{"created":"2020-03-08T09:01:31.190275+00:00","id":838,"links":{},"metadata":{"_buckets":{"deposit":"f4948886-146d-48c2-b036-5b25ae7583eb"},"_deposit":{"id":"838","owners":[],"pid":{"revision_id":0,"type":"recid","value":"838"},"status":"published"},"_oai":{"id":"oai:meral.edu.mm:recid/838","sets":["1582963739756:1582967025340"]},"communities":["um"],"control_number":"838","item_1583103067471":{"attribute_name":"Title","attribute_value_mlt":[{"subitem_1551255647225":"Structure Analysis of Light [I] - Hypernuclei","subitem_1551255648112":"en"}]},"item_1583103085720":{"attribute_name":"Description","attribute_value_mlt":[{"interim":"In this research work, the binding energies of light ; hypernuclei namely ; -\r 12C, ; -\r 14N and ; -\r 16O have been calculated within the frame work of ; single-particle model by solving\r nonrelativistic Schrödinger equation. In this calculation, the Gaussian basis wave function and\r phenomenological Woods-Saxon central potential including coulomb interaction are used. By\r using the strength of Woods-Saxon potential -14.0 MeV, the calculated bound state energy of ; -\r 14N is 3.07 MeV over binding than the recent experimental results, 4.38 r 0.25 MeV which\r is observed from E373 experiment, KEK, Japan. Therefore, the binding energies of ; -\r 14N\r have investigated by varying potential strength. At the potential depth -8.5 MeV, the calculated\r binding energy of ; -\r 14N is in good agreement with the experimental result. Therefore, this\r potential strength is applied to study the structure analysis of other two light ; hypernuclei.\r The observed binding energies of 1S state for ; -\r 12C and ; -\r 16O are 3.64 MeV and 5.09 MeV\r respectively. In addition, the root-mean-square radii of these light ; hypernuclei have also\r investigated. The calculated results are 3.24 fm for ; -\r 12C, 3.11 fm for ; -\r 14N and 3.02 fm\r for ; -\r 16O respectively. It is also found that 3D and 4F states are only pure ; - atomic states\r while the other S and P states are Coulomb-assisted nuclear ; -bound states called hybrid\r states."}]},"item_1583103108160":{"attribute_name":"Keywords","attribute_value_mlt":[{"interim":"hypernucle"}]},"item_1583103120197":{"attribute_name":"Files","attribute_type":"file","attribute_value_mlt":[{"accessrole":"open_access","date":[{"dateType":"Available","dateValue":"2020-05-05"}],"displaytype":"preview","filename":"Structure Analysis of Light.pdf","filesize":[{"value":"398 Kb"}],"format":"application/pdf","licensetype":"license_note","mimetype":"application/pdf","url":{"url":"https://meral.edu.mm/record/838/files/Structure Analysis of Light.pdf"},"version_id":"a7218056-b9de-4466-8e99-ab7edcbe89e3"}]},"item_1583103131163":{"attribute_name":"Journal articles","attribute_value_mlt":[{}]},"item_1583103147082":{"attribute_name":"Conference papaers","attribute_value_mlt":[{}]},"item_1583103211336":{"attribute_name":"Books/reports/chapters","attribute_value_mlt":[{}]},"item_1583103233624":{"attribute_name":"Thesis/dissertations","attribute_value_mlt":[{"subitem_supervisor(s)":[]}]},"item_1583105942107":{"attribute_name":"Authors","attribute_value_mlt":[{"subitem_authors":[{"subitem_authors_fullname":"Phyo Wai Wai Lwin"},{"subitem_authors_fullname":"Aye Aye Min"},{"subitem_authors_fullname":"Khin Swe Myint"}]}]},"item_1583108359239":{"attribute_name":"Upload type","attribute_value_mlt":[{"interim":"Publication"}]},"item_1583108428133":{"attribute_name":"Publication type","attribute_value_mlt":[{"interim":"Journal article"}]},"item_1583159729339":{"attribute_name":"Publication date","attribute_value":"2016"},"item_1583159847033":{"attribute_name":"Identifier","attribute_value":"http://umoar.mu.edu.mm/handle/123456789/98"},"item_title":"Structure Analysis of Light [I] - Hypernuclei","item_type_id":"21","owner":"1","path":["1582967025340"],"publish_date":"2020-03-05","publish_status":"0","recid":"838","relation_version_is_last":true,"title":["Structure Analysis of Light [I] - Hypernuclei"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2021-12-13T07:58:38.135531+00:00"}