By W. J. Llope (auth.), Wolfgang Bauer, Alice Mignerey (eds.)
The research of nuclear dynamics is now in a single of its best stages. the idea is within the strategy of setting up an more and more trustworthy shipping description of heavy ion reactions from the preliminary violent part ruled via first collisions to the extra thermalized later phases of the response. this can be precise for the low-to-medium strength reactions, the place the dynamics is formulated by way of nucleonic, or quite often hadronic, levels of freedom. And it's also changing into a fact in ultrarelativistic heavy-ion reactions, the place partonic trouble-free levels of freedom must be used. Experiments at the moment are in a position to 'utilize the present accelerators and multiparticle detec tion structures to behavior extraordinary reports of heavy-ion collisions on an event-by-event foundation. furthermore, the sphere anticipates the crowning glory of the development of the Relativistic Heavy Ion Collider and the proposed improve of the nationwide Superconducting Cyclotron Laboratory, promising qualitatively new facts for the close to destiny. All of those efforts are primarily directed to the exploration of the swap the nuclear medium offers for the houses and interactions of person nucleons and, finally, the exploration of the nuclear subject section diagram. The research of this part dia gram, together with all the attention-grabbing part transitions expected from theoretical grounds, is the point of interest of lots of the theoretical and experimental investigations of nuclear dynamics carried out today.
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Arrow on the vertical axis indicates the Coulomb velocity (damped reactions). MeV. Future analysis will be dedicated to a sensitive determination of the primary sources in order to obtain an event classification for the study of hot nuclei de-excitation. REFERENCES 1. 2. 3. 4. 5. 6. 7. 8. 9. B. Borderie, Ann. de Phys. 17 (1992) 349. L. G. Moretto, G. 1. Wozniak, Ann. Rev. Nuel. Pal1. Sci . 43 (1993) 379. 1. Cugrfon, Phys. Lett. B135 (1984) 374. E. , Nuel. Phys. A495 (1989) 73e; E. , Phys. Lett.
_. I . ~ ••a. - ....... _ •. _- , ............ .... - ...... 1' .. ·.. .. 10 •• 3~ , 4p 15 . ty Figure 8. Relation between [(E* /A)1I2] and charge multiplicity. contribution of high-Z fragments, are virtually unaffected by the inclusion of prompt Z = 1 particles. We conclude that the extraction of critical exponents is unaffected by the inclusion of preequilibrium particles. 5. MULTIPLICITY AS A MEASURE OF TEMPERATURE In extracting the critical exponents, we have assumed that multiplicity is proportional to temperature in the critical region.
Also occurs for the expanding system of present interest. For example, a decrease of a from AI8 at 3 MeV to AI15 at 6 MeV 13 would change the slope of the T vs. m line but might not affect the linearity substantially. In any case, we plan to circumvent this problem by obtaining T(m) directly from the slopes of fragment spectra and, if possible, also from the ratios of isotopic yields. 6. CONCLUSIONS We have found evidence for critical fluctuations in the multifragment breakup of lA GeV gold nuclei.