two-component (neutron/proton) statistical description of low-energy heavy-ion reactions
DESCRIPTION
Two-component (neutron/proton) statistical description of low-energy heavy-ion reactions. E. Běták & M. Veselský Institute of Physics, Slovak Academy of Sciences 84511 Bratislava, Slovakia. Introduction Deep-inelastic – effect of neutron/proton composition at periphery - PowerPoint PPT PresentationTRANSCRIPT
EURISOL workshop, ECT* Trento, 16-20 Jan. 2006 1
Two-component (neutron/proton)statistical description
of low-energy heavy-ion reactions
E. Běták & M. Veselský
Institute of Physics, Slovak Academy of Sciences
84511 Bratislava, Slovakia
EURISOL workshop, ECT* Trento, 16-20 Jan. 2006 2
• Introduction
• Deep-inelastic – effect of neutron/proton composition at periphery
• Time scales of the processes
• Possible playground for pre-equilibrium
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Experiments: 86Kr on 64Ni, 112,124Sn at 25 A MeV:
- observed excess of exp. yields of neutron-rich nuclei with Z=32-34 (sometimes in wider range)
- explainable within DIT, but better fit with scaled transfer probabilities
(for details: Veselský, Souliotis: Nucl. Phys. A765 (2006), 252)
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Standard DIT ( Tassan-Got & Stefan, NPA 524 (1991) )86Kr + 64Ni at 25 AMeV
Solid - GEMINI, dash-SMM
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Correlation of skin thickness to isovector chemical potential(V. Kolomietz et al, PRC 64(2001)024315, extended Thomas-Fermi calculation)
Rn-R
p determines the difference
of N/Z at (Rn+R
p)/2 ( surface ) from
the bulk N/Z, correlates to isovector chemical potential
DIT (T-G) : macroscopic formula for R
n-R
p used, values unrealistically
large, but bulk N/Z dynamics described well
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Modified DIT (Veselský & Souliotis: Nucl.Phys. A765 (2006)):phenomenological correction, effect of shell structure on nuclear periphery (assuming Rn-Rp vs.
n-
p correlation) and
thus on transfer probabilities estimated as:
where S... = S
...exp - S
...ld , is a free parameter ( = 0.53 determined
as optimal value), s > 0 fm (only non-overlapping configurations considered)
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Modified DIT (Veselský & Souliotis: Nucl. Phys. A765)86Kr + 64Ni at 25 AMeV
solid - GEMINI, dash -SMM
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DIT Conclusions - 86Kr + 64Ni, 112,124Sn at 25 AMeV
- a microscopic correction to macroscopic DIT describes the effect of isospin asymmetry at nuclear periphery
- inversion of the bulk isospin flow due to microscopic structure at nuclear periphery
- consistent parameters for all reactions
- SMM reproduces the yields of n-rich species well while overestimating the yields of -stable isotopes close to the projectile
- GEMINI typically overestimates the width of mass distributions
- for p-rich target 112Sn stronger Coulomb interaction supresses the effect of isospin asymmetry at nuclear periphery at s < 1 fm
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Time scale (example):
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Pre-equilibrium (exciton model – master eq.):
- initial excited zone should follow the Z/N composition of overlapping region – importance of surfaces
- initial number of excitons can be estimated from the overlap of nuclei in momentum space
at higher energies and
at lower energies (below 5 or 10 A MeV above Coulomb)
projCcm AVEnE /)(54.06.4/ 0
projCcmprojT
projTproj AVE
AA
AAAn /)()08.038.0(09.0/0
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Inclusion of spin - HIC:
)()(' lEElE rotcmcm
(Běták: Fizika B12 (2003), 11)
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Pre-equilibrium exciton model suitable instrument to describe the effect of the neutron/proton composition of the initial overlapping region.
Features:
- model estimates of n0
- spin- and energy- distributions of initial phase
- spin couplings as necessary
- includes also equilibrated (CN) emission
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Thank you
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Experiments at fragment separator MARS ( Cyclotron Lab, Texas A&M University ).
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86Kr + 124Sn at 25 AMeV Standard DIT ( Tassan-Got )
solid - GEMINI, dash -SMM
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86Kr + 124Sn at 25 AMeV Modified DIT (nucl-th/0507026):
solid - GEMINI, dash -SMM
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86Kr + 112Sn at 25 AMeV Standard DIT ( Tassan-Got )
solid - GEMINI, dash -SMM
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86Kr + 112Sn at 25 AMeV Modified DIT (nucl-th/0507026):
solid - GEMINI, dash -SMM Dash-dotted - SMM, s > 0.8 fm
EURISOL workshop, ECT* Trento, 16-20 Jan. 2006 2386Kr + 64Ni at 25 AMeV, Exp. vs. Sim. vs Sim. ICF-only
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Isoscaling in nuclear processes
M.B. Tsang et al., PRL 86(2001)5023
G. Souliotis et al., PRC 68(2003)24605
M. Veselský et al., PRC 69(2004)44607