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    Π€ΠΎΡ€ΠΌΡƒΠ»Ρ‹ элСктродинамики для срСд с ΠΎΡ‚Ρ€ΠΈΡ†Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ диэлСктричСской ΠΏΡ€ΠΎΠ½ΠΈΡ†Π°Π΅ΠΌΠΎΡΡ‚ΡŒΡŽ

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    Electrodynamic formulas widely used in the description of objects containing dielectric media give results contrary to physics in the case when the permittivity of the medium takes a negative value. The problem is solved by refined formulas that allow calculating the electric potentials of the point charge and the point dipole moment, the capacitance of the capacitor, as well as the energy density of the electromagnetic field and the quality factor of the material. The formulas are valid for any media, both with positive and negative real part of the complex permittivity.Π€ΠΎΡ€ΠΌΡƒΠ»Ρ‹ элСктродинамики, ΡˆΠΈΡ€ΠΎΠΊΠΎ ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅ΠΌΡ‹Π΅ ΠΏΡ€ΠΈ описании ΠΎΠ±ΡŠΠ΅ΠΊΡ‚ΠΎΠ², содСрТащих диэлСктричСскиС срСды, Π΄Π°ΡŽΡ‚ ΠΏΡ€ΠΎΡ‚ΠΈΠ²ΠΎΡ€Π΅Ρ‡Π°Ρ‰ΠΈΠ΅ Ρ„ΠΈΠ·ΠΈΠΊΠ΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ Π² случаС, ΠΊΠΎΠ³Π΄Π° диэлСктричСская ΠΏΡ€ΠΎΠ½ΠΈΡ†Π°Π΅ΠΌΠΎΡΡ‚ΡŒ срСды ΠΏΡ€ΠΈΠ½ΠΈΠΌΠ°Π΅Ρ‚ ΠΎΡ‚Ρ€ΠΈΡ†Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠ΅ Π·Π½Π°Ρ‡Π΅Π½ΠΈΠ΅. ΠŸΡ€ΠΎΠ±Π»Π΅ΠΌΡƒ ΡΠ½ΠΈΠΌΠ°ΡŽΡ‚ ΡƒΡ‚ΠΎΡ‡Π½Π΅Π½Π½Ρ‹Π΅ Ρ„ΠΎΡ€ΠΌΡƒΠ»Ρ‹, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‰ΠΈΠ΅ Ρ€Π°ΡΡΡ‡ΠΈΡ‚Ρ‹Π²Π°Ρ‚ΡŒ элСктричСскиС ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»Ρ‹ Ρ‚ΠΎΡ‡Π΅Ρ‡Π½ΠΎΠ³ΠΎ заряда ΠΈ Ρ‚ΠΎΡ‡Π΅Ρ‡Π½ΠΎΠ³ΠΎ дипольного ΠΌΠΎΠΌΠ΅Π½Ρ‚Π°, Π΅ΠΌΠΊΠΎΡΡ‚ΡŒ кондСнсатора, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΏΠ»ΠΎΡ‚Π½ΠΎΡΡ‚ΡŒ энСргии элСктромагнитного поля ΠΈ Π΄ΠΎΠ±Ρ€ΠΎΡ‚Π½ΠΎΡΡ‚ΡŒ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π°. Π€ΠΎΡ€ΠΌΡƒΠ»Ρ‹ справСдливы для Π»ΡŽΠ±Ρ‹Ρ… срСд ΠΊΠ°ΠΊ с ΠΏΠΎΠ»ΠΎΠΆΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΉ, Ρ‚Π°ΠΊ ΠΈ с ΠΎΡ‚Ρ€ΠΈΡ†Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ Π΄Π΅ΠΉΡΡ‚Π²ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΉ Ρ‡Π°ΡΡ‚ΡŒΡŽ комплСксной диэлСктричСской проницаСмости

    Electrodynamic Formulas for Media with Negative Permittivity

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    ΠŸΠΎΡΡ‚ΡƒΠΏΠΈΠ»Π°: 02.10.2023. ΠŸΡ€ΠΈΠ½ΡΡ‚Π° Π² ΠΏΠ΅Ρ‡Π°Ρ‚ΡŒ: 10.11.2023.ΠŸΡƒΠ±Π»ΠΈΠΊΡƒΠ΅Ρ‚ΡΡ Π² порядкС обсуТдСния.Received: 02.10.2023. Accepted: 10.11.2023.Published in order of discussion.Π€ΠΎΡ€ΠΌΡƒΠ»Ρ‹ элСктродинамики, ΡˆΠΈΡ€ΠΎΠΊΠΎ ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅ΠΌΡ‹Π΅ ΠΏΡ€ΠΈ описании ΠΎΠ±ΡŠΠ΅ΠΊΡ‚ΠΎΠ², содСрТащих диэлСктричСскиС срСды, Π΄Π°ΡŽΡ‚ ΠΏΡ€ΠΎΡ‚ΠΈΠ²ΠΎΡ€Π΅Ρ‡Π°Ρ‰ΠΈΠ΅ Ρ„ΠΈΠ·ΠΈΠΊΠ΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ Π² случаС, ΠΊΠΎΠ³Π΄Π° диэлСктричСская ΠΏΡ€ΠΎΠ½ΠΈΡ†Π°Π΅ΠΌΠΎΡΡ‚ΡŒ срСды ΠΏΡ€ΠΈΠ½ΠΈΠΌΠ°Π΅Ρ‚ ΠΎΡ‚Ρ€ΠΈΡ†Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠ΅ Π·Π½Π°Ρ‡Π΅Π½ΠΈΠ΅. ΠŸΡ€ΠΎΠ±Π»Π΅ΠΌΡƒ ΡΠ½ΠΈΠΌΠ°ΡŽΡ‚ ΡƒΡ‚ΠΎΡ‡Π½Π΅Π½Π½Ρ‹Π΅ Ρ„ΠΎΡ€ΠΌΡƒΠ»Ρ‹, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‰ΠΈΠ΅ Ρ€Π°ΡΡΡ‡ΠΈΡ‚Ρ‹Π²Π°Ρ‚ΡŒ элСктричСскиС ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»Ρ‹ Ρ‚ΠΎΡ‡Π΅Ρ‡Π½ΠΎΠ³ΠΎ заряда ΠΈ Ρ‚ΠΎΡ‡Π΅Ρ‡Π½ΠΎΠ³ΠΎ дипольного ΠΌΠΎΠΌΠ΅Π½Ρ‚Π°, Π΅ΠΌΠΊΠΎΡΡ‚ΡŒ кондСнсатора, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΏΠ»ΠΎΡ‚Π½ΠΎΡΡ‚ΡŒ энСргии элСктромагнитного поля ΠΈ Π΄ΠΎΠ±Ρ€ΠΎΡ‚Π½ΠΎΡΡ‚ΡŒ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π°. Π€ΠΎΡ€ΠΌΡƒΠ»Ρ‹ справСдливы для Π»ΡŽΠ±Ρ‹Ρ… срСд ΠΊΠ°ΠΊ с ΠΏΠΎΠ»ΠΎΠΆΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΉ, Ρ‚Π°ΠΊ ΠΈ с ΠΎΡ‚Ρ€ΠΈΡ†Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ Π΄Π΅ΠΉΡΡ‚Π²ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΉ Ρ‡Π°ΡΡ‚ΡŒΡŽ комплСксной диэлСктричСской проницаСмости.Electrodynamic formulas widely used in the description of objects containing dielectric media give results contrary to physics in the case when the permittivity of the medium takes a negative value. The problem is solved by refined formulas that allow calculating the electric potentials of the point charge and the point dipole moment, the capacitance of the capacitor, as well as the energy density of the electromagnetic field and the quality factor of the material. The formulas are valid for any media, both with positive and negative real part of the complex permittivity.ЀинансированиС Ρ€Π°Π±ΠΎΡ‚Ρ‹: Ρ€Π°Π±ΠΎΡ‚Π° Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½Π° Π² Ρ€Π°ΠΌΠΊΠ°Ρ… Π½Π°ΡƒΡ‡Π½ΠΎΠΉ Ρ‚Π΅ΠΌΠ°Ρ‚ΠΈΠΊΠΈ Госзадания Π˜Π½ΡΡ‚ΠΈΡ‚ΡƒΡ‚Π° Ρ„ΠΈΠ·ΠΈΠΊΠΈ ΠΈΠΌ. Π›. Π’. ΠšΠΈΡ€Π΅Π½ΡΠΊΠΎΠ³ΠΎ БО РАН.The investigation was carried out within the state assignment of Kirensky Institute of Physics

    Resonances of electromagnetic oscillations in a spherical metal nanoparticle

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    ВСкст ΡΡ‚Π°Ρ‚ΡŒΠΈ Π½Π΅ публикуСтся Π² ΠΎΡ‚ΠΊΡ€Ρ‹Ρ‚ΠΎΠΌ доступС Π² соотвСтствии с ΠΏΠΎΠ»ΠΈΡ‚ΠΈΠΊΠΎΠΉ ΠΆΡƒΡ€Π½Π°Π»Π°.Electrodynamic analysis of plasma oscillations in a spherical metal nanoparticle is performed. It is shown that typical reduction in the frequency and quality factor of the resonances with increasing nanoparticle radius fades if the mode number grows. Depending on the particle radius, the resonant enhancement of the electric field might considerably either increase or decrease with increasing mode number

    Design of bandpass filters composed of dielectric layers separated by gratings of strip conductors

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    ВСкст ΡΡ‚Π°Ρ‚ΡŒΠΈ Π½Π΅ публикуСтся Π² ΠΎΡ‚ΠΊΡ€Ρ‹Ρ‚ΠΎΠΌ доступС Π² соотвСтствии с ΠΏΠΎΠ»ΠΈΡ‚ΠΈΠΊΠΎΠΉ ΠΆΡƒΡ€Π½Π°Π»Π°.We derive the design formulas for novel multilayer bandpass filters in which every dielectric layer (resonator) is separated from the adjacent layer or external medium by a grating of strip conductors. Every grating acts as a semireflecting mirror. Such novel filters have wide stop bands compared to conventional filters with multilayer dielectric mirrors between resonators at the same passband width. The parameters of the lowpass, lumped-element prototype filter, as well as the theory of resonator-coupling coefficients, are considered in our approach. The computed frequency response of the fifth-order Chebyshev filter that was synthesized using the proposed formulas is also presented

    Design of bandpass filters composed of dielectric layers separated by gratings of strip conductors

    No full text
    ВСкст ΡΡ‚Π°Ρ‚ΡŒΠΈ Π½Π΅ публикуСтся Π² ΠΎΡ‚ΠΊΡ€Ρ‹Ρ‚ΠΎΠΌ доступС Π² соотвСтствии с ΠΏΠΎΠ»ΠΈΡ‚ΠΈΠΊΠΎΠΉ ΠΆΡƒΡ€Π½Π°Π»Π°.We derive the design formulas for novel multilayer bandpass filters in which every dielectric layer (resonator) is separated from the adjacent layer or external medium by a grating of strip conductors. Every grating acts as a semireflecting mirror. Such novel filters have wide stop bands compared to conventional filters with multilayer dielectric mirrors between resonators at the same passband width. The parameters of the lowpass, lumped-element prototype filter, as well as the theory of resonator-coupling coefficients, are considered in our approach. The computed frequency response of the fifth-order Chebyshev filter that was synthesized using the proposed formulas is also presented

    Study of the fields scattered by a periodic strip structure of thin magnetic films

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    ВСкст ΡΡ‚Π°Ρ‚ΡŒΠΈ Π½Π΅ публикуСтся Π² ΠΎΡ‚ΠΊΡ€Ρ‹Ρ‚ΠΎΠΌ доступС Π² соотвСтствии с ΠΏΠΎΠ»ΠΈΡ‚ΠΈΠΊΠΎΠΉ ΠΆΡƒΡ€Π½Π°Π»Π°.Components of the fields scattered by a periodic planar strip structure of thin magnetic films possessing a uniaxial magnetic anisotropy in the plane have been calculated using the phenomenological model. Regularities in the dependence of these fields on the design parameters of the structure have been studied. The results obtained agree with the numerical analysis of the micromagnetic model of this structure. It has been shown that, near the edges of strips magnetized orthogonally to the major axis, the components of the scattered field can exceed the external magnetizing field by a few orders of magnitude. This fact makes it possible to design highly efficient magnetoresistive elements on the basis of a strip structure of magnetic films and thin semiconductor films
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