{"_buckets": {"deposit": "f3f06015-d2e7-44ff-ae72-313723f1d9a4"}, "_deposit": {"created_by": 23, "id": "5146", "owner": "23", "owners": [23], "owners_ext": {"displayname": "", "username": ""}, "pid": {"revision_id": 0, "type": "recid", "value": "5146"}, "status": "published"}, "_oai": {"id": "oai:meral.edu.mm:recid/5146", "sets": ["1582963739756", "1582967025340", "user-um"]}, "communities": ["um"], "item_1583103067471": {"attribute_name": "Title", "attribute_value_mlt": [{"subitem_1551255647225": "Effects of Different Potential Models for the 16O+144,154Sm Fusion Reactions", "subitem_1551255648112": "en"}]}, "item_1583103085720": {"attribute_name": "Description", "attribute_value_mlt": [{"interim": "Fusion cross sections are evaluated by numerically solving the Schr dinger equation within the following potentials under the incoming wave boundary conditions. Four versions of proximity potentials, three versions of Woods-Saxon parameterizations and a simple analytical fusion potential from the mean field description are employed. The fusion barrier heights and positions are also evaluated for asymmetry colliding systems. Coupled-channels calculations are also performed for 16O+144,154Sm systems. It is found that Prox 10, all versions of Woods-Saxon potentials and mean field potentials can reproduce the experimental barrier heights and barrier positions within ±5% for most of the colliding systems. The percentage deviations for other potentials vary up to ±14%. We can say that the largest deviation is found for the system, 40Ca+124Sn with largest charge product for most of the potentials. The comparison of fusion cross sections reveals that mean field potential reproduces the experimental data better than other potentials at energies above and below the Coulomb barrier."}]}, "item_1583103108160": {"attribute_name": "Keywords", "attribute_value_mlt": [{"interim": "Fusion cross section"}, {"interim": "nuclear potential"}, {"interim": "coulomb potential"}]}, "item_1583103120197": {"attribute_name": "Files", "attribute_type": "file", "attribute_value_mlt": [{"accessrole": "open_access", "date": [{"dateType": "Available", "dateValue": "2020-09-02"}], "displaytype": "preview", "download_preview_message": "", "file_order": 0, "filename": "Effects of Different Potential Models for the 16O+144,154Sm Fusion Reactions.pdf", "filesize": [{"value": "543 Kb"}], "format": "application/pdf", "future_date_message": "", "is_thumbnail": false, "licensetype": "license_0", "mimetype": "application/pdf", "size": 543000.0, "url": {"url": "https://meral.edu.mm/record/5146/files/Effects of Different Potential Models for the 16O+144,154Sm Fusion Reactions.pdf"}, "version_id": "d7240f07-d61d-47e0-a52b-e8f65c5c1ee8"}]}, "item_1583103131163": {"attribute_name": "Journal articles", "attribute_value_mlt": [{"subitem_issue": "1", "subitem_journal_title": "Universities Research Journal", "subitem_pages": "257-268", "subitem_volume": "5"}]}, "item_1583105942107": {"attribute_name": "Authors", "attribute_value_mlt": [{"subitem_authors": [{"subitem_authors_fullname": "Kyaw Thiha"}, {"subitem_authors_fullname": "Nyein Wint Lwin"}]}]}, "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": "2012-12-02"}, "item_title": "Effects of Different Potential Models for the 16O+144,154Sm Fusion Reactions", "item_type_id": "21", "owner": "23", "path": ["1582963739756", "1582967025340"], "permalink_uri": "http://hdl.handle.net/20.500.12678/0000005146", "pubdate": {"attribute_name": "Deposited date", "attribute_value": "2020-09-02"}, "publish_date": "2020-09-02", "publish_status": "0", "recid": "5146", "relation": {}, "relation_version_is_last": true, "title": ["Effects of Different Potential Models for the 16O+144,154Sm Fusion Reactions"], "weko_shared_id": -1}