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HARMONIC WEAK MAASS FORMS AND PERIOD FUNCTIONS

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dc.contributor.author최소영-
dc.date.accessioned2025-12-22T09:00:18Z-
dc.date.available2025-12-22T09:00:18Z-
dc.date.issued2025-11-
dc.identifier.issn1226-3524-
dc.identifier.issn2383-6245-
dc.identifier.urihttps://scholarworks.gnu.ac.kr/handle/sw.gnu/81430-
dc.description.abstractThere are two fundamental differential operators in the theory of harmonic Maass forms. Let N = 2 or 3. Extending results of Bringmann et al. and those of Choi and Kim, we show that the images of a harmonic weak Maass form on Γ0 (N ) under these two operators are intricately related through their period functions-
dc.format.extent7-
dc.language영어-
dc.language.isoENG-
dc.publisher충청수학회-
dc.titleHARMONIC WEAK MAASS FORMS AND PERIOD FUNCTIONS-
dc.typeArticle-
dc.publisher.location대한민국-
dc.identifier.bibliographicCitation충청수학회지, v.38, no.4, pp 281 - 287-
dc.citation.title충청수학회지-
dc.citation.volume38-
dc.citation.number4-
dc.citation.startPage281-
dc.citation.endPage287-
dc.type.docTypeY-
dc.identifier.kciidART003269871-
dc.description.isOpenAccessN-
dc.description.journalRegisteredClasskci-
dc.subject.keywordAuthorPeriod function-
dc.subject.keywordAuthorHarmonic Maass form-
dc.subject.keywordAuthorDifferential operator.-
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