plane PROBABILITY DISTRIBUTION

9
p l a n e P R O B A B I L I T Y D I S T R I B U T I O N T r a n s v e r s a l v e l o c i t y ( v x ) r e d u c t i o n w i t h i n c r 2 4 S n + 6 4 N i ( 3 5 A M e V ) b - i m p a c t p a r a m e t e r

description

124 Sn + 64 Ni (35AMeV) b- impact parameter.  plane PROBABILITY DISTRIBUTION. Transversal velocity (v x ) reduction with increasing b. 124. 64. Sn +. Ni 35 MeV/nucl. 1.5. AH/AL= 4.6-10. E. =2700-3100. 2F. exp. 1.4. theo. Filtered. 1.3. . 1.2. 1.1. - PowerPoint PPT Presentation

Transcript of plane PROBABILITY DISTRIBUTION

Page 1: plane PROBABILITY   DISTRIBUTION

plane P

RO

BA

BIL

ITY

DIS

TR

IBU

TIO

N

Tra n sv e rs al v e lo ci ty (v

x ) re d uc t io n wit h in c re as in g b

124Sn

+ 64N

i (35A

MeV

)b- im

pact param

eter

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Th. (No Filter included)

Filtered

-180 -150 -120 -90 -60 -30 0 30 60 90 120 150 180

1.0

1.1

1.2

1.3

1.4

1.5

exp

theo

AH/AL= 4.6-10E2F

=2700-3100

124Sn +

64Ni 35 MeV/nucl.

<V

_R

>

plane

Preliminary

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-180 -150 -120 -90 -60 -30 0 30 60 90 120 150 1800.9

1.0

1.1

1.2

1.3

1.4

1.5-180 -150 -120 -90 -60 -30 0 30 60 90 120 150 180

0.9

1.0

1.1

1.2

1.3

1.4

1.5-180 -150 -120 -90 -60 -30 0 30 60 90 120 150 180

0.9

1.0

1.1

1.2

1.3

1.4

1.5

E2F

=3500-3900

<V

_R

>

plane

E2F

=3100-3500

<V

_R

>1/25/03 14:03:40

AH/AL

124Sn + 64Ni 35 MeV/nucl.

E2F

=2700-3100

<

V_

R>

2.6-4.6 1.6-2.6 1.0-1.6

E.Piasecki et al. IWM(2001) November 28, Catania(I) (preliminary)

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r DE

PE

ND

EN

CE

OF

IMF

ISO

SP

IN C

OM

PO

SIT

ION

: EO

S IN

FL

UE

NC

E

asystiffasysoft

124Sn

+64N

i35A

MeV

124Sn

64Ni

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ISOSCALING and SYMMETRY ENERGY

Isoscaling result: lnR21=Ct+N+Z

Tn

T

p

2)(2)(

2

1

2

212

2

1

2

2

IIIIEII

Esym

sym

n

2)(2)(

2

1

2

212

2

1

2

2

IIIIEII

Esym

sym

p

Interpretation:

Consequences:

0

symE np

2

2

22

1

1 )()(4A

Z

A

ZEsymn

0

symE

1.)

2.)np )/( 0symsym CE for

np for )/( 0symsym CE

3.) ))((4

/

/ln 12

11

22 IIETZN

ZNsym

always

Derivation of )( sourcesymE ?Yes, if 12 , II measured

From Mirror Isobar Yield Ratios!

;

)exp()(),(

),(1,22,1 T

B

Z

N

NZY

ZNY

Observations: - too large N/Z for both n-rich and n-poor systems

- too small value for )( sourcesymE Problems: Evaporation corrections, Equilibrium scenario

Heavier IMF’s – liquid phase ?

1

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NECK ISOSCALING

N = 0.95

Z=1

Z=3

Z=2

Z=5 Z=7Z=6

Z=8

Z=4

Z=9lnR

21

NiSn

NiSn58112

64124

at 35 MeV/n (b=6,7,8fm) = 0.69

asystiff

asysoft

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Z

ln R

21NECK ISOSCALING

= -1.07

N=2

N=3

N=8N=7N=6N=5

N=4

NiSn

NiSn58112

64124

at 35 MeV/n (b=6,7,8fm)

= -0.68

asystiff

asysoft

“GRAND CANONICAL” NECK?

MeVII

ET sym 324

12

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Dynamical Isoscaling

Z=1

Z=7

primary

final

yieldionlightSn

Sn112

124

A

ZNR

AfZNY

12221

2

2

2ln

)(exp)(),(

not very sensitive to Esym ?

124Sn Carbon isotopes (primary)

A

Asy-softAsy-stiff

M.J. van Goethem, G. Verde,M. ColonnaMSU data (2001-02)

nucl-ex/0210004

50 AMeV

(central coll.)

Page 9: plane PROBABILITY   DISTRIBUTION

1. Competition of dissipative reaction mechanisms

2. N/Z of fast particle emission

3. (n,p) correlation functions

4. Isospin fractionation (isoscaling) *

5. Fragment multiplicities *

6. Isospin content of neck fragments *

7. Fast fission multiplicities

8. Isospin diffusion (charge equilibration)

9. n – p collective flows light isobar flows*

10. -/+ yields*

11. Deconfinement precursors

n-radii, n-star cooling, hybrid stars

ISOSPIN IN REACTIONS: ISOSPIN IN REACTIONS: EOS – SENSITIVE OBSERVABLESEOS – SENSITIVE OBSERVABLES

* Asy-stiff indications but low asymmetries so far