Отрывок: (8) When (i) the resonance regime = 0 is implemented and (ii) the fiber has the optimal length z = Lσm (see figure 1)s, where Lxm = 2(2m+ 1)pi Qg + 2Qp , Lym = 2(2m+ 1)pi Qg , (9) W σ2 (0, L σ m) = 1, all the incident energy becomes stored in the generated OV mode with the topological charge opposite to the incident one (see figure 1). |LVσ` 〉 e−iωt −→ |LVσ−`〉 e−iωt . (10) as is seen from Eq. (9). Since Qg/Qp ∼ 2k∆/ncopK and K ∼ It is important to note that t...
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dc.contributor.authorYavorsky, M.A.-
dc.contributor.authorVikulin, D.V.-
dc.contributor.authorAlexeyev, C.N.-
dc.date.accessioned2019-04-24 16:06:51-
dc.date.available2019-04-24 16:06:51-
dc.date.issued2019-
dc.identifierDspace\SGAU\20190424\75937ru
dc.identifier.citationYavorsky M.A. Dynamic polarization-dependent optical-vortex-controlling via a fiber with acousto-optic interaction / M.A. Yavorsky, D.V. Vikulin, C.N. Alexeyev // Сборник трудов ИТНТ-2019 [Текст] : V междунар. конф. и молодеж. шк. "Информ. технологии и нанотехнологии" : 21-24 мая : в 4 т. / Самар. нац.-исслед. ун-т им. С. П. Королева (Самар. ун-т), Ин-т систем. обраб. изобр. РАН-фил. ФНИЦ "Кристаллография и фотоника" РАН ; [под ред. Р. В. Скиданова]. - Самара: Новая техника, 2019. - Т. 1 : Компьютерная оптика и нанофотоника. - 2019. - С. 666-670.ru
dc.identifier.urihttp://repo.ssau.ru/handle/Informacionnye-tehnologii-i-nanotehnologii/Dynamic-polarizationdependent-opticalvortexcontrolling-via-a-fiber-with-acoustooptic-interaction-75937-
dc.description.abstractWe report a new dynamic polarization-dependent mode conversion in a circular optical fiber endowed with the acousto-optic interaction, in which the sign of the topological charge of the generated fiber optical vortex are governed by the linear polarization direction of the incident beam. The described e_ect can be useful in developing new acousto-optic devices such, for example, as polarization-controlled optical vortex intensity modulators. Yet, this type of all-fiber wavelength-tunable optical vortex generation and controlling should be especially useful in such vortex-based applications as micromechanics, classical and quantum information encryption, and simulation of quantum computing.ru
dc.description.sponsorshipThis work was supported by V.I. Vernadsky Crimean Federal University, grant no. VG 01/2017.ru
dc.language.isoenru
dc.publisherИзд-во «Новая техника»ru
dc.titleDynamic polarization-dependent optical-vortex-controlling via a fiber with acousto-optic interactionru
dc.typeArticleru
dc.textpart(8) When (i) the resonance regime = 0 is implemented and (ii) the fiber has the optimal length z = Lσm (see figure 1)s, where Lxm = 2(2m+ 1)pi Qg + 2Qp , Lym = 2(2m+ 1)pi Qg , (9) W σ2 (0, L σ m) = 1, all the incident energy becomes stored in the generated OV mode with the topological charge opposite to the incident one (see figure 1). |LVσ` 〉 e−iωt −→ |LVσ−`〉 e−iωt . (10) as is seen from Eq. (9). Since Qg/Qp ∼ 2k∆/ncopK and K ∼ It is important to note that t...-
Располагается в коллекциях: Информационные технологии и нанотехнологии

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