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The Phase Diagram of QCD

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Presentation on theme: "The Phase Diagram of QCD"— Presentation transcript:

1 The Phase Diagram of QCD
Bedanga Mohanty NISER Outline: Phase Diagram of QCD Experimental Realization Summary INSA Meeting, NISER – December 28-30, 2016 01/21

2 Phase diagram Phase diagram of Water Electromagnetic interaction
Precisely known Phase diagram of strong interactions Largely still a conjecture NSAC Long range plan Many Unique 02/21

3 Heavy-Ion Collisions and QCD Phase diagram
Colliding two nuclei we expect to create the QCD transitions -- De-confinement -- Chiral Symmetry Restoration in laboratory p+p like collisions A+A collisions Universe: QCD Ph. Transition: T~200MeV EW Ph. Transition: T ~ 150 GeV GUT Ph. Transition: T ~ 1016 GeV J. D. Bjorken Physical Review D 27 (1983) 140 03/21

4 Experimental access to the Phase diagram of QCD
Physical systems undergo phase transitions when external parameters such as the temperature (T) or a chemical potential (μ) are tuned. Conserved Quantities: Baryon Number ~  Electric Charge ~ Q ~ small Strangeness ~ S ~ small Varying beam energy varies Temperature and Baryon Chemical Potential P. Braun-Munzinger, J. Stachel Nature 448: ,2007 04/21

5 Establishing the Phase Diagram of QCD
Produce a QCD matter where Thermodynamics is applicable Chapter – 11 Thermal Properties of Matter NCERT - Book Demonstrate existence of Quark-Gluon Phase Establish cross-over at mB = 0 MeV Establish – QCD Critical Point and/or 1st Order Phase Transition at high mB If successful QCD PD could also find place a in text books 05/21

6 Particle Production – Thermalized Source
STAR PRL : 2004 STAR NPA : 2005 Tch = 163 ± 4 MeV B = 24 ± 4 MeV In central collisions, the system is thermalized at RHIC Statistical Model with Grand Canonical Ensemble. Incorporates the various conservation laws. Assumes thermal and chemical equilibrium. 06/21

7 QCD Phase Structure & Transition Temperature at mB = 0 MeV
PRD85 (2012) NPA 830 (2009) 805c Nature443: ,2006 Transition temperature and Cross Over established at zero baryon chemical potential 07/21

8 Establishing Quark-Gluon Plasma
If there is system of free quarks and gluons – Photons can be produced through: Compton Annihilation Bremsstrahlung In a hydrodynamic picture: Slope of momentum distribution of these photons Tc ~ 150 MeV ~ 1012 Kelvin Temperature for QCD transition from Lattice QCD 08/21

9 Establishing Quark-Gluon Plasma
TAA scaled pp + Exponential Ti = MeV > Tc Sinha, Srivastava, Alam, Sarkar, Gale, Turbide, Rasanen, Liu, d’Enteria Gold-Gold Direct Photons NLO pQCD (W. Vogelsang) Fit to pp Deconfined state of quarks And Gluons Proton-Proton Direct Photons 09/21

10 Perspective of Temperature Reached in Heavy-ion Collisions
~1012 K Nucleus-Nucleus collisions ~ 150 MeV ~109 K Neutron Star Thermonuclear Explosion (Terrestrial Nuclear explosions) ~106 K Solar Interior ~6000 K Solar Surface Room Temperature ~ 1/40 eV ~300 K Cosmic Microwave Background ~3 K ~10-6 K Rhodium metal spin cooling (2000) ~10-10 K (Low-T World Record!) Trapped Ions 10/21

11 coordinate-space-anisotropy  momentum-space-anisotropy
Collectivity coordinate-space-anisotropy  momentum-space-anisotropy y py x px y x 18/35

12 Probes of the Medium Strong Collectivity
STAR PRL : 2016 y x Low pT : Heavier hadrons have lower v2 ( ~ hydrodynamic pattern) High pT : Collectivity grouped along baryon-meson lines ( ~ Hadronization by partonic recombination) All pT : Collectivity similar for hadrons with strange and light quark (~ developed at partonic stage) 11/21

13 Partonic Collectivity
quarks mesons baryons both axes scaled by number of constituent quarks nq = 2 for mesons nq = 3 for baryons plotted vs. trans. kinetic energy particle mass dependence recombination of quarks quarks have v2 before hadronization 12/21

14 Properties of QGP Pitch has viscosity approximately
230 billion times that of water. Longest running experiment (1927-present) 8 drops so far, none ever seen fall! Viscosity: Resistance to Flow 13/21

15 Viscosity Perfect Fluid h/s ~ 0 h/s = 1/4p h/s = 2 x 1/4p
Victor Roy, et al. Perfect Fluid 14/21

16 Jets Probes of the Medium Opacity Matter we want to study Calibrated
Light Meter Calibrated LASER Jets Calibrated Heat Source

17 Quenching of Jets p+p A+A Nuclear Modification Factor:
leading particle suppressed p+p A+A back-to-back jets disappear Nuclear Modification Factor: 20/33

18 Experimental Evidence: Quenching of Jets
High pT hadron production suppressed Production of photons which do not participate in strong interactions is not suppressed No suppression in d+Au collisions initial > C (Lattice) Interpretation : Energy loss of partons in a dense medium 21/33

19 Opacity Jets Quenched The shear viscosity to entropy density ratio is found to lie between (1-2)/4p and that reflecting the stopping power was observed to be between 2-10 GeV2/fm.

20 Experimental Result: 1st Order PT
Observations consistent with 1st order Phase transition expectations STAR: Physical Review Letters 2014 15/21

21 Experiment and Theory Direct Link
Shape of distribution  Correlations < (N)2> ~ 2 < (N)3> ~ 4.5 < (N)4> - 3 < (N)2>2 ~ 7 Moments relates to Correlation length (): Study phase transition and Critical Point Moments relates to Susceptibility (c) : Study Bulk properties of QCD matter Kurtosis x Variance ~ 4)/ [c T2] Skewness x Sigma ~ [3) T]/ [c T2] STAR: Physical Review Letters 2010& 2014 M. Stephanov: Physical Review Letters 2009;2011 S. Gupta and R. Gavai : Physics Letters B 2011 M. Cheng .. F. Karsch ..: Physical Review D 2009 16/21

22 Data and QCD (Non-Zero T) 1st Comparison
1st comparison of high energy nuclear collision data to 1st principle QCD calculations Confirms formation of QGP Quark-Hadron transition is a cross over “Scale for the Phase Diagram of Quantum Chromodynamics” Science, 332, 1525(2011) 17/21

23 Theory : Critical Point
TIFR, Mumbai 18/21

24 Experimental Result: Critical Point
M.A. Stephanov, Phys. Rev. Lett. 107, (2011). Exciting Period !! BES-II ( ) CBM ( ) 4)/ c T, mB STAR: Physical Review Letters 2014 And STAR Preliminary 19/21

25 Emergent Properties of QCD Matter
Summary QCD phase transition and primordial matter created in Laboratory. System of de-confined quarks and gluons formed. The de-confined quarks and gluons (fundamental constituent of any visible matter ) exhibits the property of perfect fluidity with high degree of opacity Phase Diagram of Strong Interactions being laid out. Transition temperature and order of phase transition established at zero baryon chemical potential. Exciting experimental results on critical point and phase boundary. Susceptibility has a non-monotonic variation with beam energy. Emergent Properties of QCD Matter 20/21

26 Towards a complete test of QCD as a theory
QCD in 21st Century Standard Model & Origin of Mass Test of QCD Non-perturbative T>0 & Phase structure of QCD Phase diagram Science 332, 1525 (2011) Test of QCD, Short distance scales, perturbative regime Test of QCD, Long distance scales, Non-perturbative regime Science 322, 1224 (2008) T=0 Towards a complete test of QCD as a theory 21/21

27 Anti-Nuclei Ionization energy loss: - < dE/dx > ~ A / 2
= A (1 + m2/ p2) 5 kind of charged Particles and two Neutral particles Nature, 473, 353(2011). 4He 2011 Science, 328, 58(2010) M2 = E2 - p2 Louis Pasteur: “In the field of observation, chance only favours those minds which have been prepared” 27

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