Title:
1 a) Neutron-Rich Rare Isotope Production in
the Fermi Energy Domain (Slides1-12)
b) Heavy Residue Properties, Isoscaling and
N/Z Equilibration (Slides 13-29)
 George A. Souliotis Collaborators M.
Veselsky, G. Chubarian, L. Trache, A. Keksis,
E. Martin, D.V. Shetty, S.J. Yennello Recent
research results presented at I
The International Conference of
Nucleon-Nucleon Collisions (NN03),
Moscow, June 17-22, 2003, and
The Institute of Nuclear Physics of
NCSR Demokritos, Athens,
Greece, June 24, 2003
2 Introduction
  Production of
Neutron-Rich Nuclides (methods) ? target,
projectile fission  ? cold projectile
fragmentation (medium to high energy) Â
? deep inelastic collisions (low to medium
energies) ? multinucleon transfer reactions
(around Vb) Â Â Present work deep inelastic
collisions at Fermi energies
? 86Kr(25MeV/nucleon) 64Ni, ( PLB 543
163 (2002) ? 86Kr
124Sn, 112Sn (PRL in press , nucl-ex 0302011)
? Heavy-Residue Yield
Scaling (nucl-ex 0305027) Findings ? Enhanced
production of neutron-rich species, neutron skin
effect ? Heavy-Residue Yield
Ratios probing N/Z equilibration
Applications with RIB from TAMU upgrade and RIA
3MARS Recoil Separator and Setup
Dispersive Image
D1
D2
Production Target
Wien Filter
Q3
Q2
Q1
D3
Final Achromatic Image
PPAC1 Start T X,Y
Q4
Q5
Rotatable Arm Reaction Angle 0-12o (selectable)
PPAC2 Stop T
Beam angle set to 0o (1.0-3.0o) for KrNi
(?gr 3.5o) 4o (2.5-5.5o) for KrSn (?gr
6.5o)
Silicon Telescope ?E1, X,Y (Strips) ?E2,
Eresidual
MARS Acceptances Anglular 9 msr Momentum 4
4Experimental Details
Reactions studied ? 86Kr 22 (25 MeV/u,
1-5 pnA) 64Ni (4 mg/cm2) PLFs in
1.0-3.0o (?gr 3.5o)
? 86Kr 22 (25 MeV/u, 1-5 pnA)
124,112Sn (2 mg/cm2) PLFs in 2.5-5.5o (?gr
6.5o) Measured quantities ? ?E1, ??2, ?r
, (x,y) strips ? time of flight
(START-STOP) ? x-position at First Image
(B? information)
Extracted physical quantities ? Velocity,
Energy loss, Total Energy ? Mass-to-charge
ratio A/Q B? A/Q ? ?
? Atomic Number Z
Z ? ?E1/2 ? Ionic charge Q
Q f(E, ?)
? Mass number A
A Qint ? A/Q Â Yield
distribution (Z,A,?) Â
5 Gross Distributions 86Kr (25 MeV/u) 64Ni
Isobaric Yield Distribution
- Â
- ----- DIT/GEMINI
- - - DIT/GEMINI
- (filtered)
Z - A Distribution (relatice to Z?)
Velocity - A Distribution
References
DIT L. Tassan-Got and C. Stephan, Nucl.
Phys. A524 121 (1991) GEMINI R. Chariy et al.,
Nucl. Phys. A483 391 (1988) EPAX K.
Summerer and B. Blank, Phys. Rev. C61 034607
(2000).
6 Gross Distributions 86Kr (25 MeV/u) 124Sn
? Data ? Data Corrected (?, B?)
Isobaric Yield Distribution
- -- DIT/GEMINI
- - DIT/GEMINI
- filtered (?,B?)
- - EPAX2
Z - A Distribution (relatice to Z?)
Velocity - A Distribution
References
DIT L. Tassan-Got and C. Stephan, Nucl.
Phys. A524 121 (1991) GEMINI R. Chariy et al.,
Nucl. Phys. A483 391 (1988) EPAX2 K. Summerer
and B. Blank, Phys. Rev. C61 034607 (2000).
7 Z, Q, ? spectra (one run) 86Kr (25 MeV/u)
64Ni
Resolutions (FWHM) ?Z 0.5
?Q 0.4
?A 0.5
8 Mass distribution of Ge (Z32) isotopes
86Kr (25 MeV/u) 64Ni
- 4p
- 4p1n
- 4p2n
9 Mass distributions 86Kr (25 MeV/u) 64Ni
? Data ---- EPAX ? DIT/GEMINI
Br
Se
Larger cross sections w.r.t. DIT/GEMINI or
EPAX (Z35-31)
Ge
As
Cross sections similar to DIT/GEMINI or EPAX (Z
? 30)
Zn
Ga
G.A. Souliotis et al., Phys. Lett. B 543, 163
(2002)
10Mass distributions (cont.) 86Kr (25 MeV/u)
64Ni
- Data
- ---- EPAX
- ? DIT/GEMINI
Ni
Cu
Measured cross sections are similar to
DIT/GEMINIand EPAX
Fe
Co
Cr
Mn
11Mass distributions 124Sn (20 MeV/u) 124Sn
- Data
- ---- EPAX
- ? DIT/GEMINI
?
Ni
Cu
Measured cross sections agree with
DIT/GEMINI They are 10-100 larger than EPAX
predictions
Fe
Co
Cr
Mn
12 Estimates of Production Rates 86Kr64Ni
Use cross sections of this work, assume
86Kr beam (25MeV/u) 100 pnA
64Ni target (20 mg/cm2)
Â
GSI data M. Weber et al . Nucl. Phys. A
578 (1994) 659
13 Mass distributions 86Kr (25 MeV/u) 124Sn,
112Sn
? 86Kr 124Sn ? 86Kr 112Sn ----- EPAX
Se
Br
Larger cross sections with the n-rich 124Sn
target (Z35-30)
Ge
As
Zn
Ga
G.A. Souliotis et al., Phys. Rev. Lett.
in press, nucl-ex/0302011
14 Neutron-Proton Density Calculations for 124Sn,
112Sn
n
neutron skin
p
n
p
Thomas-Fermi
V.M. Kolomietz, A.I. Sanzhur et al., PRC 64,
024315 (2001) ------- Skyrme-Hartree-Fock
J. Friedrich, P. Reinhard, PRC 33, 335 (1986)
15 Mass Distribution of Germanium from
86Kr(25MeV/u) 124Sn,112Sn, 64Ni
Data using targets ? 124Sn ? 112Sn ?
64Ni ------ EPAX2
Ge
Target N/Z
Valley of stability 124Sn 1.48
n-rich 118Sn
112Sn 1.24
n-poor 64Ni 1.29
n-rich 60Ni
16 Comparison Data, Calculations 86Kr (25
MeV/u) 124Sn, 112Sn
? Data DIT/GEMINI (standard)
DIT/GEMINI with ?(r) EPAX
Calculation with neutron skin appears to
account for the larger cross sections with the
n-rich 64Ni, 124Sn targets
G.A. Souliotis et al., Phys. Rev. Lett.
in press, nucl-ex/0302011
17 Comparison Data/EPAX 86Kr (25 MeV/u)
64Ni, 124Sn
For near-projectile fragments and above the
projectile N/Z, the cross sections are
larger. DIC between massive n-rich nuclei appear
to be advantageous for very high N/Z RIB
production
18 Velocity vs Z correlation
86Kr 124Sn 86Kr 112Sn
?min E/A 2.2 MeV T 5.3 MeV
86Kr 64Ni 86Kr 58Ni
?min
19 N/Z vs Z correlation
86Kr 124Sn 86Kr 112Sn
N/Z
86Kr 1.39 124Sn 1.44 112Sn 1.24
SL stability line
N/Z constant
EAL evaporation attractor line
86Kr 64Ni 86Kr 58Ni
64Ni 1.29 58Ni 1.07
R. Charity, Phys. Rev. C 58, 1073 (1998)
20 Scaling of Yield Ratios
86Kr124Sn,112Sn
R21 (N,Z) Y2/Y1
R21 C exp ( ? N )
R21 C exp ( ? Z )
21 Scaling of Yield Ratios
86Kr64Ni,58Ni
R21 (N,Z) Y2/Y1
R21 C exp ( ? N )
R21 C exp ( ? Z )
22 Isoscaling Parameters ?, ?
86Kr124Sn,112Sn
86Kr64Ni,58Ni
? 0.43 ? 0.27
R21 C exp ( ? N )
R21 C exp ( ? Z )
? 0.34 ? 0.51
23 Origin of Isotopic Scaling
Grand Canonical Ensemble (equilibrium limit)
Fragment Yield Y(N,Z) F(N,Z)
expB(N,Z)/T exp (N?nZ?p)/T R21 (N,Z)
Y2(N,Z) / Y1(N,Z) C exp ( ? N ? Z)
(Isoscaling) with ? ??n/T ?
??p/T ??n ? ??Sn
??p ? ??Sp
? 4 Csym/T ( (Z1/A1)2 (Z2/A2)2 )
Extracted Parameters
J. Randrup and S. Koonin, Nucl. Phys. A 356,
223 (1981) M. B. Tsang et al. Phys. Rev. C
64, 054615 (2001) A.S. Botvina et al. Phys.
Rev. C 65, 044610 (2002)
24 Heavy Residue Isoscaling and N/Z equilibration
R21 exp ( ? N )
N/Z 86Kr124Sn gt 210Rn 1.44 86Kr112Sn gt
198Rn 1.30
? 4 Csym/T ( (Z1/A1)2 (Z2/A2)2 )
? 8 Csym/T (Z/A)3ave ?(N/Z)
86Kr124Sn,112Sn
?(N/Z) 0.14 N/Z equilibrated quasi-projectile
Evolution towards N/Z equilibration of
quasi-projectile
M. B. Tsang et al. Phys. Rev. C 64, 054615
(2001) A.S. Botvina et al. Phys. Rev. C 65,
044610 (2002)
G.A. Souliotis et al., nucl-ex/0305004, Phys.
Rev. C submitted
25 Velocity and E vs mass correlations
86Kr 124Sn 86Kr 112Sn
?min E/A 2.2 MeV T 5.3 MeV
E/A max observed
26 Isobaric Scaling of Yield Ratios
R21(N,Z) Y2/Y1
R21 C exp ( ? N ? Z) Rearrange with
? (? ?)/2
? (?
-?)/2 R21 C exp ?A ?(N? Z) C exp (?A
2?tz )
86Kr124Sn,112Sn data
?0.47
? 0.47
?
A.S. Botvina et al. Phys. Rev. C 65, 044610
(2002)
27 Heavy Residue Isobaric Scaling and N/Z
equilibration
R21 exp ?? (N?Z)
N/Z 86Kr124Sn gt 210Rn 1.44 86Kr112Sn gt
198Rn 1.30
?? 4Csym/T (Z/A)2ave ?(N/Z)qp
86Kr124Sn,112Sn ? Isobaric approach ? Isotopic
approach
?(N/Z) 0.14 N/Z equilibrated quasi-projectile
Evolution towards N/Z equilibration of
quasi-projectile
N/Z equilibration continuous process strongly
correlated with E
G.A. Souliotis et al., nucl-ex/0305027, Phys.
Lett. B, submitted
Intermediate Energy S.J. Yennello et al,
Phys. Lett. B 321, 15 (1994) (IMF yield ratios)
B.A. Lee and S.J. Yennello, Phys. Rev.
C 52, 1746 (1995)
H. Johnston et al., Phys. Lett. B 371,
186 (1996)
28 Early N/Z equilibration studies
92Mo(15MeV/u) 238U, 154Sm (1)
Derived from data using evap. code
N/Z
Evolution towards N/Z equilibration
58Ni,64Ni (8.5MeV/u) 238U (2)
N/Z equilibrated quasi-projectiles
N/Z
DIC Model (Randrup)
58Ni measured
derived 64Ni measured
derived
(1) M. Petrovici et al. , Nucl. Phys. A 477,
277 (1988) (2) R. Planeta et al., Phys. Rev. C
38, 195 (1988)
29 Summary and Outlook
Measured charge, mass, velocity distributions of
residues from 86Kr (25 MeV/u) 64Ni, 124Sn,
112Sn, Studies inside ?gr Reaction simulations
DIT/Gemini reasonable description,
Effect of the Neutron Skin
(very n-rich products) Scaling of Heavy-Residue
Yields N/Z Equilibration Plans for future work
? Investigate reactions with heavier
targets 208Pb, 238U (look ?gr ) ? Study
the process of N/Z equilibration, E/A dependence
Tools at Texas AM ? Superconducting
Solenoid Rare Isotope Line (Large Acceptance)
? MARS Line (High Resolution) ? Future
Re-accelerated beams via a Gas-Cell based ISOL
concept
Application in studies using high-N/Z beams from
RIA
TAMU Cyclotron
White Paper in http//cyclotron.tamu.edu