{"_buckets": {"deposit": "d46ae14e-ff22-4bff-90a1-0db132e64ab6"}, "_deposit": {"id": "832", "owners": [], "pid": {"revision_id": 0, "type": "depid", "value": "832"}, "status": "published"}, "_oai": {"id": "oai:repository.dl.itc.u-tokyo.ac.jp:00000832"}, "item_2_biblio_info_7": {"attribute_name": "\u66f8\u8a8c\u60c5\u5831", "attribute_value_mlt": [{"bibliographicIssueDates": {"bibliographicIssueDate": "2011-09", "bibliographicIssueDateType": "Issued"}, "bibliographicIssueNumber": "9", "bibliographicPageEnd": "34", "bibliographicPageStart": "1", "bibliographicVolumeNumber": "2011", "bibliographic_titles": [{"bibliographic_title": "Journal of high energy physics : JHEP"}]}]}, "item_2_description_5": {"attribute_name": "\u6284\u9332", "attribute_value_mlt": [{"subitem_description": "The orbifold generalization of the partition function, which would describe the gauge theory on the ALE space, is investigated from the combinatorial perspective. It is shown that the root of unity limit q \u2192 exp(2\u03c0i/k) of the q-deformed partition function plays a crucial role in the orbifold projection while the limit q \u2192 1 applies to R4. Then starting from the combinatorial representation of the partition function, a new type of multi-matrix model is derived by considering its asymptotic behavior. It is also shown that Seiberg-Witten curve for the corresponding gauge theory arises from the spectral curve of this multi-matrix model.", "subitem_description_type": "Abstract"}]}, "item_2_publisher_20": {"attribute_name": "\u51fa\u7248\u8005", "attribute_value_mlt": [{"subitem_publisher": "Springer"}]}, "item_2_relation_11": {"attribute_name": "DOI", "attribute_value_mlt": [{"subitem_relation_type_id": {"subitem_relation_type_id_text": "info:doi/10.1007/JHEP09(2011)015", "subitem_relation_type_select": "DOI"}}]}, "item_2_relation_26": {"attribute_name": "\u7570\u7248\u3067\u3042\u308b", "attribute_value_mlt": [{"subitem_relation_type": "isVersionOf", "subitem_relation_type_id": {"subitem_relation_type_id_text": "http://www.springerlink.com/content/k7716n7604368pp0/", "subitem_relation_type_select": "URI"}}, {"subitem_relation_type": "isVersionOf", "subitem_relation_type_id": {"subitem_relation_type_id_text": "http://arxiv.org/abs/1105.6091v2", "subitem_relation_type_select": "URI"}}]}, "item_2_rights_12": {"attribute_name": "\u6a29\u5229", "attribute_value_mlt": [{"subitem_rights": "\u00a9 SISSA 2011. The original publication is available at www.springerlink.com."}]}, "item_2_select_14": {"attribute_name": "\u8457\u8005\u7248\u30d5\u30e9\u30b0", "attribute_value_mlt": [{"subitem_select_item": "author"}]}, "item_2_source_id_10": {"attribute_name": "\u66f8\u8a8c\u30ec\u30b3\u30fc\u30c9ID", "attribute_value_mlt": [{"subitem_source_identifier": "AA1188279X", "subitem_source_identifier_type": "NCID"}]}, "item_2_source_id_8": {"attribute_name": "ISSN", "attribute_value_mlt": [{"subitem_source_identifier": "10298479", "subitem_source_identifier_type": "ISSN"}]}, "item_2_subject_15": {"attribute_name": "\u65e5\u672c\u5341\u9032\u5206\u985e\u6cd5", "attribute_value_mlt": [{"subitem_subject": "421", "subitem_subject_scheme": "NDC"}]}, "item_2_text_34": {"attribute_name": "\u8cc7\u6e90\u30bf\u30a4\u30d7", "attribute_value_mlt": [{"subitem_text_value": "Journal Article"}]}, "item_2_text_4": {"attribute_name": "\u8457\u8005\u6240\u5c5e", "attribute_value_mlt": [{"subitem_text_value": "Department of Basic Science, University of Tokyo"}, {"subitem_text_value": "Mathematical Physics Lab., RIKEN Nishina Center"}]}, "item_creator": {"attribute_name": "\u8457\u8005", "attribute_type": "creator", "attribute_value_mlt": [{"creatorNames": [{"creatorName": "Kimura, Taro"}], "nameIdentifiers": [{"nameIdentifier": "3212", "nameIdentifierScheme": "WEKO"}]}]}, "item_files": {"attribute_name": "\u30d5\u30a1\u30a4\u30eb\u60c5\u5831", "attribute_type": "file", "attribute_value_mlt": [{"accessrole": "open_date", "date": [{"dateType": "Available", "dateValue": "2017-05-30"}], "displaytype": "detail", "download_preview_message": "", "file_order": 0, "filename": "Kimura_JHEP09_2011_015.pdf", "filesize": [{"value": "414.5 kB"}], "format": "application/pdf", "future_date_message": "", "is_thumbnail": false, "licensetype": "license_free", "mimetype": "application/pdf", "size": 414500.0, "url": {"label": "Kimura_JHEP09_2011_015.pdf", "url": "https://repository.dl.itc.u-tokyo.ac.jp/record/832/files/Kimura_JHEP09_2011_015.pdf"}, "version_id": "e4b69854-d2fe-42a8-bb4d-ab961b74ff4f"}]}, "item_keyword": {"attribute_name": "\u30ad\u30fc\u30ef\u30fc\u30c9", "attribute_value_mlt": [{"subitem_subject": "Supersymmetric gauge theory", "subitem_subject_scheme": "Other"}, {"subitem_subject": "Matrix Models", "subitem_subject_scheme": "Other"}, {"subitem_subject": "M(atrix) Theories", "subitem_subject_scheme": "Other"}]}, "item_language": {"attribute_name": "\u8a00\u8a9e", "attribute_value_mlt": [{"subitem_language": "eng"}]}, "item_resource_type": {"attribute_name": "\u8cc7\u6e90\u30bf\u30a4\u30d7", "attribute_value_mlt": [{"resourcetype": "journal article", "resourceuri": "http://purl.org/coar/resource_type/c_6501"}]}, "item_title": "Matrix model from N = 2 orbifold partition function", "item_titles": {"attribute_name": "\u30bf\u30a4\u30c8\u30eb", "attribute_value_mlt": [{"subitem_title": "Matrix model from N = 2 orbifold partition function"}]}, "item_type_id": "2", "owner": "1", "path": ["9/10/11", "43/65/66"], "permalink_uri": "http://hdl.handle.net/2261/50583", "pubdate": {"attribute_name": "\u516c\u958b\u65e5", "attribute_value": "2017-01-06"}, "publish_date": "2017-01-06", "publish_status": "0", "recid": "832", "relation": {}, "relation_version_is_last": true, "title": ["Matrix model from N = 2 orbifold partition function"], "weko_shared_id": null}