Spin-polarization array generation for spin transport use

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dc.contributor.authorS. Mitatha
dc.contributor.authorW. Sangiamsak
dc.contributor.authorK. Kulsirirat
dc.contributor.authorC. Teeka
dc.contributor.authorP.P. Yupapin
dc.date.accessioned2025-03-10T07:37:41Z
dc.date.available2025-03-10T07:37:41Z
dc.date.issued2011
dc.description.abstractSpin-polarization can be formed by the two components of soliton (electromagnetic wave) within the metallic waveguide. Under the resonant condition, the random transverse electric and magnetic fields of the solitons corresponding to the left-hand and right hand photons can be generated. Whenever a photon is absorbed by an object, an angular momentum of either +_ or -_ is imparted to the object, in which two possible spin states known as optoelectronic spins are exhibited. Furthermore, the array of optoelectronic spins, i.e., many particles can be generated and controlled by using the modified add-drop filter, in which the broad spectrum soliton can be generated and used to form large scale spin transport applications. © 2011 World Scientific Publishing Company.
dc.identifier.citationJournal of Nonlinear Optical Physics and Materials
dc.identifier.doi10.1142/S0218863511006169
dc.identifier.issn2188635
dc.identifier.scopus2-s2.0-84857518305
dc.identifier.urihttps://repository.dusit.ac.th//handle/123456789/5033
dc.languageEnglish
dc.rights.holderScopus
dc.subjectdark-bright soliton
dc.subjectorthogonal soliton
dc.subjectspin polarization
dc.subjectSpin transport
dc.subjectspintronics
dc.titleSpin-polarization array generation for spin transport use
dc.typeArticle
mods.location.urlhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-84857518305&doi=10.1142%2fS0218863511006169&partnerID=40&md5=bc68e38d36b442b65b876ffb4eb273d1
oaire.citation.endPage387
oaire.citation.issue3
oaire.citation.startPage379
oaire.citation.volume20
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