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TERS v2.0: An improved version of TERS
We present a new version of the semimicroscopic Monte Carlo code “TERS”. The procedure for calculating multiple small angle Coulomb scattering of the residues in the target has been modified. Target-backing and residue charge-reset foils, which are often used in heavy ion-induced complete fusion rea...
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Published in: | Computer physics communications 2009-11, Vol.180 (11), p.2392-2393 |
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Main Author: | |
Format: | Article |
Language: | English |
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Citations: | Items that cite this one |
Online Access: | Get full text |
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Summary: | We present a new version of the semimicroscopic Monte Carlo code “TERS”. The procedure for calculating multiple small angle Coulomb scattering of the residues in the target has been modified. Target-backing and residue charge-reset foils, which are often used in heavy ion-induced complete fusion reactions, are included in the code.
Program title: TERS v2.0
Catalogue identifier: AEBD_v2_0
Program summary URL:http://cpc.cs.qub.ac.uk/summaries/AEBD_v2_0.html
Program obtainable from: CPC Program Library, Queen's University, Belfast, N. Ireland
Licensing provisions: Standard CPC licence, http://cpc.cs.qub.ac.uk/licence/licence.html
No. of lines in distributed program, including test data, etc.: 7309
No. of bytes in distributed program, including test data, etc.: 1 219 555
Distribution format: tar.gz
Programming language: C
Computer: The code has been developed and tested on a PC with Intel Pentium IV processor.
Operating system: Linux
RAM: About 8 Mbytes
Classification: 17.7
External routines: pgplot graphics subroutine library [1] should be installed in the system for generating residue trajectory plots. (The library is included in the CPC distribution file.)
Catalogue identifier of previous version: AEBD_v1_0
Journal reference of previous version: Comput. Phys. Comm. 179 (2008) 492
Does the new version supersede the previous version?: Yes
Nature of problem: Recoil separators are employed to select and identify nuclei of interest, produced in a nuclear reaction, rejecting unreacted beam and other undesired reaction products. It is important to know what fraction of the selected nuclei, leaving the target, reach the detection system. This information is crucial for determining absolute cross section of the studied reaction.
Solution method: Interaction of projectiles with target nuclei is treated event by event, semimicro-scopically. Position and angle (with respect to beam direction), energy and charge state of the reaction products are calculated by Monte Carlo method. Trajectory of each nuclei inside the separator is then calculated by ion optical transfer matrix method. Ratio of the number of trajectories completing their journey up to the detection system to the total number of trajectories is a direct measure of absolute transmission efficiency of the separator.
Reasons for new version: The method for calculating mean squared scattering angle (〈ϑ〉2), used earlier [2], was found to be inadequate particularly for low energy heavy residues. Energy loss of be |
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ISSN: | 0010-4655 1879-2944 1386-9485 |
DOI: | 10.1016/j.cpc.2009.06.025 |