energy dependence of the isotopic composition in nuclear fragmentation
DESCRIPTION
Energy Dependence of the Isotopic Composition in Nuclear Fragmentation. S. Yennello, D. Shetty , M. Veselsky , E. Martin, A. Keksis, G. Souliotis and D. Rowland Texas A&M University Cyclotron Institute. Two component liquid. Single component liquid. Two component liquid. Free n/p ratio - PowerPoint PPT PresentationTRANSCRIPT
Energy Dependence of the Isotopic Composition in Nuclear
Fragmentation
S. Yennello, D. Shetty, M. Veselsky, E. Martin, A. Keksis, G. Souliotis and
D. Rowland
Texas A&M University
Cyclotron Institute
Single component liquid
Two component liquid
Possible signatures:Free n/p ratiot/3He ratioN/Zfragments
Two component liquid
124Sn 124Sn
Veselsky, Phys. Rev. C 62, 064613 (2000).
0 100 200
100
0 50 100 150 200 250
100
0 50 100 150 200 250
10
100
0 50 100 150 200 250
10
100
(50MeV/nuc)
E*
QP, MeV
Co
un
ts (
arb
. u
nits
)
Co
un
ts (
arb
. u
nits
)
E*
QP, MeV
(30MeV/nuc)
E*
QP, MeV
Veselsky, Phys. Rev. C 62, 064613 (2000).
28Si + 112,124SnE*=2.5-3.5 E*=3.5-4.5 E*=4.5-5.5
E*=5.5-6.5 E*=6.5-7.5 E*=7.5-8.5
E*=8.5-9.5 E*=9.5-10.5 E*=10.5-12.5
Veselsky,Phys Lett B 497,1(2001)
QPZNaa
HeY
HY213
3
ln
Ratio of isotopic yields58Ni, 58Fe + 58Ni, 58Fe 30 Mev/nuc
ZNCeZNR ),(21
Scaling factor
ZeRS 21
Relative free neutron and proton densities
NiNinn
/
NiNipp
/
Scaling factor at 30,40,47 MeV/nuc
neutron and proton densities at 30,40,47 MeV/nuc
NiNinn
/
NiNipp
/
Energy dependence of the scaling parameter
30 MeV 40 MeV 47 MeV
0.372 0.269 0.23
-0.395 -0.372 -0.32
0.15
0.2
0.25
0.3
0.35
0.4
25 30 35 40 45 50
Beam Energy ( MeV/nuc)
alp
ha
.
Tsang PRC64, 054615 (2002)
58Fe + 58Fe / 58Ni + 58Ni
Botvina IsoscalingR21 = C exp(’A + ’(N-Z)
30 MeV/nuc 50 MeV/nuc
’ = 0.237±0.038 ’ = 0.186±0.017
’ = (n + p)/2T
’ = (n - p)/2T
28Si + 112,124Sn
Botvina IsoscalingR21 = C exp(’A + ’(N-Z)
28Si + 112,124Sn ; 50 MeV/nuc
E*
(MeV)
’
3 0.31
4 0.20
5 0.19
6 0.18
7 0.17
Summary
• The enhancement in free neutrons of neutron-rich systems is greater at lower energies.– Isoscaling in 58Ni, 58Fe + 58Ni, 58Fe– 3H/3He in 28Si + 112Sn, 124Sn– Isoscaling in 28Si + 112Sn, 124Sn
Chomaz PLB 47, 221 (1999)
Baran Nucl Phys 1999
Bao An Li PRL 2000
Theory
Summary
• The enhancement in free neutrons of neutron-rich systems is greater at lower energies.– Isoscaling in 58Ni, 58Fe + 58Ni, 58Fe– 3H/3He in 28Si + 112Sn, 124Sn– Isoscaling in 28Si + 112Sn, 124Sn
• Theoretical comparisons are in progress.
This work was supported in part by the Department of Energy and the Robert A Welch Foundation