完整後設資料紀錄
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dc.contributor.authorLai, Sheng-Hongen_US
dc.contributor.authorLee, Jen-Chien_US
dc.contributor.authorTsai, I-Hsunen_US
dc.date.accessioned2015-12-02T02:59:23Z-
dc.date.available2015-12-02T02:59:23Z-
dc.date.issued2015-10-01en_US
dc.identifier.issn0003-4916en_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.aop.2015.06.005en_US
dc.identifier.urihttp://hdl.handle.net/11536/128127-
dc.description.abstractWe extend quaternion calculation in the ADHM construction of Sp(1) (=SU(2)) self-dual Yang-Mills (SDYM) instantons to the case of biquaternion. We use the biconjugate operation of biquaternion first introduced by Hamilton to construct the non-compact SL(2, C) k-instantons. The number of parameters of this construction for SL(2, C) k-instantons is found to be twice of that of Sp(1), 16k-6. These new SL(2, C) instanton solutions contain the SL(2, C) (M, N) instanton solutions constructed previously as a subset. The structures of singularities or jumping lines of the complete SL(2, C) k = 1, 2, 3 instantons with 10, 26, 42 moduli parameters are particularly investigated. The existence of singular structures of the SL(2, C) k-instantons is mathematically consistent with recent results of solutions of complex ADHM equations. It may also help to clarify the long standing global singularity problems associated with Backlund transformations of SU(2) instantons. (C) 2015 Elsevier Inc. All rights reserved.en_US
dc.language.isoen_USen_US
dc.subjectBiquaternionsen_US
dc.subjectNon-compact ADHM instantonsen_US
dc.subjectJumping linesen_US
dc.titleBiquaternions and ADHM construction of non-compact SL(2, C) Yang-Mills instantonsen_US
dc.typeArticleen_US
dc.identifier.doi10.1016/j.aop.2015.06.005en_US
dc.identifier.journalANNALS OF PHYSICSen_US
dc.citation.volume361en_US
dc.citation.spage14en_US
dc.citation.epage32en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000360418800002en_US
dc.citation.woscount0en_US
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