Download - QCD results on conserved charge fluctuations and Beam ...theory.gsi.de/~friman/EMMI-Workshop/swagato.pdf · S pop fit — KpOp fit 0.2 0.4 0.6 0.4 0.2 HR -0.2 -0.4 -0.6 140 31 31

Transcript
Page 1: QCD results on conserved charge fluctuations and Beam ...theory.gsi.de/~friman/EMMI-Workshop/swagato.pdf · S pop fit — KpOp fit 0.2 0.4 0.6 0.4 0.2 HR -0.2 -0.4 -0.6 140 31 31

November 2015, GSI, Germany

QCD results on conserved charge fluctuations

and Beam Energy Scan

Swagato Mukherjee

Page 2: QCD results on conserved charge fluctuations and Beam ...theory.gsi.de/~friman/EMMI-Workshop/swagato.pdf · S pop fit — KpOp fit 0.2 0.4 0.6 0.4 0.2 HR -0.2 -0.4 -0.6 140 31 31

2

Baseline ?

Page 3: QCD results on conserved charge fluctuations and Beam ...theory.gsi.de/~friman/EMMI-Workshop/swagato.pdf · S pop fit — KpOp fit 0.2 0.4 0.6 0.4 0.2 HR -0.2 -0.4 -0.6 140 31 31

3

Equilibrium QCD baseline ?

Tf (μBf)

(L)QCD cumulants of conservedcharge fluctuations along:

not a fundamental QCD parameter: expt. input fora given colliding system, phase space cuts, √s …

underlying assumption: expt. observables can be mapped into thermodynamic parameters Tf ,μB

f

use a 'god-given' Tf (μBf )

MQ/σQ2[Mp/σp

2]

OR for consistency: estimate by matching expt. lower cumulants with equilibrium QCD despite all known/unknown caveats

Tf (μBf)

MQ/σQ2 [MB/σB

2 ]

equilibrium QCD baseline for higher cumulants along this Tf (μBf)

Page 4: QCD results on conserved charge fluctuations and Beam ...theory.gsi.de/~friman/EMMI-Workshop/swagato.pdf · S pop fit — KpOp fit 0.2 0.4 0.6 0.4 0.2 HR -0.2 -0.4 -0.6 140 31 31

4

monotonic functions of

√s

μB/T

Page 5: QCD results on conserved charge fluctuations and Beam ...theory.gsi.de/~friman/EMMI-Workshop/swagato.pdf · S pop fit — KpOp fit 0.2 0.4 0.6 0.4 0.2 HR -0.2 -0.4 -0.6 140 31 31

5

μQ=μS=0for simplicity of discussion:

in practice: Ms=0, MQ/MB=0.4 μQ(T ,μB), μS(T ,μB)

MX /σX along the freeze-out line:

χ(T f)= χ(T f , 0)−κ2f (dχ

dT )T f ,0

(μB

T )2

Page 6: QCD results on conserved charge fluctuations and Beam ...theory.gsi.de/~friman/EMMI-Workshop/swagato.pdf · S pop fit — KpOp fit 0.2 0.4 0.6 0.4 0.2 HR -0.2 -0.4 -0.6 140 31 31

6

BNL-Bi-CCNU: arXiv:1509:05786

Page 7: QCD results on conserved charge fluctuations and Beam ...theory.gsi.de/~friman/EMMI-Workshop/swagato.pdf · S pop fit — KpOp fit 0.2 0.4 0.6 0.4 0.2 HR -0.2 -0.4 -0.6 140 31 31

7

BNL-Bi-CCNU: arXiv:1509:05786

155 MeV147 MeV145 MeV

Tf , 0

Page 8: QCD results on conserved charge fluctuations and Beam ...theory.gsi.de/~friman/EMMI-Workshop/swagato.pdf · S pop fit — KpOp fit 0.2 0.4 0.6 0.4 0.2 HR -0.2 -0.4 -0.6 140 31 31

8

BNL-Bi-CCNU: arXiv:1509:05786

T f , 0

κ2f<0.011

slope:

Page 9: QCD results on conserved charge fluctuations and Beam ...theory.gsi.de/~friman/EMMI-Workshop/swagato.pdf · S pop fit — KpOp fit 0.2 0.4 0.6 0.4 0.2 HR -0.2 -0.4 -0.6 140 31 31

9

μQ=μS=κ2f =0

choosing for simplicity:

Page 10: QCD results on conserved charge fluctuations and Beam ...theory.gsi.de/~friman/EMMI-Workshop/swagato.pdf · S pop fit — KpOp fit 0.2 0.4 0.6 0.4 0.2 HR -0.2 -0.4 -0.6 140 31 31

10

μQ=μS=κ2f =0

choosing for simplicity:

Page 11: QCD results on conserved charge fluctuations and Beam ...theory.gsi.de/~friman/EMMI-Workshop/swagato.pdf · S pop fit — KpOp fit 0.2 0.4 0.6 0.4 0.2 HR -0.2 -0.4 -0.6 140 31 31

11

μQ=μS=κ2f =0

choosing for simplicity:

Page 12: QCD results on conserved charge fluctuations and Beam ...theory.gsi.de/~friman/EMMI-Workshop/swagato.pdf · S pop fit — KpOp fit 0.2 0.4 0.6 0.4 0.2 HR -0.2 -0.4 -0.6 140 31 31

12

μQ=μS=κ2f =0

choosing for simplicity:

Page 13: QCD results on conserved charge fluctuations and Beam ...theory.gsi.de/~friman/EMMI-Workshop/swagato.pdf · S pop fit — KpOp fit 0.2 0.4 0.6 0.4 0.2 HR -0.2 -0.4 -0.6 140 31 31

13