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DC Field | Value | Language |
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dc.contributor.author | Sangeeta | - |
dc.contributor.author | Ghosh, T. | - |
dc.contributor.author | Maheshwari, B. | - |
dc.contributor.author | Saxena, G. | - |
dc.contributor.author | Agrawal, B.K. | - |
dc.date.accessioned | 2022-06-22T13:30:55Z | - |
dc.date.available | 2022-06-22T13:30:55Z | - |
dc.date.issued | 2022-06-22 | - |
dc.identifier.uri | http://localhost:8080/xmlui/handle/123456789/3516 | - |
dc.description.abstract | The variation of total nuclear level densities (NLDs) and level density parameters with proton number (Z) are studied around the β-stable isotope, Z 0, for a given mass number. We perform our analysis for a mass range A = 40 to 180 using the NLDs from popularly used databases obtained with the single-particle energies from two different microscopic mass-models. These NLDs which include microscopic structural effects such as collective enhancement, pairing and shell corrections, do not exhibit inverted parabolic trend with a strong peak at Z 0 as predicted earlier. We also compute the NLDs using the single-particle energies from macroscopic-microscopic mass-model. Once the collective and pairing effects are ignored, the inverted parabolic trends of NLDs and the corresponding level density parameters become somewhat visible. Nevertheless, the factor that governs the (Z - Z 0) dependence of the level density parameter, leading to the inverted parabolic trend, is found to be smaller by an order of magnitude. We further find that the (Z - Z 0) dependence of NLDs is quite sensitive to the shell effects. | en_US |
dc.language.iso | en_US | en_US |
dc.subject | Level densities | en_US |
dc.subject | Level density parameter | en_US |
dc.subject | Microscopic effects | en_US |
dc.subject | Nuclear mass-models | en_US |
dc.subject | Statistical model for nuclear level densities | en_US |
dc.title | Nuclear level densities away from line of β-stability | en_US |
dc.type | Article | en_US |
Appears in Collections: | Year-2022 |
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