danДоклады Национальной академии наук БеларусиDoklady of the National Academy of Sciences of Belarus1561-83232524-2431The Republican Unitary Enterprise Publishing House "Belaruskaya Navuka"10.29235/1561-8323-2024-68-4-288-295dan-1202Research ArticleФИЗИКАPHYSICSОптические нанотрансиверы в фотоникеOptical nanotransceivers in photonicsГапоненкоС. В.GaponenkoS. V.

Гапоненко Сергей Васильевич – академик, д-р физ.-мат. наук, директор

пр. Независимости, 68, 220072, Минск

Gaponenko Sergey V. – Academician, D. Sc. (Physics and Mathematics), Director

68, Nezavisimosti Ave., 220072, Minsk

s.gaponenko@ifanbel.bas-net.byЕфимоваТ. А.EfimovaT. A.

Ефимова Таисия Адамовна – аспирант, мл. науч. сотрудник

пр. Независимости, 68, 220072, Минск

Efimova Taisia A. – Postgraduate Student, Junior Researcher

68, Nezavisimosti Ave., 220072, Minsk

t.efimova@ifanbel.bas-net.byИнститут физики им. Б. И. Степанова НАН БеларусиB. I. Stepanov Institute of Physics of the National Academy of Sciences of Belarus202405092024684288295Copyright © Гапоненко С.В., Ефимова Т.А., 20242024Гапоненко С.В., Ефимова Т.А.Gaponenko S.V., Efimova T.A.Данная работа распространяется под лицензией Creative Commons Attribution 4.0.This work is licensed under a Creative Commons Attribution 4.0 License.https://doklady.belnauka.by/jour/article/view/1202

Используемая в нанофотонике аналогия с радиофизикой, на основе которой введено и плодотворно используется понятие оптической наноантенны, обобщается на случай двухступенчатых процессов с оптическим возбуждением квантового излучателя (рассеивателя) и последующим испусканием вторичных фотонов: вводится понятие «оптический нанотрансивер» (приемопередатчик), т. е. устройство, принимающее первичные и генерирующее вторичные фотоны. Введен параметр эффективности нанотрансивера, задаваемый произведением коэффициента усиления интенсивности первичного излучения на локальную плотность фотонных состояний на частоте вторичного излучения. Данный параметр нанотрансивера задает повышение интенсивности рассеянного излучения и максимально возможное значение повышения интенсивности фотолюминесценции. Последнее достигается для излучателей с низким собственным квантовым выходом.

The analogy used in nanophotonics with radiophysics, on the basis of which the notion of an optical nanoantenna was introduced and fruitfully used, is extended to the case of two-step processes with optical excitation of a quantum emitter (scatterer) and subsequent emission of secondary photons and the concept of an “optical nanotransceiver” (transceiver), i. e. a device receiving primary and generating secondary photons is introduced. The nanotransceiver efficiency parameter is introduced, which is defined by the product of the primary radiation intensity factor and the local density of photonic states at the secondary radiation frequency. This nanotransceiver parameter determines scattered radiation intensity enhancement and a maximum possible value of photoluminescence enhancement. The latter is achieved for emitters with low intrinsic quantum yield.

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The authors declare that there are no conflicts of interest present.