Specific heat and bimodality in canonical and grand canonical versions of the thermodynamic model
| dc.creator | Chaudhuri, G. | |
| dc.creator | Gupta, S. Das | |
| dc.date | 2007-04-02 | |
| dc.date | 2007-08-26 | |
| dc.date.accessioned | 2026-07-07T10:35:25Z | |
| dc.date.available | 2026-07-07T10:35:25Z | |
| dc.description | We address two issues in the thermodynamic model for nuclear disassembly. Surprisingly large differences in results for specific heat were seen in predictions from the canonical and grand canonical ensembles when the nuclear system passes from liquid-gas co-existence to the pure gas phase. We are able to pinpoint and understand the reasons for such and other discrepancies when they appear. There is a subtle but important difference in the physics addressed in the two models. In particular if we reformulate the parameters in the canonical model to better approximate the physics addressed in the grand canonical model, calculations for observables converge. Next we turn to the issue of bimodality in the probability distribution of the largest fragment in both canonical and grand canonical ensembles. We demonstrate that this distribution is very closely related to average multiplicities. The relationship of the bimodal distribution to phase transition is discussed. | |
| dc.description | 19 pages, 5 figures | |
| dc.identifier | https://arxiv.org/abs/0704.0288 | |
| dc.identifier | http://arxiv.org/abs/0704.0288 | |
| dc.identifier | Phys.Rev.C76:014619,2007 | |
| dc.identifier | doi:10.1103/PhysRevC.76.014619 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/179744 | |
| dc.subject | Nuclear Theory | |
| dc.title | Specific heat and bimodality in canonical and grand canonical versions of the thermodynamic model | |
| dc.type | text |