Bimodality and Coulomb effects with a canonical thermodynamic model
| dc.creator | Chaudhuri, G. | |
| dc.creator | Gupta, S. Das | |
| dc.creator | Gulminelli, F. | |
| dc.date | 2008-09-01 | |
| dc.date.accessioned | 2026-07-07T12:15:26Z | |
| dc.date.available | 2026-07-07T12:15:26Z | |
| dc.description | The effect of the Coulomb interaction on the phase diagram of finite nuclei is studied within the Canonical Thermodynamic Model. If Coulomb effects are artificially switched off, this model shows a phenomenology consistent with the liquid-gas phase transition. The inclusion of Coulomb does not significantly affect the phase diagram but it drastically modifies the nature and order parameter of the transition. A clear understanding of the phenomenon can be achieved looking at the distribution of the largest fragment produced in each fragmentation event. Possible connections with experimental observations are outlined. | |
| dc.description | Submitted to NPA | |
| dc.identifier | https://arxiv.org/abs/0809.0170 | |
| dc.identifier | http://arxiv.org/abs/0809.0170 | |
| dc.identifier | Nucl.Phys.A815:89-99,2009 | |
| dc.identifier | doi:10.1016/j.nuclphysa.2008.11.001 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/211495 | |
| dc.subject | Nuclear Theory | |
| dc.title | Bimodality and Coulomb effects with a canonical thermodynamic model | |
| dc.type | text |