33 research outputs found

    Relaxation of a relativistic electron beam in plasma in the trapping regime

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    A model for collective relaxation of high-power relativistic electron beams in plasmas is proposed, which describes beam-plasma interaction in the regime when amplitudes of unstable waves are large enough to trap beam electrons. The model predicts profiles of energy release along the plasma column in a good quantitative agreement with experimental measurements.Π—Π°ΠΏΡ€ΠΎΠΏΠΎΠ½ΠΎΠ²Π°Π½ΠΎ модСль ΠΊΠΎΠ»Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡ— рСлаксації ΠΏΠΎΡ‚ΡƒΠΆΠ½ΠΎΠ³ΠΎ Ρ€Π΅Π»ΡΡ‚ΠΈΠ²Ρ–ΡΡ‚ΡΡŒΠΊΠΎΠ³ΠΎ Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΡƒΡ‡ΠΊΠ°, яка описує Π²Π·Π°Ρ”ΠΌΠΎΠ΄Ρ–ΡŽ ΠΏΡƒΡ‡ΠΊΠ° Π· плазмою Π² Ρ€Π΅ΠΆΠΈΠΌΡ–, ΠΏΡ€ΠΈ якому СнСргія нСстійких коливань Π²ΠΈΡΠ²Π»ΡΡ”Ρ‚ΡŒΡΡ Π΄ΠΎΡΡ‚Π°Ρ‚Π½ΡŒΠΎΡ— для захоплСння Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Ρ–Π² ΠΏΡƒΡ‡ΠΊΠ°. МодСль ΠΏΠ΅Ρ€Π΅Π΄Π±Π°Ρ‡Π°Ρ” ΠΏΡ€ΠΎΡ„Ρ–Π»Ρ– СнСрговиділСння ΠΏΡƒΡ‡ΠΊΠ° Π² ΠΏΠ»Π°Π·ΠΌΡ– ΠΏΠΎ Π΄ΠΎΠ²ΠΆΠΈΠ½Ρ– установки, які Π·Π½Π°Ρ…ΠΎΠ΄ΡΡ‚ΡŒΡΡ Π² Π³Π°Ρ€Π½Ρ–ΠΉ ΠΊΡ–Π»ΡŒΠΊΡ–ΡΠ½Ρ–ΠΉ Π·Π³ΠΎΠ΄Ρ– Π· Π΅ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΈΠΌΠΈ Π΄Π°Π½ΠΈΠΌΠΈ.ΠŸΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Π° модСль ΠΊΠΎΠ»Π»Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΠΉ рСлаксации ΠΌΠΎΡ‰Π½ΠΎΠ³ΠΎ рСлятивистского элСктронного ΠΏΡƒΡ‡ΠΊΠ°, ΠΎΠΏΠΈΡΡ‹Π²Π°ΡŽΡ‰Π°Ρ взаимодСйствиС ΠΏΡƒΡ‡ΠΊΠ° с ΠΏΠ»Π°Π·ΠΌΠΎΠΉ Π² Ρ€Π΅ΠΆΠΈΠΌΠ΅, ΠΏΡ€ΠΈ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΌ энСргия нСустойчивых ΠΊΠΎΠ»Π΅Π±Π°Π½ΠΈΠΉ оказываСтся достаточной для Π·Π°Ρ…Π²Π°Ρ‚Π° элСктронов ΠΏΡƒΡ‡ΠΊΠ°. МодСль прСдсказываСт ΠΏΡ€ΠΎΡ„ΠΈΠ»ΠΈ энСрговыдСлСния ΠΏΡƒΡ‡ΠΊΠ° Π² ΠΏΠ»Π°Π·ΠΌΠ΅ ΠΏΠΎ Π΄Π»ΠΈΠ½Π΅ установки, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ находятся Π² Ρ…ΠΎΡ€ΠΎΡˆΠ΅ΠΌ количСствСнном согласии с ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹ΠΌΠΈ Π΄Π°Π½Π½Ρ‹ΠΌΠΈ

    Hybrid Tamm-cavity modes in photonic crystal with resonant nanocomposite defect layer

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    Hybrid optical modes in a one-dimensional photonic crystal with a resonant nanocomposite defect bounded by a metallic layer are studied. The nanocomposite consists of spherical metallic constituents, that are distributed in a dielectric matrix. Transmittance, reflectance, and absorbance spectra of this structure, which is shined by light with normal incidence, are calculated. The possibility of control of the hybrid modes spectral characteristics by changing the thickness of the layer adjacent to the metal, the number of layers, and the nanocomposite filling factor is shown.This research was funded by the Russian Foundation for Basic Research, Government of Krasnoyarsk Territory, Krasnoyarsk Region Science and Technology Support Fund to the research Project No 18-42-243025

    Long-lived magnetoexcitons in 2D-fermion system

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    The paper addresses the experimental technique that, when applied to a 2D-electron system in the integer quantum Hall regime with filling factor ν = 2 (the Hall insulating state), allows resonant excitation of magnetoexcitons, their detection, control of an ensemble of long-lived triplet excitons and investigation of their radiationless decay related to exciton spin relaxation into the ground state. The technique proposed enables independent control of photoexcited electrons and Fermi-holes using photoinduced resonance reflection spectra as well as estimate with a reasonable degree of accuracy the resulting density of photoinduced electron-hole pairs bound into magnetoexcitons. The mere existence of triplet excitons was directly established by inelastic light scattering spectra which were analyzed to determine the value of singlet-triplet exciton splitting. It was found that the lifetimes of triplet excitons conditioned by electron spin relaxation in highly perfect GaAs/AlGaAs heterostructures with highly mobile 2D electrons are extremely long exceeding 100  ΞΌs at T < 1 K. The paper presents a qualitative explanation of the long-spin relaxation lifetimes which are unprecedented for translation-invariant 2D systems. This enabled us to create sufficiently high concentrations of triplet magnetoexcitons, electrically neutral excitations following Bose–Einstein statistics, in a Fermi electron system and investigate their collective properties. At sufficiently high densities of triplet magnetoexcitons and low temperatures, T < 1 K, the degenerate magnetofermionic system exhibits condensation of the triplet magnetoexcitons into a qualitatively new collective state with unusual properties which occurs in the space of generalized moments (magnetic translation vectors). The occurrence of a condensed phase is accompanied with a significant decrease in the viscosity of the photoexcited system, which is responsible for electron spin transport at macroscopic distances, as well as with the effects of threshold enhancement of the system response to the external action of the electromagnetic field and emergence of a new intensive radiative recombination channel

    Research of the thermal desorption processes in oxide mixtures at laser effect

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    To investigate the physical-chemical processes occurring during the heating stage of spent nuclear fuel magneto plasma reprocessing a study of thermal desorption of oxides and oxide mixtures as SNF simulators under the influence of stationary laser radiation are being studied. Preliminary experiments were carried out. X-ray diffraction and energy dispersive X-ray microanalysis of the film deposited on the substrate after laser influence on a mixture of Bβ‚‚O₃/ZrOβ‚‚ oxides have been performed.Для вивчСння Ρ„Ρ–Π·ΠΈΠΊΠΎ-Ρ…Ρ–ΠΌΡ–Ρ‡Π½ΠΈΡ… процСсів, Ρ‰ΠΎ Π²Ρ–Π΄Π±ΡƒΠ²Π°ΡŽΡ‚ΡŒΡΡ Π½Π° стадії Π½Π°Π³Ρ€Ρ–Π²Ρƒ ΠΌΠ°Π³Π½Ρ–Ρ‚ΠΎΠΏΠ»Π°Π·ΠΌΠΎΠ²ΠΎΡ— ΠΏΠ΅Ρ€Π΅Ρ€ΠΎΠ±ΠΊΠΈ Π²Ρ–Π΄ΠΏΡ€Π°Ρ†ΡŒΠΎΠ²Π°Π½ΠΎΠ³ΠΎ ядСрного ΠΏΠ°Π»ΠΈΠ²Π° (Π’Π―ΠŸ), ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΡ‚ΡŒΡΡ дослідТСння процСсів тСрмодСсорбції оксидів Ρ– оксидних ΡΡƒΠΌΡ–ΡˆΠ΅ΠΉ - Ρ–ΠΌΡ–Ρ‚Π°Ρ‚ΠΎΡ€Ρ–Π² Π’Π―ΠŸ ΠΏΡ€ΠΈ Π²ΠΏΠ»ΠΈΠ²Ρ– стаціонарного Π»Π°Π·Π΅Ρ€Π½ΠΎΠ³ΠΎ Π²ΠΈΠΏΡ€ΠΎΠΌΡ–Π½ΡŽΠ²Π°Π½Π½Ρ. ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΠΏΠΎΠΏΠ΅Ρ€Π΅Π΄Π½Ρ– СкспСримСнти, Π²ΠΈΠΊΠΎΠ½Π°Π½Ρ– Ρ€Π΅Π½Ρ‚Π³Π΅Π½ΠΎΠ΄ΠΈΡ„Ρ€Π°ΠΊΡ†Ρ–ΠΉΠ½ΠΈΠΉ Ρ– СнСргодиспСрсійний Ρ€Π΅Π½Ρ‚Π³Π΅Π½Ρ–Π²ΡΡŒΠΊΠΈΠΉ ΠΌΡ–ΠΊΡ€ΠΎΠ°Π½Π°Π»Ρ–Π·ΠΈ ΠΏΠ»Ρ–Π²ΠΊΠΈ, осадТСної Π½Π° ΠΏΡ–Π΄ΠΊΠ»Π°Π΄ΠΊΡƒ після Π»Π°Π·Π΅Ρ€Π½ΠΎΠ³ΠΎ Π²ΠΏΠ»ΠΈΠ²Ρƒ Π½Π° ΡΡƒΠΌΡ–Ρˆ оксидів Bβ‚‚O₃/ZrOβ‚‚.Для изучСния Ρ„ΠΈΠ·ΠΈΠΊΠΎ-химичСских процСссов, происходящих Π½Π° стадии Π½Π°Π³Ρ€Π΅Π²Π° ΠΌΠ°Π³Π½ΠΈΡ‚ΠΎΠΏΠ»Π°Π·ΠΌΠ΅Π½Π½ΠΎΠΉ ΠΏΠ΅Ρ€Π΅Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ ΠΎΡ‚Ρ€Π°Π±ΠΎΡ‚Π°Π²ΡˆΠ΅Π³ΠΎ ядСрного Ρ‚ΠΎΠΏΠ»ΠΈΠ²Π° (ОЯВ), проводится исслСдованиС тСрмодСсорбции оксидов ΠΈ оксидных смСсСй – ΠΈΠΌΠΈΡ‚Π°Ρ‚ΠΎΡ€ΠΎΠ² ОЯВ ΠΏΡ€ΠΈ воздСйствии стационарного Π»Π°Π·Π΅Ρ€Π½ΠΎΠ³ΠΎ излучСния. ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½Ρ‹ ΠΏΡ€Π΅Π΄Π²Π°Ρ€ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Π΅ экспСримСнты, Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½Ρ‹ Ρ€Π΅Π½Ρ‚Π³Π΅Π½ΠΎΠ΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΎΠ½Π½Ρ‹ΠΉ ΠΈ энСргодиспСрсионный рСнтгСновский ΠΌΠΈΠΊΡ€ΠΎΠ°Π½Π°Π»ΠΈΠ·Ρ‹ ΠΏΠ»Π΅Π½ΠΊΠΈ, осаТдСнной Π½Π° ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΡƒ ΠΏΡ€ΠΈ Π»Π°Π·Π΅Ρ€Π½ΠΎΠΌ воздСйствии Π½Π° смСсь оксидов Bβ‚‚O₃/ZrOβ‚‚
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