{"created":"2020-09-03T07:46:51.207879+00:00","id":5169,"links":{},"metadata":{"_buckets":{"deposit":"807b073a-c2d4-4f07-8366-ed18382be139"},"_deposit":{"created_by":23,"id":"5169","owner":"23","owners":[23],"owners_ext":{"displayname":"","email":"myanila@mu.edu.mm","username":""},"pid":{"revision_id":0,"type":"recid","value":"5169"},"status":"published"},"_oai":{"id":"oai:meral.edu.mm:recid/5169","sets":["1582963739756","1582963739756:1582967025340"]},"communities":["um"],"item_1583103067471":{"attribute_name":"Title","attribute_value_mlt":[{"subitem_1551255647225":"The Influence of the N/Z Ratio of Neutron Richness on the Subbarrier Fusion Dynamics","subitem_1551255648112":"en"}]},"item_1583103085720":{"attribute_name":"Description","attribute_value_mlt":[{"interim":"The isotopic dependence of the interacting potential and fusion cross sections in 53 isotopic reactions A1C+A2Si, A1O+A2Mg, A1O+A2Si, A1Si+A2Si, A1Mg+A2S, A1Si+A2Ni, A1Ca+A2Ca, A1S+A2Ni, A1Ar+A2Ni, A1Ca+A2Ni, A1Ni+A2Ni, A1Ti+A2Ni, A1Ca+A2Ti and A1O+A2Sm with 1  N/Z  1.6 are studied in systematically. An analytical form obtained in the framework of the Extended Thomas-Fermi method is used to calculate the nuclear part of the interacting potential in single barrier passing model. We investigated the relationships between the changes of potential energy and fusion cross section as a function of (N/Z − 1) quantity."}]},"item_1583103108160":{"attribute_name":"Keywords","attribute_value_mlt":[{"interim":"Potential barrier"},{"interim":"barrier position and height"},{"interim":"fusion cross section"}]},"item_1583103120197":{"attribute_name":"Files","attribute_type":"file","attribute_value_mlt":[{"accessrole":"open_access","date":[{"dateType":"Available","dateValue":"2020-09-03"}],"displaytype":"preview","filename":"The Influence of the N.pdf","filesize":[{"value":"193 Kb"}],"format":"application/pdf","licensetype":"license_0","url":{"url":"https://meral.edu.mm/record/5169/files/The Influence of the N.pdf"},"version_id":"e206784c-0501-4479-b7e9-eb5e35787d30"}]},"item_1583103147082":{"attribute_name":"Conference papers","attribute_value_mlt":[{"subitem_acronym":"ICPM","subitem_c_date":"25-27 November 2018","subitem_conference_title":"International Conference on Physics, Mandalay","subitem_place":"University of Mandalay"}]},"item_1583105942107":{"attribute_name":"Authors","attribute_value_mlt":[{"subitem_authors":[{"subitem_authors_fullname":"Kyaw Thiha"},{"subitem_authors_fullname":"Nyein Wink Lwin"}]}]},"item_1583108359239":{"attribute_name":"Upload type","attribute_value_mlt":[{"interim":"Publication"}]},"item_1583108428133":{"attribute_name":"Publication type","attribute_value_mlt":[{"interim":"Conference paper"}]},"item_1583159729339":{"attribute_name":"Publication date","attribute_value":"2018-11-03"},"item_title":"The Influence of the N/Z Ratio of Neutron Richness on the Subbarrier Fusion Dynamics","item_type_id":"21","owner":"23","path":["1582963739756","1582967025340"],"publish_date":"2020-09-03","publish_status":"0","recid":"5169","relation_version_is_last":true,"title":["The Influence of the N/Z Ratio of Neutron Richness on the Subbarrier Fusion Dynamics"],"weko_creator_id":"23","weko_shared_id":-1},"updated":"2021-12-13T03:44:44.733915+00:00"}