Apparent Temperatures in Hot Quasi-Projectiles and the Caloric Curve View Full Text


Ontology type: schema:Chapter      Open Access: True


Chapter Info

DATE

1997

AUTHORS

J. Péter , M. Assenard , F. Gulminelli , Y.-G. Ma , A. Siwek , G. Auger , Ch. O. Bacri , J. Benlliure , E. Bisquer , F. Bocage , B. Borderie , R. Bougault , R. Brou , P. Buchet , J. L. Charvet , A. Chbihi , J. Colin , D. Cussol , R. Dayras , E. De Filippo , A. Demeyer , D. Doré , D. Durand , P. Eudes , J. D. Frankland , E. Galichet , E. Genouin-Duhamel , E. Gerlic , M. Germain , D. Gourio , D. Guinet , P. Lautesse , J. L. Laville , J. F. Lecolley , A. Le Fèvre , T. Lefort , R. Legrain , O. Lopez , M. Louvel , N. Marie , V. Métivier , L. Nalpas , A. D. Nguyen , M. Parlog , E. Plagnol , O. Politi , A. Rahmani , T. Reposeur , M. F. Rivet , E. Rosato , F. Saint-Laurent , S. Salou , J. C. Steckmeyer , M. Stern , G. Tabacaru , B. Tamain , L. Tassan-Got , O. Tirel , E. Vient , C. Volant , J. P. Wieleczko

ABSTRACT

The dependence of nuclear temperature upon excitation energy has been experimentally studied with increasing values of excitation energy over the years. At excitation energies per nucleon, E*/A, lower than 6 MeV the temperatures deduced from the kinetic properties of the emitted particles and clusters follow the Fermi gas law : E* = (A/k).T2. The value of the inverse level density parameter k was found to be in the range 8 to 13[1]. When excitation energies up to 10 MeV per nucléon were reached, temperatures obtained from the relative populations of excited levels in the emitted light nuclei did not overcome 5–6 MeV[2], but this limitation could be explained by side-feeding effects. Such hot nuclei were formed in fusion or deep inelastic reactions. At incident energies above 40–50 MeV/u, binary dissipative collisions dominate and the quasi-projectiles reach excitation energies per nuclEon and kinetic temperatures above 10 MeV[4, 5]. The study of projectile “spectators” in reactions at several hundreds of MeV/u made it possible to reach similar excitation energies[3]. In this Aladin experiment at GSI, the temperature was obtained via the relative abundances of two isotope pairs[6]. The relation between this temperature Tr0 and E*/A was interpreted as indicating a phase transition, with the nuclear gas regime dominating above E*/A = 10 MeV, as predicted[7]. However, a monotonic increase of the temperature with excitation energy was observed in similar conditions[8] and questions were raised about the significance of these caloric curves[9, 10, 11, 12], about the role played by the mass dependence of the decaying nucleus upon E*/A[13], as well as the strong effects of side-feeding, especially at high temperatures [14]. This point will be discussed by Xi Hong Fei at this meeting.[15]. More... »

PAGES

91-98

References to SciGraph publications

Identifiers

URI

http://scigraph.springernature.com/pub.10.1007/978-1-4615-4905-5_12

DOI

http://dx.doi.org/10.1007/978-1-4615-4905-5_12

DIMENSIONS

https://app.dimensions.ai/details/publication/pub.1037702167


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22 schema:description The dependence of nuclear temperature upon excitation energy has been experimentally studied with increasing values of excitation energy over the years. At excitation energies per nucleon, E*/A, lower than 6 MeV the temperatures deduced from the kinetic properties of the emitted particles and clusters follow the Fermi gas law : E* = (A/k).T2. The value of the inverse level density parameter k was found to be in the range 8 to 13[1]. When excitation energies up to 10 MeV per nucléon were reached, temperatures obtained from the relative populations of excited levels in the emitted light nuclei did not overcome 5–6 MeV[2], but this limitation could be explained by side-feeding effects. Such hot nuclei were formed in fusion or deep inelastic reactions. At incident energies above 40–50 MeV/u, binary dissipative collisions dominate and the quasi-projectiles reach excitation energies per nuclEon and kinetic temperatures above 10 MeV[4, 5]. The study of projectile “spectators” in reactions at several hundreds of MeV/u made it possible to reach similar excitation energies[3]. In this Aladin experiment at GSI, the temperature was obtained via the relative abundances of two isotope pairs[6]. The relation between this temperature Tr0 and E*/A was interpreted as indicating a phase transition, with the nuclear gas regime dominating above E*/A = 10 MeV, as predicted[7]. However, a monotonic increase of the temperature with excitation energy was observed in similar conditions[8] and questions were raised about the significance of these caloric curves[9, 10, 11, 12], about the role played by the mass dependence of the decaying nucleus upon E*/A[13], as well as the strong effects of side-feeding, especially at high temperatures [14]. This point will be discussed by Xi Hong Fei at this meeting.[15].
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