V. Lindenstruth
GSI Helmholtz Centre for Heavy Ion Research
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Featured researches published by V. Lindenstruth.
Physical Review C | 2000
J. B. Elliott; S. Albergo; F. Bieser; F.P. Brady; Z. Caccia; D. Cebra; A. D. Chacon; J. L. Chance; Y. Choi; S. Costa; M. L. Gilkes; J. A. Hauger; A. Hirsch; E. Hjort; A. Insolia; M. Justice; D. Keane; J. C. Kintner; V. Lindenstruth; Michael Annan Lisa; H. S. Matis; M. A. McMahan; C. McParland; W. F. J. Müller; D. Olson; M. D. Partlan; N. Porile; R. Potenza; G. Rai; J. O. Rasmussen
The cluster distributions of three different systems are examined to search for signatures of a continuous phase transition. In a system known to possess such a phase transition, both sensitive and insensitive signatures are present; while in systems known not to possess such a phase transition, only insensitive signatures are present. It is shown that nuclear multifragmentation results in cluster distributions belonging to the former category, suggesting that the fragments are the result of a continuous phase transition.
Physical Review C | 2003
J. B. Elliott; L. G. Moretto; L. Phair; G. J. Wozniak; S. Albergo; F. Bieser; F.P. Brady; Z. Caccia; D. Cebra; A. D. Chacon; J. L. Chance; Y. Choi; S. Costa; M. L. Gilkes; J. A. Hauger; A. Hirsch; E. Hjort; A. Insolia; M. Justice; D. Keane; J. C. Kintner; V. Lindenstruth; Michael Annan Lisa; H. S. Matis; M. A. McMahan; C. McParland; W. F. J. Müller; D. Olson; M. D. Partlan; N. Porile
Author(s): Elliott, J.B.; Moretto, L.G.; Phair, L.; Wozniak, G.L.; Albergo, S.; Bieser, F.; Brady, F.P.; Caccia, Z.; Cebra, D.A.; Chacon, A.D.; Chance, J.L.; Choi, Y.; Costa, S.; Gilkes, M.L.; Hauger, J.A.; Hirsch, A.S.; Hjort, E.L.; Insolia, A.; Justice, M.; Keane, D.; Kintner, J.C.; Lindenstruth, V.; Lisa, M.A.; Matis, H.S.; McMahan, M.; McParland, C.; Muller, W.F.J.; Olson, D.L.; Partlan, M.D.; Porile, N.T.; Potenza, R.; Rai, G.; Rasmussen, J.; Ritter, H.G.; Romanski, J.; Romero, J.L.; Russo, G.V.; Sann, H.; Scharenberg, R.P.; Scott, A.; Shao, Y.; Srivastava, B.K.; Symons, T.J.M.; Tincknell, M.; Tuve, C.; Wang, S.; Warren, P.; Wieman, H.H.; Wienold, T.; Wolf, K.
Physical Review C | 2002
B. Srivastava; R. P. Scharenberg; S. Albergo; F. Bieser; F.P. Brady; Z. Caccia; D. Cebra; A. D. Chacon; J. L. Chance; Y. Choi; S. Costa; J. B. Elliott; M. L. Gilkes; J. A. Hauger; A. Hirsch; E. Hjort; A. Insolia; M. Justice; D. Keane; J. C. Kintner; V. Lindenstruth; Michael Annan Lisa; H. S. Matis; M. A. McMahan; C. McParland; W. F. J. Müller; D. Olson; M. D. Partlan; N. Porile; R. Potenza
A systematic analysis of the multifragmentation (MF) in fully reconstructed events from 1A GeV Au, La and Kr collisions with C has been performed. This data is used to provide a definitive test of the variable volume version of the statistical multifragmentation model (SMM). A single set of SMM parameters directly determined by the data and the semi-empiricalmass formula are used after the adjustable inverse level density parameter,
Physical Review Letters | 2000
J.B. Elliott; L. G. Moretto; L. Phair; G. J. Wozniak; S. Albergo; F. Bieser; F.P. Brady; Z. Caccia; D. Cebra; A. D. Chacon; J. L. Chance; Y. Choi; S. Costa; M. L. Gilkes; J. A. Hauger; A. Hirsch; E. Hjort; A. Insolia; M. Justice; D. Keane; J. C. Kintner; V. Lindenstruth; Michael Annan Lisa; H. S. Matis; M. A. McMahan; C. McParland; W. F. J. Müller; D. Olson; M. D. Partlan; N. Porile
epsilon_{o}
Physics Letters B | 1998
J. B. Elliott; S. Albergo; F. Bieser; F.P. Brady; Z. Caccia; D. Cebra; A. D. Chacon; J. L. Chance; Y. Choi; S. Costa; M. L. Gilkes; J. A. Hauger; A. Hirsch; E. Hjort; A. Insolia; M. Justice; D. Keane; J. C. Kintner; V. Lindenstruth; Michael Annan Lisa; H. S. Matis; M. A. McMahan; C. McParland; W. F. J. Müller; D. Olson; M. D. Partlan; N. Porile; R. Potenza; G. Rai; J. O. Rasmussen
is determined by the fragment distributions. The results from SMM for second stage multiplicity, size of the biggest fragment and the intermediate mass fragments are in excellent agreement with the data. Multifragmentation thresholds have been obtained for all three systems using SMM prior to secondary decay. The data indicate that both thermal excitation energy
NUCLEAR PHYSICS IN THE 21st CENTURY:International Nuclear Physics Conference INPC 2001 | 2001
J.B. Elliott; L.G. Moretto; L. Phair; G.J. Wozniak; Luc Beaulieu; H. Breuer; R. G. Korteling; K. Kwiatkowski; T. Lefort; L. Pienkowski; A. Ruangma; V. E. Viola; S. J. Yennello; S. Albergo; F. Bieser; F.P. Brady; Z. Caccia; D. Cebra; A.D. Chacon; J.L. Chance; Y. Choi; S. Costa; M.L. Gilkes; J. A. Hauger; A. Hirsch; E. L. Hjort; A. Insolia; M. Justice; D. Keane; J.C. Kintner
E_{th}^{*}
Physical Review Letters | 1996
J. A. Hauger; S. Albergo; F. Bieser; F.P. Brady; Z. Caccia; D. Cebra; A. D. Chacon; J. L. Chance; Y. Choi; S. Costa; J. B. Elliott; M. L. Gilkes; A. Hirsch; E. Hjort; A. Insolia; M. Justice; D. Keane; J. C. Kintner; V. Lindenstruth; M. A. Lisa; U. Lynen; H. S. Matis; M. A. McMahan; C. McParland; W. F. J. Müller; D. Olson; M. D. Partlan; N. Porile; R. Potenza; G. Rai
and the isotope ratio temperature
Physical Review Letters | 1994
M. L. Gilkes; S. Albergo; F. Bieser; F.P. Brady; Z. Caccia; D. Cebra; A. D. Chacon; J. L. Chance; Y. Choi; Salvatore Costa; J. B. Elliott; J. A. Hauger; A. Hirsch; E. L. Hjort; A. Insolia; M. Justice; D. Keane; J. C. Kintner; V. Lindenstruth; Michael Annan Lisa; U. Lynen; H. S. Matis; M. A. McMahan; C. McParland; W. F. J. Müller; D. L. Olson; M. D. Partlan; Norbert T. Porile; R. Potenza; G. Rai
T_{He-DT}
Physical Review Letters | 1993
M. B. Tsang; W. C. Hsi; W. G. Lynch; D. R. Bowman; C. K. Gelbke; M. A. Lisa; Graham F. Peaslee; G. J. Kunde; M. Begemann-Blaich; T. Hofmann; J. Hubele; J. Kempter; P. Kreutz; W. D. Kunze; V. Lindenstruth; U. Lynen; M. Mang; W. F. J. Müller; M. Neumann; B. Ocker; C. A. Ogilvie; J. Pochodzalla; F. Rosenberger; H. Sann; A. Schüttauf; V. Serfling; J. Stroth; W. Trautmann; A. Tucholski; A. Wörner
decrease with increase in system size at the critical point. The breakup temperature obtained from SMM also shows the same trend as seen in the data. The SMM model is used to study the nature of the MF phase transition. The caloric curve for Kr exhibits back-bending (finite latent heat) while the caloric curves for Au and La are consistent with a continuous phase transition (nearly zero latent heat) and the values of the critical exponents
Physical Review Letters | 1994
W. C. Hsi; G. J. Kunde; J. Pochodzalla; W. G. Lynch; M. B. Tsang; M. L. Begemann-Blaich; D. R. Bowman; R. J. Charity; F. Cosmo; A. Ferrero; C. K. Gelbke; T. Glasmacher; T. Hofmann; G. Imme; I. Iori; J. Hubele; J. Kempter; P. Kreutz; W. D. Kunze; V. Lindenstruth; Michael Annan Lisa; U. Lynen; M. Mang; A. Moroni; W. F. J. Müller; M. Neumann; B. Ocker; C.A. Ogilvie; Graham F. Peaslee; G. Raciti
tau