flavour symmetry Exact SU(3) flavour symmetry Broken
More informationOff-equilibrium Non-Gaussian Cumulants: criticality, complexity, and universality
Off-equilibrium Non-Gaussian Cumulants: criticality, complexity, and universality Swagato Mukherjee SM, R. Venugopalan, Y. Yin: arxiv:1605.09341 & arxiv:1506.00645 June 2016, Wroclaw hope: observe something
More informationVan der Waals equation: event-by-event fluctuations, quantum statistics and nuclear matter
Van der Waals equation: event-by-event fluctuations, quantum statistics and nuclear matter Volodymyr Vovchenko In collaboration with Dmitry Anchishkin, Mark Gorenstein, and Roman Poberezhnyuk based on:
More informationFluctuations of conserved charges and freeze-out conditions in heavy ion collisions
Probing the Extremes of Matter with Heavy Ions - Erice, 34th Course Fluctuations of conserved charges and freeze-out conditions in heavy ion collisions Frithjof Karsch Brookhaven National Laboratory &
More informationarxiv:hep-ph/ v1 26 Oct 2005
Acta Phys. Hung. A / () HEAVY ION PHYSICS arxiv:hep-ph/0510344v1 26 Oct 2005 The role of noise and dissipation in the hadronization of the quark-gluon plasma Eduardo S. Fraga 1 1 Instituto de Física, Universidade
More informationHOT HADRONIC MATTER. Hampton University and Jefferson Lab
200 Cr oss sect ion (m b) 0 K ptotal 20 5 K pelastic 2 1 K N 1 1.6 2 3 4 2 5 6 7 8 9 20 30 3 40 THE ROLE OF BARYON RESONANCES IN Relativistic Heavy Ion Collider (RHIC) HOT HADRONIC MATTER Au+Au K d 2.5
More informationarxiv: v1 [hep-lat] 19 Feb 2012
Cent. Eur. J. Phys. -5 Author version Central European Journal of Physics Determination of Freeze-out Conditions from Lattice QCD Calculations Review Article arxiv:.473v [hep-lat] 9 Feb Frithjof Karsch,
More informationProbing QCD Phase Diagram in Heavy Ion Collisions
LQCD LHC Probing QCD Phase Diagram in Heavy Ion Collisions QCD Phase Diagram from LQCD Fluctuations of conserved charges as probe of thermalization and QCD phase boundary Linking LQCD results to HIC data
More informationIndications for a critical end point in the phase diagram for hot and dense nuclear matter
Indications for a critical end point in the phase diagram for hot and dense nuclear matter Roy A. Lacey Stony Brook University Outline Introduction Phase Diagram Search strategy Theoretical guidance Femtoscopic
More informationMeasures of charge fluctuations in nuclear collisions
Measures of charge fluctuations in nuclear collisions Jacek Zaranek* Institut für Kernphysik, Universität Frankfurt, D-60486 Frankfurt, Germany Received 27 November 2001; published 29 August 2002 The properties
More informationThe critical end point of QCD: lattice and experiment
The critical end point of QCD: lattice and experiment Sourendu Gupta ILGTI: TIFR Patnitop 2009 January 2, 2010 SG (ILGTI: TIFR) CEP: lattice and experiment Patnitop 09 1 / 28 Outline 1 On lattice 2 In
More informationThe strange degrees of freedom in QCD at high temperature. Christian Schmidt
The strange degrees of freedom in QCD at high temperature Christian Schmidt Christian Schmidt LAT 213 1 Abstract We use up to fourth order cumulants of net strangeness fluctuations and their correlations
More informationExploring the QCD phase diagram with conserved charge fluctuations
New Frontiers in QCD 2013 Exploring the QCD phase diagram with conserved charge fluctuations Frithjof Karsch Brookhaven National Laboratory & Bielefeld University OUTLINE conserved charge fluctuations
More informationFluid dynamics with a critical point
Fluid dynamics with a critical point Marlene Nahrgang PhD student of Institut für Theoretische Physik, Goethe- Universität Frankfurt am Main. Scientific interests include QCD, quark-gluon plasma, and particle
More informationTransport of Fluctuations
Transport of Fluctuations Masakiyo Kitazawa (Osaka U.) INT Workshop 16-3 Exploring the QCD Phase Diagram through Energy Scan INT, Seattle, 6/Oct./2016 J-PARC Heavy-Ion Program (J-PARC-HI) J-PARC-HI Program
More informationInsights (?) from lattice QCD at finite baryo-chemical potential (title given to me)
Exploring the QCD Phase Diagram through Energy Scans Insights (?) from lattice QCD at finite baryo-chemical potential (title given to me) Frithjof Karsch Bielefeld University & Brookhaven National Laboratory
More informationThe critical point in QCD
The critical point in QCD Thomas Scha fer North Carolina State University The phase diagram of QCD L = q f (id/ m f )q f 1 4g 2 Ga µνg a µν 2000: Dawn of the collider era at RHIC Au + Au @200 AGeV What
More informationEquilibration and decoupling of a relativistic gas in a Friedmann-Robertson-Walker spacetime
Equilibration and decoupling of a relativistic gas in a Friedmann-Robertson-Walker spacetime Juan M. Torres-Rincon (Frankfurt Institute for Advanced Studies) in collaboration with J. Tindall, J.-B. Rosé,
More informationStudy of Transitions and Decays of Bottomonia at Belle
1 Study of Transitions and Decays of Bottomonia at Belle Saurabh Sandilya University of Cincinnati (On behalf of the Belle Collaboration) Outline Introduction (Bottomonia, KEKB & Belle detector) Transitions
More informationThe QCD phase diagram at real and imaginary chemical potential
Strongnet Meeting Trento, October 211 The QCD phase diagram at real and imaginary chemical potential Owe Philipsen Is there a critical end point in the QCD phase diagram? Is it connected to a chiral phase
More informationSearching for the QCD critical point in nuclear collisions
Critical Point and Onset of Deconfinement, Florence, 3-6 July 2006 Searching for the QCD critical point in nuclear collisions F.K. Diakonos Outline. Observational critical QCD - basic predictions 2. CMC
More informationPast, Present, and Future of the QGP Physics
Past, Present, and Future of the QGP Physics Masayuki Asakawa Department of Physics, Osaka University November 8, 2018 oward Microscopic Understanding In Condensed Matter Physics 1st Macroscopic Properties
More informationarxiv: v1 [hep-ph] 2 Apr 2019 Juan M. Torres-Rincon and Edward Shuryak
Nuclear correlations and modifications of the nucleon-nucleon potential due to the QCD critical mode arxiv:194.161v1 [hep-ph] 2 Apr 219 and Edward Shuryak Department of Physics and Astronomy, Stony Brook
More informationQCD Phase Diagram. M. Stephanov. U. of Illinois at Chicago. QCD Phase Diagram p. 1/13
QCD Phase Diagram p. 1/13 QCD Phase Diagram M. Stephanov U. of Illinois at Chicago QCD Phase Diagram p. 2/13 QCD phase diagram (contemporary view) T, GeV QGP 0.1 crossover critical point hadron gas vacuum
More informationHeavy Mesonic Spectral Functions at Finite Temperature and Finite Momentum
Heavy Mesonic Spectral Functions at Finite Temperature and Finite Momentum Masayuki Asakawa Department of Physics, Osaka University September 2011 @ EMMI Workshop QCD Phase Diagram T LHC RHIC QGP (quark-gluon
More informationBeam Energy Scan Program in STAR Experimental Approach to the QCD Phase Diagram
Beam Energy Scan Program in STAR Experimental Approach to the QCD Phase Diagram Grazyna Odyniec / LBNL, Berkeley for STAR Collaboration Central Au+Au @ 7.7 GeV event in STAR TPC CPOD 2010, Dubna, Russia,
More informationOverview* of experimental results in heavy ion collisions
Overview* of experimental results in heavy ion collisions Dipartimento di Fisica Sperimentale dell Universita di Torino and INFN Torino * The selection criteria of the results presented here are (to some
More informationConstraining the QCD equation of state in hadron colliders
Constraining the QCD equation of state in hadron colliders Akihiko Monnai (KEK, Japan) with Jean-Yves Ollitrault (IPhT Saclay, France) AM and J.-Y. Ollitrault, Phys. Rev. C 96, 044902 (2017) New Frontiers
More informationQCD matter with isospin-asymmetry. Gergely Endrődi. Goethe University of Frankfurt in collaboration with Bastian Brandt, Sebastian Schmalzbauer
QCD matter with isospin-asymmetry Gergely Endrődi Goethe University of Frankfurt in collaboration with Bastian Brandt, Sebastian Schmalzbauer SIGN 2017 22. March 2017 Outline introduction: QCD with isospin
More informationThe QCD phase diagram at low baryon density from lattice simulations
ICHEP 2010 Paris, July 2010 The QCD phase diagram at low baryon density from lattice simulations Owe Philipsen Introduction Lattice techniques for finite temperature and density The phase diagram: the
More informationMicroscopic collectivity: The ridge and strangeness enhancement from string string interactions in Pythia8
Microscopic collectivity: The ridge and strangeness enhancement from string string interactions in Pythia8 Christian Bierlich bierlich@thep.lu.se Lund University / University of Copenhagen May 15, 2018
More informationLepton-Rich Cold Quark Matter
Lepton-Rich Cold Quark Matter José C. Jiménez Eduardo S. Fraga Instituto de Física Universidade Federal do Rio de Janeiro 56th International School of Subnuclear Physics, Erice 2018 José C. Jiménez, Eduardo
More informationThermal dileptons as fireball probes at SIS energies
Thermal dileptons as fireball probes at SIS energies Critical Point and Onset of Deconfinement 2016, Wrocław. Florian Seck TU Darmstadt in collaboration with T. Galatyuk, P. M. Hohler, R. Rapp & J. Stroth
More informationOutline: Introduction and Motivation
Heavy ion collisions at lower energies: challenges and opportunities Beam Energy Scan (BES I and II) from RHIC Lijuan Ruan (Brookhaven National Laboratory) Outline: Introduction and Motivation Results
More informationMultiplicity fluctuations of (net) charges and (net) protons from iebe- VISHNU hybrid model
Multiplicity fluctuations of (net) charges and (net) protons from iebe- VISHNU hybrid model Reporter: Jixing Li ( 李继行 ) Supervisor: Prof. Huichao Song Peking University Reference: Jixing Li, Hao-jie Xu,Huichao
More informationarxiv: v1 [nucl-ex] 25 Jan 2012
Cent. Eur. J. Phys. 1-5 Author version Central European Journal of Physics New results from fluctuation analysis in NA49 at the CERN SPS Research Article arxiv:1201.5237v1 [nucl-ex] 25 Jan 2012 Maja Maćkowiak-Paw
More informationThermodynamic Signatures of Additional Strange and Charm Baryons
Thermodynamic Signatures of Additional Strange and Charm Baryons Swagato Mukherjee April 2015, GHP, Baltimore, MD Heavy-ion collisions: a sketch Time initial state QGP, hydro. expansion Tc, μ c freeze-out
More informationBulk matter formed in Pb Pb collisions at the LHC
Bulk matter formed in Pb Pb collisions at the LHC Introductory remarks is quark matter at LHC in equilibrium? Energy dependence of hadron production and the quark hadron phase boundary The fireball expands
More informationHadronization by coalescence plus fragmentation from RHIC to LHC
Vincenzo Minissale University of Catania INFN LNS Hadronization by coalescence lus fragmentation from RHIC to LHC Nucleus Nucleus 015, June 015 Vincenzo Greco Francesco Scardina arxiv:150.0613 Outline
More informationCOLLISIONS IN ADS AND THE THERMALISATION OF HEAVY IONS
COLLISIONS IN ADS AND THE THERMALISATION OF HEAVY IONS Towards more realistic models of the QGP thermalisation Work with Michał Heller, David Mateos, Jorge Casalderrey, Paul Romatschke and Scott Pratt
More informationInitial baryon number fluctuations and its hydrodynamic propagation on a Bjorken background
Initial baryon number fluctuations and its hydrodynamic propagation on a Bjorken background Mauricio Martinez Guerrero In collaboration with Stefan Floerchinger arxiv:1507.05569 Correlations and Fluctuations
More informationMagnetized QCD phase diagram
Magnetized QCD phase diagram Márcio Ferreira, Pedro Costa, and Constança Providência CFisUC, University of Coimbra, Portugal New Frontiers in QCD 2018 May 30 - June 29 Yukawa Institute for Theoretical
More informationOn the role of fluctuations in (2+1)-flavor QCD
On the role of fluctuations in (2+1)-flavor QCD Bernd-Jochen Schaefer Germany Germany November 29 th, 217 Conjectured QC3D phase diagram Temperature early universe LHC crossover vacuum RHIC SPS =
More informationHagedorn States in Relativistic Heavy Ion Collisions
Hagedorn States in Relativistic Heavy Ion Collisions Jacquelyn Noronha-Hostler Frankfurt Institute for Advanced Studies, Frankfurt am Main Excited Hadrons : February 25 th, 211 : Jefferson Lab Newport
More informationarxiv:hep-ph/ v3 2 Jan 2001
Thermalization temperature in Pb+Pb collisions at SpS energy from hadron yields and midrapidity p t distributions of hadrons and direct photons D. Yu. Peressounko and Yu. E. Pokrovsky Russian Research
More informationarxiv:hep-ph/ v3 14 Nov 2005
arxiv:hep-ph/596v3 4 Nov 25 3D Relativistic Hydrodynamic Computations Using Lattice-QCD-Inspired Equations of State Yogiro Hama a, Rone P.G. Andrade a, Frédérique Grassi a, Otávio Socolowski Jr. b, Takeshi
More informationFreeze-out parameters: lattice meets experiment
Freeze-out parameters: lattice meets experiment Claudia Ratti Università degli Studi di Torino and INFN, Sezione di Torino In collaboration with R. Bellwied, S. Borsanyi, Z. Fodor, S. Katz, S. Krieg, K.
More informationBased on work in progress in collaboration with: F. Scardina, S. Plumari and V. Greco
Marco Ruggieri Dipartimento di Fisica e Astronomia, Università degli Studi di Catania, Catania (Italy) Based on work in progress in collaboration with: F. Scardina, S. Plumari and V. Greco Bari, 2012 December
More informationPoS(WPCF2011)012. New results on event-by-event fluctuations in A+A collisions at the CERN SPS. Grzegorz Stefanek for the NA49 Collaboration
New results on eventbyevent fluctuations in AA collisions at the CERN SPS for the NA9 Collaboration Jan Kochanowski University, Kielce, Poland Email: grzegorz.stefanek@pu.kielce.pl The study of central
More informationarxiv: v1 [hep-ph] 18 Feb 2016
Nuclear Physics A Nuclear Physics A 00 (2016) 1 5 www.elsevier.com/locate/procedia arxiv:1602.05811v1 [hep-ph] 18 Feb 2016 Abstract Confronting fluctuations of conserved charges in central nuclear collisions
More informationThe Quark-Gluon Plasma and the ALICE Experiment
The Quark-Gluon Plasma and the ALICE Experiment David Evans The University of Birmingham IoP Nuclear Physics Conference 7 th April 2009 David Evans IoP Nuclear Physics Conference 2009 1 Outline of Talk
More informationQGP Thermodynamics and Phase Transitions. Mahnaz Q. Haseeb Department of Physics CIIT, Islamabad
QGP Thermodynamics and Phase Transitions Mahnaz Q. Haseeb Department of Physics CIIT, Islamabad Outline Thermodynamics in QGP What are the phase transitions? Order of the phase transition Where to study
More informationHeavy Ion Physics Lecture 3: Particle Production
Heavy Ion Physics Lecture 3: Particle Production HUGS 2015 Bolek Wyslouch echniques to study the plasma Radiation of hadrons Azimuthal asymmetry and radial expansion Energy loss by quarks, gluons and other
More informationHydrodynamical description of ultrarelativistic heavy-ion collisions
Frankfurt Institute for Advanced Studies June 27, 2011 with G. Denicol, E. Molnar, P. Huovinen, D. H. Rischke 1 Fluid dynamics (Navier-Stokes equations) Conservation laws momentum conservation Thermal
More informationLambda-Lambda correlation from an integrated dynamical model
ExHIC, March 28, 2016 Lambda-Lambda correlation from an integrated dynamical model Tetsufumi Hirano (Sophia Univ.) Collaborators: Asumi Taniguchi Hiromi Hinohara Koichi Murase References for the model:
More informationNonequilibrium dynamics and transport near the chiral phase transition of a quark-meson model
FAIRNESS 2013, 15-21 September 1 Nonequilibrium dynamics and transport near the chiral phase transition of a quark-meson model A Meistrenko 1, C Wesp 1, H van Hees 1,2 and C Greiner 1 1 Institut für Theoretische
More informationMFT: Motivations and Expectations
Physics Week NFN NF Frascati 18 pril 2012 ntonio Uras for the MFT Working Group yon group @ PN Outline Physics Motivations ow mass and low pt dimuon reach: a unique feature at the H ow pt reach for open
More informationEquation of state. Pasi Huovinen Uniwersytet Wroc lawski. Collective Flows and Hydrodynamics in High Energy Nuclear Collisions
Equation of state Pasi Huovinen Uniwersytet Wroc lawski Collective Flows and Hydrodynamics in High Energy Nuclear Collisions Dec 14, 2016, University of Science and Technology of China, Hefei, China The
More informationarxiv: v1 [hep-ph] 11 Jun 2008
Proc. 4th Winter Workshop on Nuclear Dynamics (008) 000 000 4th Winter Workshop on Nuclear Dynamics South Padre, Texas, USA April 1, 008 arxiv:0806.180v1 [hep-ph] 11 Jun 008 A fully integrated Boltzmann+hydrodynamics
More informationQCD in Heavy-ion collisions
QCD in Heavy-ion collisions RPP 2012, Montpellier transition t p z q IPhT, Saclay 1 Outline 1 2 3 4 5 6 7 transition 2 1 transition 2 3 4 5 6 transition 7 2 Asymptotic freedom Running coupling : α s =
More informationAzimuthal anisotropy of the identified charged hadrons in Au+Au collisions at S NN. = GeV at RHIC
Journal of Physics: Conference Series PAPER OPEN ACCESS Azimuthal anisotropy of the identified charged hadrons in Au+Au collisions at S NN = 39-200 GeV at RHIC To cite this article: S S Vdovkina 2017 J.
More informationGlobal and Collective Dynamics at PHENIX
Global and Collective Dynamics at PHENIX Takafumi Niida for the PHENIX Collaboration University of Tsukuba Heavy Ion collisions in the LHC era in Quy Nhon outline n Introduction of v n n Higher harmonic
More informationLattice Methods for Hadron Spectroscopy: new problems and challenges
Lattice Methods for Hadron Spectroscopy: new problems and challenges Sinéad Ryan School of Mathematics, Trinity College Dublin, Ireland INT, Seattle, 10 th August, 2012 Sinéad Ryan (TCD) 1 / 28 Plan A
More informationUnderstanding hadronization on the basis of fluctuations of conserved charges
Understanding hadronization on the basis of fluctuations of conserved charges R. Bellwied (University of Houston) in collaboration with S. Jena, D. McDonald (University of Houston) C. Ratti, P. Alba, V.
More informationMassimo D Elia Dipartimento di Fisica and INFN Genova, Via Dodecaneso 33, I Genova, ITALY
A test of first order scaling of the N f =2 QCD phase transition Guido Cossu SNS and INFN Pisa, Piazza dei Cavalieri 7, I-56127 Pisa, ITALY g.cossu@sns.it Massimo D Elia Dipartimento di Fisica and INFN
More informationJanuary 31, PHY357 Lecture 8. Quark composition of hadrons. Hadron magnetic moments. Hadron masses
January 3, 08 PHY357 Lecture 8 Quark composition of hadrons Hadron magnetic moments Hadron masses January 3, 08 Quark rules for building Hadrons! Three types of stable quark configurations established!
More informationarxiv: v1 [nucl-th] 23 Jan 2019
arxiv:1901.08157v1 [nucl-th] 23 Jan 2019 Cyclotron Institute and Department of Physics and Astronomy, Texas A&M University, College Station TX 77843, USA E-mail: rjfries@comp.tamu.edu Michael Kordell Cyclotron
More informationEstimates of thermal nucleation of quark matter during bounce
Estimates of thermal nucleation of quark matter during bounce Bruno Mintz 1 Eduardo Fraga 1, Giuseppe Pagliara 2 and Jürgen Schaffner Bielich 2 (1) Universidade Federal do Rio de Janeiro (2) Ruprecht Karls
More informationThermal model fits: an overview
Thermal model fits: an overview Volodymyr Vovchenko Goethe University Frankfurt & Frankfurt Institute for Advanced Studies Light up 2018 An ALICE and theory workshop, CERN June 14, 2018 The conventional
More informationThe Quark-Gluon plasma in the LHC era
The Quark-Gluon plasma in the LHC era Journées de prospective IN2P3-IRFU, Giens, Avril 2012 t z IPhT, Saclay 1 Quarks and gluons Strong interactions : Quantum Chromo-Dynamics Matter : quarks ; Interaction
More informationKinetics of the chiral phase transition
Kinetics of the chiral phase transition Hendrik van Hees, Christian Wesp, Alex Meistrenko and Carsten Greiner Institut für Theoretische Physik, Universität Frankfurt, Max-von-Laue-Straße 1, 60438 Frankfurt
More informationJ/Ψ-suppression in the hadron resonance gas
J/Ψ-suppression in the hadron resonance gas Dariusz Prorok Institute of Theoretical Physics University of Wroc law Wroc law, 17 February 2014 HECOLS workshop and XXXII Max-Born Symposium Dariusz Prorok
More informationHeavy Ions at the LHC: First Results
Heavy Ions at the LHC: First Results Thomas Schaefer North Carolina State University Heavy ion collision: Geometry R Au /γ y R Au x b z rapidity : y = 1 2 log ( E + pz E p z ) transverse momentum : p 2
More informationHadronic Effects on T cc in Relativistic Heavy Ion Collisions
Hadronic Effects on T cc in Relativistic Heavy Ion Collisions Juhee Hong Yonsei University New Frontiers in QCD 2018, YITP, Kyoto University arxiv: 1804.05336, JH, Sungtae Cho, Taesoo Song, and Su Houng
More informationStrong Interaction Effects. of Strong Magnetic Fields. CPODD Workshop 2012 RIKEN BNL, June Berndt Mueller. Wednesday, June 27, 12
Strong Interaction Effects of Strong Magnetic Fields Berndt Mueller CPODD Workshop 2012 RIKEN BNL, 25-27 June 2012 Overview Pseudoscalar QED-QCD couplings CME phenomenology Results M. Asakawa, A. Majumder
More informationMATTER. Sourendu Gupta (TIFR, Mumbai) for the Indian Lattice Gauge Theory Initiative at IIT-Roorkee. March 13, 2005
MATTER Sourendu Gupta (TIFR, Mumbai) for the Indian Lattice Gauge Theory Initiative at IIT-Roorkee March 13, 2005 1 Can the mass of this system be computed from the standard model of particle physics?
More informationMultiplicity Fluctuations in Statistical Models
Multiplicity Fluctuations in Statistical Models Michael Hauer Outline Introduction Particle Anti Particle Gas Hadron Gas Comparison with Data Summary 1 Statistical Ensembles Grand Canonical Canonical Microcanonical
More informationMonte Carlo Non-Linear Flow modes studies with AMPT
Monte Carlo Non-Linear Flow modes studies with AMP Daniel Noel Supervised by: Naghmeh Mohammadi 2 July - 31 August 218 1 Introduction Heavy-ion collisions at the Large Hadron Collider (LHC) generate such
More informationNA61/SHINE results on Le vy analysis of HBT correlation functions
Introduction NA61/SHINE results on Le vy analysis of HBT correlation functions 56th International School of Subnuclear Physics, Erice, Sicily, 2018 Barnaba s Po rfy for the NA61/SHINE Collaboration Wigner
More informationarxiv: v2 [nucl-ex] 22 Jun 2015
arxiv:153.558v [nucl-ex] Jun 15 Energy Dependence of Moments of Net-Proton and Net-Charge Multiplicity Distributions at SAR (for the SAR Collaboration) Institute of Particle Physics and Key Laboratory
More informationWhen Perturbation Theory Fails...
When Perturbation Theory Fails... Brian Tiburzi (University of Maryland) When Perturbation Theory Fails... SU(3) chiral perturbation theory? Charm quark in HQET, NRQCD? Extrapolations of lattice QCD data?
More informationPions in the quark matter phase diagram
Pions in the quark matter phase diagram Daniel Zabłocki Instytut Fizyki Teoretycznej, Uniwersytet Wrocławski, Poland Institut für Physik, Universität Rostock, Germany Bogoliubov Laboratory of Theoretical
More informationQCD thermodynamics OUTLINE:
QCD thermodynamics Frithjof Karsch, BNL OUTLINE: Equation of state and transition temperature QCD phase diagram close to the chiral limit Charge fluctuations and the RHIC search for the critical point
More informationPhilipe de Almeida Mota
Philipe de Almeida Mota Personal Data birth date: december 9, 1983 nationality: Brazilian gender: male degree: M.Sc. in Physics (currently Ph.D. student) residential address: Av. Epitácio Pessoa 3100,
More informationHeavy-Quark Transport in the QGP
Heavy-Quark Transport in the QGP Hendrik van Hees Goethe-Universität Frankfurt November 9, 211 Hendrik van Hees (GU Frankfurt) Heavy-Quark Transport November 9, 211 1 / 19 Motivation Fast equilibration
More information