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Please use this identifier to cite or link to this item: https://digital.lib.ueh.edu.vn/handle/UEH/60080
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dc.contributor.authorT. D. Doen_US
dc.contributor.otherN. N. Trongen_US
dc.contributor.otherL. X. Truongen_US
dc.date.accessioned2020-05-04T08:27:34Z-
dc.date.available2020-05-04T08:27:34Z-
dc.date.issued2020-
dc.identifier.issn0133-3852 (Print), 1588-273X (Online)-
dc.identifier.urihttp://digital.lib.ueh.edu.vn/handle/UEH/60080-
dc.description.abstractLet d ∈ {3, 4, 5,...} and p ∈ (0, 1]. We consider the Hermite operator L = −Δ + |x|2 on its maximal domain in L2(ℝd). Let HpL(Rd) be the completion of {f∈L2(Rd):MLf∈Lp(Rd)} with respect to the quasi-norm ∥⋅∥HpL=∥ML⋅∥Lp, where MLf(⋅)=supt>0∣∣e−tLf(⋅)∣∣ for all f ∈ L2(ℝd). We characterise HpL(Rd) in terms of Lusin integrals associated with the Hermite operator for p∈(dd+1,1].en_US
dc.formatPortable Document Format (PDF)en_US
dc.language.isoenen_US
dc.publisherAkadémiai Kiadóen_US
dc.relation.ispartofAnalysis Mathematicaen_US
dc.relation.ispartofseriesVol. 46, Issue 1en_US
dc.rightsSpringeren_US
dc.subjectHermite operatoren_US
dc.subjectHardy spaceen_US
dc.subjectLusin integralen_US
dc.subjectAtom decompositionen_US
dc.subjectHeat kernelen_US
dc.titleLusin characterisation of hardy spaces associated with hermite operatorsen_US
dc.typeJournal Articleen_US
dc.identifier.doihttps://doi.org/10.1007/s10476-020-0016-z-
dc.format.firstpage47en_US
dc.format.lastpage66en_US
ueh.JournalRankingISI, Scopusen_US
item.languageiso639-1en-
item.cerifentitytypePublications-
item.grantfulltextnone-
item.openairetypeJournal Article-
item.fulltextOnly abstracts-
item.openairecristypehttp://purl.org/coar/resource_type/c_18cf-
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