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dc.contributor.authorLai, Sheng-Hongen_US
dc.contributor.authorLee, Jen-Chien_US
dc.contributor.authorTsai, I-Hsunen_US
dc.date.accessioned2018-08-21T05:54:31Z-
dc.date.available2018-08-21T05:54:31Z-
dc.date.issued2017-02-01en_US
dc.identifier.issn0003-4916en_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.aop.2016.10.012en_US
dc.identifier.urihttp://hdl.handle.net/11536/146072-
dc.description.abstractThe SL(2, C) Yang-Mills instanton solutions constructed recently by the biquaternion method were shown to satisfy the complex version of the ADHM equations and the monad construction. Moreover, we discover that, in addition to the holomorphic vector bundles on CP3 similar to the case of SU(2) ADHM construction, the SL(2, C) instanton solutions can be used to explicitly construct instanton sheaves on CP3. Presumably, the existence of these instanton sheaves is related to the singularities of the SL(2, C) instantons on S-4 which do not exist for SU(2) instantons. (C) 2016 Elsevier Inc. All rights reserved.en_US
dc.language.isoen_USen_US
dc.subjectInstanton sheavesen_US
dc.subjectMonad constructionen_US
dc.subjectSingularities of gauge fieldsen_US
dc.subjectSL(2, C) Yang-Mills instantonen_US
dc.subjectBiquaternion ADHM constructionen_US
dc.titleYang-Mills instanton sheavesen_US
dc.typeArticleen_US
dc.identifier.doi10.1016/j.aop.2016.10.012en_US
dc.identifier.journalANNALS OF PHYSICSen_US
dc.citation.volume377en_US
dc.citation.spage446en_US
dc.citation.epage465en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000394197800028en_US
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