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ФИЗИКА ЭЛЕМЕНТАРНЫХ ЧАСТИЦ И АТОМНОГО ЯДРА

Оптоэлектронный транзисторный эффект в полярной квантовой системе, возбуждаемой трихроматическим полем: Аннотации

Bogolyubov, Jr., N. N., Andrey Vladimirovich Soldatov, Н. Н. Боголюбов (мл.)

Published May 31, 2024• 0 citations
OpenAlex

Abstract

The fluorescent radiative properties of a two-level quantum polar system with broken spatial inversion symmetry being realized as a model of a single-electron two-level “atom” with permanent atomic electric dipole moment, so that its electric dipole operator diagonal matrix elements are not equal to each other, were examined. In practice, such a system can be realized as an asymmetric quantum dot. A particular case when this system is driven by a trichromatic external field, with two high-frequency bichromatic field components of equal Rabi frequencies and carrier frequencies being placed symmetrically around the atomic transition frequency, and one more low-frequency component being in resonance with the Rabi frequency of the high-frequency components, was analyzed. It was shown that the high-frequency spectral properties of the fluorescent radiation can be altered with equal efficiency either by controlling the intensity of the low-frequency component of the trichromatic driving field or by changing the degree of the quantum dot asymmetry. Possible options to apply this potentially use

Related papers

Optoelectronic Transistor Effect in a Polar Quantum System Driven by a Trichromatic Field

N. N. Bogolyubov, Andrey Vladimirovich Soldatov

Abstract The fluorescent radiative properties of a two-level quantum polar system with broken spatial inversion symmetry being realized as a model of a single-electron two-level “atom” with permanent atomic electric dipole moment, so that its electric dipole operator diagonal matrix elements are not equal to each other, were examined. In practice, such a system can be realized as an asymmetric quantum dot. A particular case when this system is driven by a trichromatic external field, with two high-frequency bichromatic field components of equal Rabi frequencies and carrier frequencies being placed symmetrically around the atomic transition frequency, and one more low-frequency component being in resonance with the Rabi frequency of the high-frequency components, was analyzed. It was shown that the high-frequency spectral properties of the fluorescent radiation can be altered with equal efficiency either by controlling the intensity of the low-frequency component of the trichromatic driving field or by changing the degree of the quantum dot asymmetry. Possible options to apply this potentially useful effect for practical purposes in the field of optoelectronics are also discussed.

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Fluorescence by a polar quantum system in a polychromatic field

Jr. Bogolyubov, Andrey Vladimirovich Soldatov

Spectral properties of fluorescent radiation from a two-level quantum system with broken inversion spatial symmetry, which can be described by a model of an one-electron two-level atom whose electric dipole moment operator has permanent unequal diagonal matrix elements, were studied. The case of the excitation of this system by a polychromatic laser field, comprised of $N-1$ high-frequency components with the frequencies close to or being in resonance with the atomic transition frequency, and a low-frequency component whose frequency coincides with the Rabi frequency of the high-frequency components, was considered. Special attention was given to the resonant bichromatic and nearly resonant trichromatic excitation. In the former case it was shown that by changing the intensity of the low-frequency component, one can efficiently alter spectral properties of the fluorescent radiation of the system in the high-frequency range, while in the latter case it was found that the fluorescent behavior of the system in question reveals a kind of an optoelectronic transistor effect. Options for the experimental detection and practical usage of the effects under study were discussed.

arXiv:2412.11243•Dec 15, 2024•0 citations

Флуоресценция некогерентно возбуждаемой полярной квантовой системы, находящейся под воздействием сильного нерезонансного внешнего поля: Аннотации

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ФИЗИКА ЭЛЕМЕНТАРНЫХ ЧАСТИЦ И АТОМНОГО ЯДРА•Mar 24, 2026•0 citations

Resonance fluorescence of polar quantum systems in a bichromatic field

Nikolai Nikolaevich Bogoliubov, Andrey Vladimirovich Soldatov

We study spectral properties of fluorescent radiation from a two-level quantum system with broken inversion spatial symmetry, which can be implemented as a model of a one-electron two-level atom whose electric dipole moment operator has permanent unequal diagonal matrix elements. We consider the case of the excitation of this system by a bichromatic laser field consisting of a high-frequency resonance component with the frequency coinciding with the atomic transition frequency and a low-frequency component whose frequency coincides with the Rabi frequency of the high-frequency component. We show that by changing the intensity of the low-frequency component, we can efficiently control spectral properties of the fluorescent radiation of the system in the high-frequency range. We discuss possible methods for the experimental detection and practical use of the effects under study.

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Abstract We studied spectral properties of high-frequency fluorescent radiation from a two-level quantum system with broken inversion spatial symmetry, which can be implemented as a model of a one-electron two-level asymmetric polar semiconductor quantum dot whose electric dipole moment operator has permanent unequal diagonal matrix elements. The case of the excitation of this system by incoherent pumping of some sort supplemented with an additional driving monochromatic field, which frequency is much lower than the optical transition frequency of the quantum dot, was considered. An analytical expression for the fluorescence spectrum as a function of the amplitude and frequency of the monochromatic driving field, as well as of the pumping intensity, was derived. We also discussed feasible practical applications of the effects under study in the field of quantum optics and optoelectronics for the generation of high-frequency radiation, possessing stationary equidistant spectrum, and for the control of the radiative properties of such nanodevices as spasers (dipole nanolasers).

Laser Physics Letters•Oct 29, 2024•0 citations

Time-dependent fluorescence by incoherently pumped polar quantum dot driven by a low-frequency monochromatic field

Andrey Vladimirovich Soldatov

We studied time-dependent features of high-frequency fluorescent radiation from a two-level quantum system with broken inversion spatial symmetry. The system in question was modelled after a one-electron two-level asymmetric polar semiconductor quantum dot whose electric dipole moment operator has permanent unequal diagonal matrix elements. The dot was permanently excited by incoherent pumping of some sort. Our attention was focused on the evolution of the fluorescence spectrum following abrupt switching on of an additional driving monochromatic field, which frequency is much lower than the optical transition frequency of the quantum dot. An analytical expression for the fluorescence spectrum as a function of the amplitude, initial phase and frequency of the monochromatic driving field, as well as of the pumping intensity and the elapsed time, was derived.

arXiv:2412.11249•Dec 15, 2024•0 citations
The fluorescent radiative properties of a two-level quantum polar system with broken spatial inversion symmetry being realized as a model of a single-electron two-level “atom” with permanent atomic electric dipole moment, so that its electric dipole operator diagonal matrix elements are not equal to each other, were examined. In practice, such a system can be realized as an asymmetric quantum dot. A particular case when this system is driven by a trichromatic external field, with two high-frequency bichromatic field components of equal Rabi frequencies and carrier frequencies being placed symmetrically around the atomic transition frequency, and one more low-frequency component being in resonance with the Rabi frequency of the high-frequency components, was analyzed. It was shown that the high-frequency spectral properties of the fluorescent radiation can be altered with equal efficiency either by controlling the intensity of the low-frequency component of the trichromatic driving field or by changing the degree of the quantum dot asymmetry. Possible options to apply this potentially use
Abstract The fluorescent radiative properties of a two-level quantum polar system with broken spatial inversion symmetry being realized as a model of a single-electron two-level “atom” with permanent atomic electric dipole moment, so that its electric dipole operator diagonal matrix elements are not equal to each other, were examined. In practice, such a system can be realized as an asymmetric quantum dot. A particular case when this system is driven by a trichromatic external field, with two high-frequency bichromatic field components of equal Rabi frequencies and carrier frequencies being placed symmetrically around the atomic transition frequency, and one more low-frequency component being in resonance with the Rabi frequency of the high-frequency components, was analyzed. It was shown that the high-frequency spectral properties of the fluorescent radiation can be altered with equal efficiency either by controlling the intensity of the low-frequency component of the trichromatic driving field or by changing the degree of the quantum dot asymmetry. Possible options to apply this potentially useful effect for practical purposes in the field of optoelectronics are also discussed.
Spectral properties of fluorescent radiation from a two-level quantum system with broken inversion spatial symmetry, which can be described by a model of an one-electron two-level atom whose electric dipole moment operator has permanent unequal diagonal matrix elements, were studied. The case of the excitation of this system by a polychromatic laser field, comprised of N−1N-1N−1 high-frequency components with the frequencies close to or being in resonance with the atomic transition frequency, and a low-frequency component whose frequency coincides with the Rabi frequency of the high-frequency components, was considered. Special attention was given to the resonant bichromatic and nearly resonant trichromatic excitation. In the former case it was shown that by changing the intensity of the low-frequency component, one can efficiently alter spectral properties of the fluorescent radiation of the system in the high-frequency range, while in the latter case it was found that the fluorescent behavior of the system in question reveals a kind of an optoelectronic transistor effect. Options for the experimental detection and practical usage of the effects under study were discussed.
High-frequency fluorescent radiation by incoherently pumped polar two-level quantum system possessing permanent electric dipole moments and simultaneously interacting with external low-frequency field and dissipative environment of some kind was studied. The system in question may be represented by a one-electron two-level asymmetric polar semiconductor quantum dot characterized by the electric dipole moment operator with unequal diagonal matrix elements in its ground and excited quantum states. An analytical expression for the steady-state fluorescence spectrum as a function of the amplitude, initial phase and carrier frequency of the driving field, as well as of the pumping intensity, was derived. It was shown that in the case of strong external field an interaction with the environment is modified, which alters in its turn the fluorescence spectrum.
We study spectral properties of fluorescent radiation from a two-level quantum system with broken inversion spatial symmetry, which can be implemented as a model of a one-electron two-level atom whose electric dipole moment operator has permanent unequal diagonal matrix elements. We consider the case of the excitation of this system by a bichromatic laser field consisting of a high-frequency resonance component with the frequency coinciding with the atomic transition frequency and a low-frequency component whose frequency coincides with the Rabi frequency of the high-frequency component. We show that by changing the intensity of the low-frequency component, we can efficiently control spectral properties of the fluorescent radiation of the system in the high-frequency range. We discuss possible methods for the experimental detection and practical use of the effects under study.
Abstract We studied spectral properties of high-frequency fluorescent radiation from a two-level quantum system with broken inversion spatial symmetry, which can be implemented as a model of a one-electron two-level asymmetric polar semiconductor quantum dot whose electric dipole moment operator has permanent unequal diagonal matrix elements. The case of the excitation of this system by incoherent pumping of some sort supplemented with an additional driving monochromatic field, which frequency is much lower than the optical transition frequency of the quantum dot, was considered. An analytical expression for the fluorescence spectrum as a function of the amplitude and frequency of the monochromatic driving field, as well as of the pumping intensity, was derived. We also discussed feasible practical applications of the effects under study in the field of quantum optics and optoelectronics for the generation of high-frequency radiation, possessing stationary equidistant spectrum, and for the control of the radiative properties of such nanodevices as spasers (dipole nanolasers).
We studied time-dependent features of high-frequency fluorescent radiation from a two-level quantum system with broken inversion spatial symmetry. The system in question was modelled after a one-electron two-level asymmetric polar semiconductor quantum dot whose electric dipole moment operator has permanent unequal diagonal matrix elements. The dot was permanently excited by incoherent pumping of some sort. Our attention was focused on the evolution of the fluorescence spectrum following abrupt switching on of an additional driving monochromatic field, which frequency is much lower than the optical transition frequency of the quantum dot. An analytical expression for the fluorescence spectrum as a function of the amplitude, initial phase and frequency of the monochromatic driving field, as well as of the pumping intensity and the elapsed time, was derived.