{"_buckets": {"deposit": "25c43c36-3c1b-439b-93f3-af353b4fbc67"}, "_deposit": {"created_by": 155, "id": "7088", "owner": "155", "owners": [155], "owners_ext": {"displayname": "", "username": ""}, "pid": {"revision_id": 0, "type": "depid", "value": "7088"}, "status": "published"}, "_oai": {"id": "oai:meral.edu.mm:recid/00007088", "sets": ["user-mmu"]}, "communities": ["mmu"], "item_1583103067471": {"attribute_name": "Title", "attribute_value_mlt": [{"subitem_1551255647225": "The Most Unstable Conditions of Modulation Instability", "subitem_1551255648112": "en"}]}, "item_1583103085720": {"attribute_name": "Description", "attribute_value_mlt": [{"interim": "Modulation instability is one of the most ubiquitous types of instabilities in nature. As one of the\nkey characteristics of modulation instability, the most unstable condition attracts lots of attention.\nThe most unstable condition is investigated here with two kinds of initial wave systems via a\nnumerical high-order spectral method HOS for surface water wave field. Classically, one carrier\nwave and a pair of sidebands are implied as the first kind of initial wave system: “seeded” wave\nsystem. In the second kind of initialwave system: “un-seeded”wave system, only one carrier wave\nis implied. Two impressive new results are present. One result shows that the grow rates of lower\nand upper sideband are differentwithin the “seeded”wave system. Itmeans that, for a given wave\nsteepness, the most unstable lower sideband is not in pair with the most unstable upper sideband.\nAnother result shows the fastest growing sidebands are exactly in pair from “unseeded” wave\nsystem. And the most unstable conditions of “unseeded” wave system are more or less the mean\nvalue of those derived from the lower sidebands and upper sidebands within the “seeded” wave\nsystem.\n1."}]}, "item_1583103108160": {"attribute_name": "Keywords", "attribute_value_mlt": [{"interim": "Modulation instability"}, {"interim": "most unstable condition"}, {"interim": "high-order spectral method"}, {"interim": "fastest-growing-sidebands"}]}, "item_1583103120197": {"attribute_name": "Files", "attribute_type": "file", "attribute_value_mlt": [{"accessrole": "open_access", "date": [{"dateType": "Available", "dateValue": "2020-12-29"}], "displaytype": "preview", "download_preview_message": "", "file_order": 0, "filename": "Mee Mee Soe.pdf", "filesize": [{"value": "2.3 MB"}], "format": "application/pdf", "future_date_message": "", "is_thumbnail": false, "licensetype": "license_0", "mimetype": "application/pdf", "size": 2300000.0, "url": {"url": "https://meral.edu.mm/record/7088/files/Mee Mee Soe.pdf"}, "version_id": "3a66c090-c8c6-4f6d-b892-cbf937f74cb8"}]}, "item_1583103131163": {"attribute_name": "Journal articles", "attribute_value_mlt": [{"subitem_issue": "Hindawi Publishing Corporation", "subitem_journal_title": "Journal of Applied Mathematics", "subitem_pages": "11", "subitem_volume": "2012, Article ID 656873"}]}, "item_1583105942107": {"attribute_name": "Authors", "attribute_value_mlt": [{"subitem_authors": [{"subitem_authors_fullname": "Mee Mee Soe"}]}]}, "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": "2012-03-26"}, "item_1583159847033": {"attribute_name": "Identifier", "attribute_value": "doi:10.1155/2012/656873"}, "item_title": "The Most Unstable Conditions of Modulation Instability", "item_type_id": "21", "owner": "155", "path": ["1608152118915"], "permalink_uri": "http://hdl.handle.net/20.500.12678/0000007088", "pubdate": {"attribute_name": "Deposited date", "attribute_value": "2020-12-29"}, "publish_date": "2020-12-29", "publish_status": "0", "recid": "7088", "relation": {}, "relation_version_is_last": true, "title": ["The Most Unstable Conditions of Modulation Instability"], "weko_shared_id": -1}