Please use this identifier to cite or link to this item: http://dspace.iitrpr.ac.in:8080/xmlui/handle/123456789/3792
Full metadata record
DC FieldValueLanguage
dc.contributor.authorBanger, P.-
dc.contributor.authorKaur, P.-
dc.contributor.authorGautam, S.-
dc.date.accessioned2022-07-29T07:32:21Z-
dc.date.available2022-07-29T07:32:21Z-
dc.date.issued2022-07-29-
dc.identifier.urihttp://localhost:8080/xmlui/handle/123456789/3792-
dc.description.abstractWe develop time-splitting finite-difference methods, using an implicit Backward–Euler and a semi-implicit Crank–Nicolson discretization schemes, to study the spin-orbit-coupled (SO-coupled) spinor Bose–Einstein condensates with coherent coupling in quasi-one- and quasi-two-dimensional traps. The split equations involving kinetic energy and spin-orbit-coupling operators are solved using either a time implicit Backward–Euler or a semi-implicit Crank–Nicolson method. We explicitly develop the methods for pseudospin-1/2, spin-1 and spin-2 condensates. The results for ground states obtained with time-splitting Backward–Euler and Crank–Nicolson methods are in excellent agreement with time-splitting Fourier spectral method, which is one of the popular methods to solve the mean-field models for SO-coupled spinor condensates. We confirm the emergence of different phases in SO-coupled pseudospin-1/2, spin-1 and spin-2 condensates with coherent coupling.en_US
dc.language.isoen_USen_US
dc.subjectSpinor BECen_US
dc.subjectCoherent couplingen_US
dc.subjectSpin-orbit couplingen_US
dc.subjectSemi-implicit methodsen_US
dc.titleSemi-implicit finite-difference methods to study the spin-orbit- and coherently-coupled spinor Bose-Einstein condensatesen_US
dc.typeArticleen_US
Appears in Collections:Year-2022

Files in This Item:
File Description SizeFormat 
Full Text.pdf2.71 MBAdobe PDFView/Open    Request a copy


Items in DSpace are protected by copyright, with all rights reserved, unless otherwise indicated.