Title: Prezentace aplikace PowerPoint
1Spectator response to participants blast
-experimental evidence and possible implications
New tool for investigating the momentum-
dependent properties of nuclear matter.
Vladimir Henzl GSI-Darmstadt, Germany
2Outline
Introduction motivation
- properties of nuclear matter and relevance for
astrophysics - static vs. dynamic properties peculiarities of
investigated systems - standard tools of investigation collective
flows, kaon production, ...
Spectator response
- original idea and theoretical predictions
- first observation reacceleration of
fragmentation residues
Experimental approach possibilities of FRS
Results of dedicated experiments
- spectator response in AuAu _at_ 1 A GeV
- spectator response in AuAu,Al _at_ 500 A MeV
- comparison with BUU calculations
Summary Outlook
3General motivation
Astrophysical interest
- evolution of the early universe
- supernovae explosions
- formation and stability of neutron stars
influenced by properties of the nuclear matter
(NM)under extreme conditions (high T, P, ?, )
Properties of the NM
- static (in)compressibility, phase transitions,
excitation - dynamic viscosity, momentum dependence of the
mean field
4Static vs. dynamic properties
Aichelin et al. PRL 58(1987)1926
Static properties are studied in dynamical
processes !!!
Problem most of the experimental observables are
not selective
gt the interpretation is influenced by competing
phenomena,
!!! The results are very often ambiguous !!!
5Present knowledge
Recent analysis (Danielewicz et al.)
Science 298 (2002) 1592
Attempt to constrain nuclear matter equation of
state by results of performed experiments.
Only the most extreme models could be excluded
by the experiment
6Tools to investigate the nuclear matter
BUU calculations 124Sn 124Sn Tlab 800
MeV/u b 5 fm L. Shi, P. Danielewicz, R.
Lacey, PRC 64 (2001)
Standard tools
eliptic flow, radial flow, transverse momentum,
(anti)kaon production,
Spectator response
the spectator is not a passive witness, but
rather a victim of violent participants !
! New !
- L. Shi, P. Danielewicz, R. Lacey, PRC 64 (2001)
- M.V.Ricciardi et al. PRL 90(2003)212302
7Spectator response to the participant blast
8Spectator response or what can we learn from
victims
Theoretical prediction (Shi, Danielewicz, Lacey)
PCMS/A 682 MeV/c
- Net momentum change depends on nonlocality of
nuclear mean field. - Net momentum change is almost insensitive to the
stiffness of the EoS.
Spectator response is selectively sensitive to
nonlocal properties of nuclear mean field !!!
9Idea
BUU calculations 124Sn 124Sn Tlab 800
MeV/u b 5 fm L. Shi, P. Danielewicz, R.
Lacey, PRC 64 (2001)
Motivation for new experiments
1) to improve experimental signature of spec.
response
2) to establish correlation of Ares and impact
parameter b
3) to study possible dependence of spectator
response on incident energy and/or size of the
colliding system
Observation
Proposal of new experimental program
197Au197Au _at_ 0.5 and 1.0 A GeV
T.Enqvist et al. NPA658(1999)47
BUU by V.H.
... aproved and carried out in 2004
10Experimental approach
11Experiment at the Fragment Separator
Inverse kinematics
From ToF ??? /???? 400
A/?A 400
(36m)
Once mass and charge are identified (A, Z are
integer numbers) the velocity is calculated from
B?
??? /???? B?/?B? 2000
gt very precise determination!
12Characteristics of the data
AuAu_at_1 A GeV
Pbp_at_1 A GeV
- unambiguous identification precise
longitudinal momenta
- limited acceptance 15mrad, 1.5 in momentum
only one fragment in one reaction measured
13Velocity distributions with limited acceptance
136XenatPb _at_ 1 A GeV (D.Henzlova)
- limited momentum acceptance
Several magnetic field settings need to be
combined to get complete velocity distribution
(each color 1 magnetic setting)
14Information from full acceptance experiments
238UCu _at_ 1 A GeV - ALADIN
fission
fragmentation
197Au197Au _at_ 1 A GeV - ALADIN
fission
- single, unambiguously identified fragment at FRS
is predominantly largest residue per collision
15Information from the Zmax
Aladin data AuAu _at_ 400, 600, 800, 1000 A MeV
Aladin data AuAu _at_ 600 A MeV
- Zbound is a measure of the impact parameter
- the largest fragment is well correlated with
Zbound (for Zmaxgt30 Amaxgt65)
Zmax carries information on impact parameter
- fragments with Zgt20 are produced in reactions
with b 9fm (in AuAu system)
- peripheral collisions investigated
16Different reaction processes
How to distinguish fragmentation and fission?
238U (1 A GeV) Pb
197Au197Au _at_ 1 A GeV (V.H.)
fission
Fragmentation heaviest residues fully accepted
(Agt90)
Fission Only forward and backward component
accepted
17Results of dedicated experiments
18First dedicated experiment
V.H. PhD thesis (in preparation)
- most peripheral collisions yield deceleration
mean velocities in agreement with Morrissey
systematics.
- with decreasing mass loss, velocities level off
and increase
residues with Ares 85 on average faster than
the beam
19More dedicated experiments
V.H. PhD thesis (in preparation)
- reacceleration smaller with smaller incident
energy
- reacceleration smaller in smaller reaction
systems
all systems yield clearly visible net
reacceleration
Reacceleration and its behavior is an
experimental fact !
Interpretation possible only with help of
calculations
20New experimental data gt new simulations
- BUU calculations with MD mean fields
qualitatively agree with experiment (no
sensitivity to stiffness of EoS)
- BUU calculations with static MI field are not
able to describe trend of the data
BUT Correlation of Ares with impact parameter b
nontrivial !!!
21How to relate Ares and an impact parameter
Aladin
- Zmax2 has different (and worse) correlation with
Zbound (impact par.)
Region of mixing Zmax Zmax2 cant be used to
deduce b !
22New experimental data gt new simulations
Only data in blue area suitable for extraction of
impact parameter !!!
Calculations with MD MF induce gain of the
momenta, but for too low impact parameters with
respect to the experiment !!!
Open question which parameters of BUU can
influence the spectator response?
... one possible idea ...
23Summary outlook
24Summary Outlook
Summary
- longitudinal velocities of fragmentation
residues measured in AuAu _at_ 0.5, 1 A GeV, AuAl
_at_ 0.5 A MeV
- reacceleration phenomena seen in all systems,
its strength depends on incident energy and size
of the colliding system
- only BUU with MD MF induce recovery of the
fragment velocities with decreasing impact
parameter, in qualitative agreement with the
experiment
- further experiments simulations needed to
constrain MD properties of nuclear mean field
Outlook
- AuAu/Al _at_ 1/0.5 A GeV data analysis finished,
interpretation in progress
- More BUU calculations on the way, many more needed
- 112,124Sn112,124Sn _at_ 1 A GeV experiment in
preparation - 2005/2006
25Comparison with ALADIN
26Information from full acceptance experiments
197Au197Au 1AGeV - ALADIN
fission
fragmentation
- single, unambiguously identified fragment at FRS
is predominantly largest residue per collision