FRAGMENTATION PHASE-TRANSITION IN ATOMIC CLUSTERS .1. MICROCANONICAL THERMODYNAMICS

Citation
Dhe. Gross et al., FRAGMENTATION PHASE-TRANSITION IN ATOMIC CLUSTERS .1. MICROCANONICAL THERMODYNAMICS, Zeitschrift fur Physik. D, Atoms, molecules and clusters, 39(1), 1997, pp. 75-83
Citations number
45
Categorie Soggetti
Physics, Atomic, Molecular & Chemical
ISSN journal
01787683
Volume
39
Issue
1
Year of publication
1997
Pages
75 - 83
Database
ISI
SICI code
0178-7683(1997)39:1<75:FPIAC.>2.0.ZU;2-Z
Abstract
The volume W of the accessible N-body phase space and its dependence o n the total energy is directly calculated. The famous Boltzmann relati on S = k ln(W) defines microcanonical thermodynamics (MT). We study how phase transitions appear in MT. Here we first develop the thermody namics of microcanonical phase transitions of first and second order i n systems which are thermodynamically stable in the sense of van Hove. We show how both kinds of phase transitions can unambiguously be iden tified in relatively small isolated systems of similar to 100 atoms by the shape of the microcanonical caloric equation of state < T(E/N) > and not so well by the coexistence of two spatially clearly separated phases. i.e. within microcanonical thermodynamics one does not need to go to the thermodynamic limit in order to identify phase transitions. In contrast to ordinary (canonical) thermodynamics of the bulk microc anonical thermodynamics (MT) gives an insight into the coexistence reg ion. Here the form of the specific heat c(E/N) connects transitions of first and second order in a natural way. The essential three paramete rs which identify the transition to be of first order, the transition temperature T-tr, the latent heat q(lat), and the interphase surface e ntropy Delta s(surf) can very well be determined in relatively small s ystems like clusters by MT. It turns out to be essential whether the c luster is studied canonically at constant temperature or microcanonica lly at constant energy. Especially the study of phase separations like solid and liquid or, as studied here, liquid and gas is very natural in the microcanonical ensemble, whereas phase separations become expon entially suppressed within the canonical description. The phase transi tion towards fragmentation is introduced. The general features of MT a s applied to the fragmentation of atomic clusters are discussed. The s imilarities and differences to the boiling of macrosystems are pointed out.