Systematics of directed and elliptic flow of light particles in heavy ion collisions in the 1A GeV...

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Transcript of Systematics of directed and elliptic flow of light particles in heavy ion collisions in the 1A GeV...

Systematics of directed and elliptic flow of light particles in heavy ion collisions in the 1A GeV

regime

王永佳兰州大学核科学与技术学院

合作者:郭琛琛 ( 北京师范大学 )导师:李庆峰 ( 湖州师范学院理学院 ) 张鸿飞 ( 兰州大学核科学与技术学院 ) [Ref.] W. Reisdorf et al. FOPI Collaboration NPA(2012)876.1-60

Outline

Ultrarelativistic Quantum-Molecular-Dynamics (UrQMD) model Initializationpotential updates--Skyrme potentialscross section---medium effectcluster construction

Results yieldcollective flow of proton, deuteron, mass 3 (triton and 3

He) and 4He comparison of directed flow of 3H with 3He

Ultrarelativistic Quantum-Molecular-Dynamics (UrQMD) model

• study collisions of p+p, p+A and A+A systems at incident energies covered by INDRA/GSI experiments up to highest energies presently available at LHC/CERN.

• recently updates:various Skyrme interactions have been introduced,

like ImQMD, LQMDmomentum-modified density-dependent nucleon n

ucleon elastic cross section (NNECS)isospin denpendence in cluster recognition, iso-MS

T (minimum spanning tree )

UrQMD Model: Initialization

0 2 4 6 8 10 120.00

0.04

0.08

0.12

0.16

0.20

2 4 6 8 10 12

n p all

197AuWoods-Saxon

r (fm)

n p all

197AuHard-sphere

• Woods-Saxon (WS)• Hard-sphere (HS)

0 30 60 90 120 150-0.010

-0.008

-0.006

-0.004

-0.002

0.000

bind

ing

ener

gy (G

eV)

t (fm/c)

197Au5 random eventsx

(fm

)

Initialization : Hard-sphere

Potential updates

like ImQMD,LQMD

mdCoulloc UUUTH

potential energy density functional:

Change the symmetry potential by varying the η

momentun dependent term:

22 /GeV500c

1.57MeV,

2

,,

2

0

1ln2

ijji

jiij

md ppU

2211

3/22

3/50

2/3221

,02211,

,02221

03,00

5432

3

24

1

)2

3()45(3

80

3

)12()12(364

1

2

45964

1

2

,16

1

18

3

2

xtxtC

txtg

xtxtg

txttg

tt

s

isosur

sur

2

03/5

0

3/82

0

,2

00

1

0

2

)(2

)]([212

spn

isosursurloc

Cg

ggu

1

SkP (K=200MeV)

Cross section

2 3 4

20

100

UrQMD-np-total UrQMD-pp-total Expt.-pp-tot Expt.-np-tot

cros

s se

ctio

n (m

b)

sNN

(GeV)

0.1 1 10 100 1000

10

100

UrQMD-pp-inel UrQMD-pp-el Expt.-pp-el Expt.-pp-inel

cros

s se

ctio

n (m

b)

Elab

(GeV)

0.1 1 10 100

10

100

UrQMD-np-inel UrQMD-np-el Expt.-np-el Expt.-np-inel

cross

sect

ion (m

b)

Elab(GeV)

[Ref] S.A. Bass et al. Prog.Part. Nucl. Phys. 41, 255 (1998)

Momentum-modified density-dependent nucleon nucleon elastic cross section (NNECS)

0 1 20.0

0.5

1.0

0.5 1.0

f

u

FU1 FU2 FU3 FU4

p (GeV/c)

FU3FP1 FU4FP14 FU4FP15 FU3FP16

[Ref] Qingfeng Li et al. PRC 83.044617

Cluster construction• minimum spanning tree (MST)

relative distances : dr<2.8 fm

relative momenta : dp<0.2 GeV/c

• isospin dependent minimum spanning tree (Iso-MST)

relative distances :

1. proton-proton, dr<2.5 fm

2. neutron-neutron, neutron-proton, dr<4.5 fm

relative momenta : dp<0.2 GeV/c

ImQMD: Yingxun Zhang and Zhuxia Li, et al. PRC 85, 051602(R) (2012)

relative momenta: dp<0.25 GeV/c

0 5 10 15 201E-3

0.01

0.1

1

10

100

yield

charge (Z)

MST FOPI Iso-MST

E=150A MeV

Resluts: yield

0 5 10 151E-4

1E-3

0.01

0.1

1

10

100

1000

yield

charge (Z)

MST FOPI Iso-MST

FU4FP15E=250A MeVAu+Au

Au+Au,b=0-2fm, SkP-FU3FP16,Hard-sphere

Resluts: proton and deuteron yield

100 100010

100

deuteron

FOPI-p FOPI-d MST-p MST-d iso-MST-p iso-MST-d

yiel

d

Elab (A MeV)

Au+Aub

0<0.15

SkP-FU3FP16 proton

100 1000

1

10

FOPI-t FOPI-He3 iso-MST-t iso-MST-He3 MST-t MST-He3

yiel

d

Elab

(A MeV)

triton

He3

Au+Au,b=0-2fm, SkP-FU3FP16,Hard-sphere

Resluts: directed flow of proton

100 10000.0

0.2

0.4

0.6

0.8

1.0

FU4FP14-p FU4FP14-p FOPI-b0<0.25

FOPI-0.25<b0<0.45

FU4FP15-pu

t0>0.8

V1 s

lope

of p

roto

n

Elab

(A MeV)

Resluts: directed flow of proton

400 600 800 1000 1200 1400 16000.0

0.2

0.4

0.6

0.8

1.0

FOPI-b0<0.25 FOPI-0.25<b0<0.45

FU3FP16-b0<0.25 FU3FP16-0.25<b0<0.45

FU4FP14-b0<0.25 FU4FP14-0.25<b0<0.45

FU4FP15-0.25<b0<0.45

ut0>0.4

V1 s

lope o

f pro

ton

Elab

(A MeV)

Resluts: directed flow of deuteron

100 10000.0

0.3

0.6

0.9

1.2

FOPI-b0<0.25

FOPI-0.25<b0<0.45

FU4FP14-d FU4FP14-d FU4FP15-d

ut0>0.8

V1 s

lope o

f deute

ron

Elab

(A MeV)

Resluts: directed flow of deuteron

400 600 800 1000 1200 1400 16000.0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1.0

FOPI-b0<0.25

FOPI-0.25<b0<0.45

FU3FP16-d FU3FP16-d FU4FP14-d FU4FP14-d FU4FP15-d

V1 s

lope o

f deute

ron

Elab

(A MeV)

Au+Au,ut0>0.4

Comparison with experimental data

[Ref] W.Reisdorf et al. NPA876.1-60 (2012)

0.0 0.2 0.4 0.6 0.8 1.0

0.0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1.0

V1

y0

p d FOPI-p FOPI-d

Au+AuE=1000A MeV0.25<b

0<0.45

ut0>0.4

FU3FP16

Comparison with experimental data

0.0 0.2 0.4 0.6 0.8 1.0

0.0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1.0

V1

y0

A3 He4 FOPI-A3 FOPI-He4

Au+AuE=1000A MeV0.25<b

0<0.45

ut0>0.4

FU3FP16

0.0 0.2 0.4 0.6 0.8 1.0

0.0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1.0

V1

y0

A3 He4 FOPI-He4 FOPI-A3

Au+AuE=250A MeV0.25<b

0<0.45

ut0>0.8

FU3FP16

Comparison with experimental data

Resluts: elliptic flow of proton

100 1000-0.125

-0.100

-0.075

-0.050

-0.025

0.000

0.025

0.050

FOPI-p FU3FP16 FU4FP15

Au+Au0.25<b

0<0.45

ut0>0.8

V2 o

f pro

ton

Elab

(A MeV)

Resluts: elliptic flow of deuteron

100 1000-0.20

-0.15

-0.10

-0.05

0.00

0.05

FOPI-d FU3FP16 FU4FP15

Au+Au0.25<b

0<0.45

ut0>0.8

V2 of

deu

tero

n

Elab

(A MeV)

Elliptic flow of A3 (triton and He3)

100 1000

-0.2

-0.1

0.0

FOPI-A3 FU3FP16 FU4FP15

Au+Au0.25<b

0<0.45

ut0>0.8

V2 o

f mass

3

Elab

(A MeV)

p d A3 He40.25

0.50

0.75

1.00

1.25

1.50

V1 sl

ope

Iso-MST MST FOPI

E=1500A MeV0.25<b

0<0.45

ut0>0.4

Influence of Iso-MST on directed flow

Result from FOPI experimentV

1 slo

pe

Elab=400A MeV

impact parameter b0

Comparison of directed flow of 3H with 3He

0.0 0.2 0.4 0.6 0.8 1.0

0.0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

H3 He3

E=1500A MeVAu+Au0.25<b

0<0.45

FU3FP16ut

0>0.4

V1

y0

3H: slope: 1.1120.0203He: slope: 1.0460.021

Comparison of directed flow of 3H with 3He

0.0 0.2 0.4 0.6 0.8 1.0

0.0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

H3 He3

FU3FP16E=1000A MeV0.25<b

0<0.45

ut0>0.4

V1

y0

3H: slope: 1.0990.0183He: slope: 1.0420.016

Comparison of directed flow of 3H with 3He

0.00

0.25

0.50

0.75

0.0 0.2 0.4 0.6 0.8

0.00

0.25

0.50

0.75

H3 He3

E=400A MeV0.25<b

0<0.45

ut0>0.4

V1

MST

H3: slope: 0.6320.024He3: slope: 0.6030.019

H3: slope: 0.5650.019He3: slope: 0.5360.014

Iso-MST

V1

y0

Summary

UrQMD model InitializationSkyrme potentialCross section-- nuclear medium effectCluster recognition-MST, Iso-MST

Study of collective flow of p, d, A3, He4 in heavy ion collisions in the 1A GeV regimeIso-MST influence on directed flowComparison of directed flow of 3H with 3He