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SpecTk
NSCL DAQ, SpecTcl
ARIS SpecTcl development
FRIB Estimated Rates
The projected beam intensities at FRIB are available online at
FRIB Beam Rate Calculator
Tools for COSY and LISE++ from Mauricio Portillo
Transport Integral: A method to calculate the time evolution
of phase-space distributions
D.Bazin and B.M.Sherrill, Physical Review E, vol.50 (5), 1994, pp.4017-4021.
An analytical technique using integral equations for
the transport of ion-optical intensity distributions through magnetic systems
is described. It can serve as an alternative to Monte Carlo simulation to
calculate the time evolution of phase-space distributions of any given shape.
Under the assumption of linear optics, the solution of the integral equations
can be reduced to convolution products. One major application of this
approach is the fast calculation of the transmission and purification of
radioactive nuclear beams produced by projectile fragmentation.
transport_integral.pdf
Application to fusion-evaporation: LisFus & PACE4
O.B.Tarasov, D.Bazin, NIM B204 (2003) 174-178
A new fusion-evaporation model, LisFus,
for the fast calculation of fusion-residue cross sections has been developed within
the framework of the LISE code.
This model can calculate very small cross sections quickly compared with
programs using the Monte Carlo method. This type of fast calculation is
necessary to estimate fusion-residue yields. Using this model, the LISE program
can now calculate the transmission of fusion residues
through a fragment separator.
It
is also possible to use fusion-residue cross sections calculated by the
program PACE,
which has been incorporated into the LISE package. The PACE code is a modified version of JULIAN,
the Hillman-Eyal evaporation code, using a Monte Carlo treatment of angular
momentum. A comparison between PACE and the
LisFus model is presented.
NIM B204 (2003) 174-178
5_15/lise_5_15.html
Universal parameterization
of momentum distribution of
projectile fragmentation products
Fragment momentum distributions measured in relativistic heavy-ion
collisions are typically observed to be Gaussian-shaped. Within the framework of the well-known statistical model,
a parabolic dependence of the width of the Gaussian momentum distributions is obtained, and the fragment velocity is equal to the projectile velocity.
However, this model is unable to account for the following:
The differences in widths associated with nuclides of the same mass;
The apparently anomalously small values of s0 observed at lower energies;
The reduction of the fragment-to-projectile velocity ratio at low energies;
The occurrence of an exponential tail in momentum distributions in reactions at low energies
Different models, both theoretical and empirical parameterizations, have been developed to explain these phenomena. Each of these
models has advantages and drawbacks depending on energy, projectile mass, and other parameters. The universal parameterization, which avoids the indicated drawbacks inherent in the statistical
model, has been developed and adapted in the LISE program.
This momentum-distribution model is universal: it includes a definition of the distribution width depending on beam energy and
on prefragment excitation energy, an estimate of the most probable fragment velocity, and a low-energy exponential tail. An attempt to describe experimental distributions of fragmentation products was made
using a convolution of Gaussian and exponential line shapes.
NNC 2003, Moscow (pdf 1.6 MB)
2026, compilation (pdf 2.3 MB)
Nuclear Physics A734 (2004) 536-540 (pdf 0.3 MB)
Statistical model calculations in heavy ion reactions (PACE)
A.Gavron, Phys.Rev. C21 (1980) 230-236
Results of various fusion experiments with heavy ions are compared with
predictions of model calculations (PACE). In some reactions there is evidence for
nonstatistical effects based on significant discrepancies between the
calculations and the experimental results. Alternative explanations of these
discrepancies are considered.
pace2.pdf
Calculated Nuclide Production Yields in Relativistic Collisions of Fissile Nuclei
J.Benlliure, A.Grewe, M.de Jong, K.-H.Schmidt, S.Zhdanov
Nucl.Phys. A628, 458 (1998)
A model calculation is presented which predicts the complex nuclide distribution resulting from peripheral relativistic heavy-ion collisions involving fissile nuclei. The model is based on a modern version of the abrasion-ablation model which describes the formation of excited prefragments due to the nuclear collisions and their consecutive decay. The competition between the evaporation of different light particles and fission is computed with an evaporation code which takes dissipative effects and the emission of intermediate-mass fragments into account. The nuclide distribution resulting from fission processes is treated by a semi-empirical description which includes the excitation-energy dependent influence of nuclear shell effects and pairing correlations. The calculations of collisions between 238U and different reaction partners reveal that a huge number of isotopes of all elements up to uranium is produced. The complex nuclide distribution shows the characteristics of fragmentation, mass-asymmetric low-energy fission and mass-symmetric high-energy fission. The yields of the different components for different reaction partners are studied. Consequences for technical applications are discussed.
NPA98_fission.pdf
A Reexamination of the Abrasion-Ablation Model for
the
Description of the Nuclear Fragmentation Reaction
J.-J.Gaimard, K.-H.Schmidt, Nucl.Phys. A531, 709 (1991)
The nuclear fragmentation reaction is studied as an important production
mechanism for secondary beams. The geometrical abrasion model and a
macroscopic evaporation model which describe the two steps of the reaction are
reexamined. Several improvements and modifications of these models are
discussed and a new model description incorporating these elements is
proposed. In particular, the excitation energy and the angular-momentum
distribution of the prefragments, the formulation of evaporation as a
diffusion process and the role of microscopic structure in the production
cross section are considered. The new model description preserves the
simplicity and the transparency of the original models. The predictions of the
new model are compared with those of the original models and with experimental
cross sections. While the original models showed several systematic
discrepancies in comparison to measured cross sections, the new model is able
to reproduce the whole body of experimental data with satisfactory agreement.
ABLA07 - towards a complete description of the decay channels of
a nuclear system from spontaneous fission to multifragmentation
Aleksandra Kelić, M. Valentina Ricciardi and Karl-Heinz Schmidt
The physics and the technical algorithms of the statistical de-excitation code ABLA07 are
documented. The new developments of ABLA07 have been guided by the empirical knowledge
obtained in a recent experimental campaign on the nuclide distributions measured at GSI,
Darmstadt. Besides distinct signatures of very asymmetric binary splits, lighter systems show
clear features of multifragmentation, while heavy systems reveal the influence of dynamics and
microscopic structure on the fission process. ABLA07 includes elaborate but efficient
descriptions of all these processes, with one set of the model parameters fixed for all systems
and all energies.
ABLA07.pdf
Modified Empirical Parametrization of Fragmentation Cross Section
K.Summerer, B.Blank, Phys.Rev. C61, 034607 (2000)
New experimental data obtained mainly at the GSI/FRS facility
allow one to modify the empirical parametrization
of fragmentation cross sections. It will be shown that minor
modifications of the parameters lead to
a much better reproduction of measured cross sections. The
most significant changes refer to the description of
fragmentation yields close to the projectile and of the memory
effect of neutron-deficient projectiles.
epax.pdf
ATIMA
ATIMA is a user program developed at GSI which calculates various
physical quantities characterizing the slowing-down of protons and heavy ions
in matter for specific kinetic energies ranging from 1 keV/u to 500 GeV/u such
as
- stopping power
- energy loss
- energy-loss straggling
- angular straggling
- range
- range straggling
- beam parameters (magnetic rigidity, time-of-flight, velocity, etc.)
- atomic charge-changing cross sections
- charge-state evolutions
- equilibrium charge-state distributions
http://www-linux.gsi.de/~weick/atima/
Charge states of relativistic heavy ions in matter
C.Scheidenberger, Th.Stohlker, W.E.Meyerhof, H.Geissel,
P.H. Mokler, B. Blank, NIM B142 (1998) 441-462.
Experimental and theoretical results on charge-exchange
cross-sections and charge-state distributions of relativistic
heavy ions penetrating through matter are presented. The data
were taken at the Lawrence Berkeley Laboratory's
BEVALAC accelerator and at the heavy-ion synchrotron SIS of
GSI in Darmstadt in the energy range 80 1000
MeV/u. Beams from Xe to U impinging on solid and gaseous
targets between Be and U were used. Theoretical models
for the charge-state evolution inside matter for a given
initial charge state are presented. For this purpose, computer
codes have been developed, which are briefly described.
Examples are given which show the successes and limitations
of the models.
charge-global.pdf
http://www-linux.gsi.de/~weick/charge_states/
Charged particle transport code
1. K.L. Brown, D.C. Carey, Ch. Iselin and F. Rothacker:
Transport, a Computer Program for Designing Charged Particle Beam Transport
Systems. CERN 73-16 (1973) & CERN 80-04 (1980).
2. Urs Rohrer,
Compendium of Transport Enhancements
Particle interactions with matter
The Stopping and Range of Ions in Matter (SRIM)
J.F.Ziegler
SRIM is a
group of programs that calculate the stopping and range of ions (up to 2
GeV/amu) in matter using a quantum-mechanical treatment of ion-atom
collisions (assuming a moving atom as an "ion", and all
target atoms as "atoms"). This calculation is made very
efficient by the use of statistical algorithms that allow the ion to make
jumps between calculated collisions and then average the collision results
over the intervening gap. During the collisions, the ion and atom have a
screened Coulomb collision, including exchange and correlation interactions
between the overlapping electron shells. The ion has long range interactions
creating electron excitations and plasmons within the target. These are
described by including the target's collective electronic
structure and interatomic bond structure when the calculation is set up (tables
of nominal values are supplied). The charge state of the ion within the target
is described using the concept of effective charge, which includes a velocity
dependent charge state and long range screening due to the collective electron
sea of the target.
http://www.srim.org
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