By Mark D. Baker (auth.), Wolfgang Bauer, Gary D. Westfall (eds.)

The twelfth iciness Workshop on Nuclear Dynamics carried at the culture, all started in 1978, of bringing jointly scientists operating in all regimes of nuclear dynamics. This huge variety of similar themes permits the researcher attending the Workshop to be uncovered to paintings that in general will be thought of outdoors his/her box, yet might po­ tentially upload a brand new size to the knowledge of his/her paintings. At Snowbird, we introduced jointly experimentalists operating with heavy ion beams from 10 MeV/nucleon as much as two hundred GeV /nucleon and theoretical physicists operating in different components starting from antisymmetrized fermionic dynamics to perturbative quantum chromo dynamics. Fu­ ture paintings at RHIC was once mentioned additionally, with shows from a number of of the experimen­ tal teams. moreover, a number of talks addressed problems with cross-disciplinary relevance, from the research of water-drop-collisions, to the multi-fragmentation of buckyballs. sincerely the sphere of nuclear dynamics has a vivid destiny. the certainty of the nuclear equation of kingdom in all of its manifestations is being increased on all fronts either theoretically and experimentally. destiny Workshops on Nuclear Dynamics will surely have a lot growth to file. Gary D. Westfall Wolfgang Bauer Michigan country Universzty v earlier WORKSHOPS the next desk features a checklist of the dates and destinations of the former iciness Workshops on Nuclear Dynamics in addition to the participants of the organizing committees. The chairpersons of the meetings are underlined.

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2 o 4 0 2 4 0 2 4 11 Figure 1. Transverse energy flow component Vj as a function of pseudorapidity centrality (PCal ET) windows. The reaction plane resolution has been unfolded. 1) for several The angle ef' = ef. y weighted sum over all ef •. In order to avoid autocorrelations the 'f/ range used for the azimuthal ET analysis has to be excluded from the efT determination. It turns out that the dominant anisotropy, and therefore the strength of the flow signal, is contained in the first moment VI within the parametrization d 2ET / def' d'f/ = (E T )/27r .

The present work attempts to distinguish between these two scenarios. Recent experimental results provide evidence that the characteristics of the multifragmenting system (excitation, size, charge, etc) change on a time scale concurrent with the fragment emission process [12, 13]. These results indicate that for IMFs with 4 :S Z :S 9 the strength of the fragment-fragment Coulomb interaction increases as the average velocity of the emitted fragments increase. Such a result is consistent with the prompt emission of energetic fragment pairs from a highly excited, and perhaps smaller, system and less energetic pairs at a later time when the system has cooled, and possibly expanded.

Thus, Aoki claimed that this decay mode is either blocked, or the Ho does not exist. 23 GeV /c 2 (2MA). However, Dover et al. pointed out[14] that Aoki's interpretation of the decay chain in this one event implies a repulsive interaction between two A particles, which disagrees with most 21 Table 2. 6 GeV /c/nucleon 197 AU+ 197 Au collisions that are predicted by several different models. 4 O. ~o. models of nuclear forces§. Very recently, two new claims of the existence of an Ho dibaryon were made.

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