1991
DOI: 10.1103/physreva.44.6294
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Models of fragmentation and partitioning phenomena based on the symmetric groupSnand combinational analysis

Abstract: Various models for fragmentation and partitioning phenomena are developed using methods from permutation groups and combinational analysis. The appearance and properties of power laws in these models are discussed. Several exactly soluble cases are studied. An application to nuclear fragmentation and clusterization is given. A connection with Ewenss approach [Theor. Popul. Biol. 3, 87 (1972); Mathematical Population Genetics (Springer, Berlin, 1979)] to genetic diversity is mentioned. Applications to the socia… Show more

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Cited by 50 publications
(63 citation statements)
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“…That is, for any given permutation, the total A is equal to the sum of the cycle length times the number of cycles of that length in that specific permutation. The canonical partition function for non-interacting particles such as Fermi-Dirac or Bose-Einstein particles in a box or in a one body potential well such as a harmonic oscillator well has a form given by eq.2 in section 2 [85,86,87]. For identical particles in a box of volume V and a system at temperature T , the ω weight factor for a cycle of length k is that of eq.6 with the q k = 1 in that equation for Bose-Einstein particles and q k = (−1) (k+1) for Fermi-Dirac particles.…”
Section: Applications To Other Areasmentioning
confidence: 99%
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“…That is, for any given permutation, the total A is equal to the sum of the cycle length times the number of cycles of that length in that specific permutation. The canonical partition function for non-interacting particles such as Fermi-Dirac or Bose-Einstein particles in a box or in a one body potential well such as a harmonic oscillator well has a form given by eq.2 in section 2 [85,86,87]. For identical particles in a box of volume V and a system at temperature T , the ω weight factor for a cycle of length k is that of eq.6 with the q k = 1 in that equation for Bose-Einstein particles and q k = (−1) (k+1) for Fermi-Dirac particles.…”
Section: Applications To Other Areasmentioning
confidence: 99%
“…A reader interested in the application of the methods of sect.2 to multiparticle multiplicity distributions can find the details and several other individual cases in [89,90]. In a series of papers [85,86], Hegyi has considered many interesting aspects of multiparticle production and has also introduced a generalized distribution for its description.…”
Section: Applications To Other Areasmentioning
confidence: 99%
“…A previous set of papers [1][2][3] proposed a statistical model for describing this behavior. Each possible fragmentation outcome is given a particular probability, and the resulting partition functions and ensemble averages are known to be exactly solvable.…”
Section: Introductionmentioning
confidence: 99%
“…Most treatments of the equation of state have treated heated nuclear matter as a homogeneous system. Statistical [5][6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21][22][23] and percolation [24][25][26] models have been used by many groups to study nuclear multifragmentation and the role of clusters on nuclear properties. This paper explores various thermodynamic properties using an exactly solvable canonical ensemble model that allows for clusterization and leads to simple analytic expressions for thermodynamic quantities such as the equation of state.…”
mentioning
confidence: 99%
“…In earlier papers [20][21][22][23] the question of the thermodynamics of a fragmenting system was raised. There, it was assumed that the thermodynamic variables were contained in a single parameter x such that the weight of a particular cluster partition was proportional to x m , where m is the total number of clusters in that partition.…”
mentioning
confidence: 99%