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Displaced Harmonic Oscillator V ∼ min [(x + d)2, (x − d)2] as a Benchmark Double-Well Quantum Model

dc.contributor.authorZnojil, Miloslav
dc.date.accessioned2025-12-05T14:01:24Z
dc.date.available2025-12-05T14:01:24Z
dc.date.issued2022
dc.description.abstractFor the displaced harmonic double-well oscillator, the existence of exact polynomial bound states at certain displacements (Formula presented.) is revealed. The N-plets of these quasi-exactly solvable (QES) states are constructed in closed form. For non-QES states, the Schrödinger equation can still be considered “non-polynomially exactly solvable” (NES) because the exact left and right parts of the wave function (proportional to confluent hypergeometric function) just have to be matched in the origin. © 2022 by the author.eng
dc.formatp. 309-323
dc.identifier.doi10.3390/quantum4030022
dc.identifier.issn2624-960X
dc.identifier.obd43880788
dc.identifier.urihttp://hdl.handle.net/20.500.12603/2013
dc.language.isoeng
dc.peerreviewedyes
dc.publicationstatuspostprint
dc.publisherMDPI
dc.relation.ispartofQuantum Reports, volume 4, issue: 3eng
dc.relation.publisherversionhttps://www.mdpi.com/2624-960X/4/3/22
dc.rights.accessOpen Access
dc.rights.licenseCC BY
dc.source.urlhttps://www.mdpi.com/2624-960X/4/3/22
dc.subjectdisplaced harmonic oscillatorseng
dc.subjectdouble-well–single-well transitioneng
dc.subjectmatching-method solutionseng
dc.subjectquasi-exact and non-polynomial exact bound stateseng
dc.titleDisplaced Harmonic Oscillator V ∼ min [(x + d)2, (x − d)2] as a Benchmark Double-Well Quantum Modeleng
dc.typearticle

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