13 research outputs found

    Ultra-fast relaxation of electrons in wide-gap dielectrics

    Get PDF
    Low-energy electrons scattered in the conduction band of a dielectric solid should behave like Bloch electrons and will interact with perturbations of the atomic lattice, i.e. with phonons. Thus the phonon-based description of low-energy scattering within an energy band structure of a solid bears certain advantages against common free-electron scattering mechanisms. Moreover, the inelastic scattering is described by the dielectric energy loss function. With these collective scattering models we have performed the simulation of excited electron relaxation and attenuation in the insulator SiO2. After excitation to a mean initial energy of several eV their energy relaxation occurs within a short time interval of 200 fs to full thermalization. There is a very rapid impact ionization cooling connected with cascading of electrons at the beginning during the first 10 fs, followed by much slower attenuation due to phonon losses in wide-gap dielectrics and insulators

    Specific features of the thermoluminescence kinetics of shallow traps in anion-defective single crystals of aluminum oxide

    No full text
    The kinetics of thermoluminescence (TL) arising from shallow traps in single crystals of anion-defective aluminum oxide has been considered. It has been shown that the TL peak at 320-350 К is characterized by identical kinetic parameters in samples containing various concentrations of shallow traps. Кinetic TL parameters for this peak have been calculated by analyzing of the luminescence isothermal decay curves, varying the heating rate, and the peak shape. An interactive relationship of shallow and dosimetric traps in the crystals under study has been supposed.ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ Π°Π½Π°Π»ΠΈΠ· ΠΊΠΈΠ½Π΅Ρ‚ΠΈΠΊΠΈ Ρ‚Π΅Ρ€ΠΌΠΎΠ»ΡŽΠΌΠΈΠ½Π΅ΡΡ†Π΅Π½Ρ†ΠΈΠΈ (Π’Π›), обусловлСнной ΠΌΠ΅Π»ΠΊΠΈΠΌΠΈ Π»ΠΎΠ²ΡƒΡˆΠΊΠ°ΠΌΠΈ Π² монокристаллах Π°Π½ΠΈΠΎΠ½-Π΄Π΅Ρ„Π΅ΠΊΡ‚Π½ΠΎΠ³ΠΎ оксида алюминия. Показано, Ρ‡Ρ‚ΠΎ Π’Π› ΠΏΠΈΠΊΠ° ΠΏΡ€ΠΈ 320-350 К характСризуСтся ΠΈΠ΄Π΅Π½Ρ‚ΠΈΡ‡Π½Ρ‹ΠΌΠΈ кинСтичСскими ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Π°ΠΌΠΈ Ρƒ ΠΎΠ±Ρ€Π°Π·Ρ†ΠΎΠ² с Ρ€Π°Π·Π»ΠΈΡ‡Π½ΠΎΠΉ ΠΊΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€Π°Ρ†ΠΈΠ΅ΠΉ ΠΌΠ΅Π»ΠΊΠΈΡ… Π»ΠΎΠ²ΡƒΡˆΠ΅ΠΊ. Рассчитаны кинСтичСскиС ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ‹ Π’Π› этого ΠΏΠΈΠΊΠ° ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ Π°Π½Π°Π»ΠΈΠ·Π° ΠΊΡ€ΠΈΠ²Ρ‹Ρ… изотСрмичСского затухания Π»ΡŽΠΌΠΈΠ½Π΅ΡΡ†Π΅Π½Ρ†ΠΈΠΈ, Π²Π°Ρ€ΠΈΠ°Ρ†ΠΈΠΈ скоростСй Π½Π°Π³Ρ€Π΅Π²Π° ΠΈ Π°Π½Π°Π»ΠΈΠ·Π° Ρ„ΠΎΡ€ΠΌΡ‹ ΠΏΠΈΠΊΠ°. Высказано ΠΏΡ€Π΅Π΄ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΠ΅ ΠΎ Π½Π°Π»ΠΈΡ‡ΠΈΠΈ ΠΈΠ½Ρ‚Π΅Ρ€Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΠΉ взаимосвязи ΠΌΠ΅Π»ΠΊΠΈΡ… ΠΈ дозимСтричСских Π»ΠΎΠ²ΡƒΡˆΠ΅ΠΊ Π² исслСдуСмых кристаллах.Π’ΠΈΠΊΠΎΠ½Π°Π½ΠΎ Π°Π½Π°Π»iΠ· ΠΊiΠ½Π΅Ρ‚ΠΈΠΊΠΈ Ρ‚Π΅Ρ€ΠΌΠΎΠ»ΡŽΠΌiнСсцСнцiΡ— (Π’Π›), ΠΎΠ±ΡƒΠΌΠΎΠ²Π»Π΅Π½ΠΎΡ— ΠΌiΠ»ΠΊΠΈΠΌΠΈ пастками Π² Π°Π½iΠΎΠ½-Π΄Π΅Ρ„Π΅ΠΊΡ‚Π½ΠΈΡ… монокристалах оксиду алюмiΠ½iю. Показано, Ρ‰ΠΎ Π’Π› ΠΏiΠΊΠ° ΠΏΡ€ΠΈ 320- 350 К Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€ΠΈΠ·ΡƒΡ”Ρ‚ΡŒΡΡ iΠ΄Π΅Π½Ρ‚ΠΈΡ‡Π½ΠΈΠΌΠΈ ΠΊiΠ½Π΅Ρ‚ΠΈΡ‡Π½ΠΈΠΌΠΈ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Π°ΠΌΠΈ для Π·Ρ€Π°Π·ΠΊiΠ² Π· Ρ€iΠ·Π½ΠΈΠΌΠΈ ΠΊΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€Π°Ρ†iями ΠΌiΠ»ΠΊΠΈΡ… пасток. ΠžΠ±Ρ‡ΠΈΡΠ»Π΅Π½ΠΎ ΠΊiΠ½Π΅Ρ‚ΠΈΡ‡Π½i ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΈ Ρ†ΡŒΠΎΠ³ΠΎ ΠΏiΠΊΠ° ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ Π°Π½Π°Π»iΠ·Ρƒ ΠΊΡ€ΠΈΠ²ΠΈΡ… iΠ·ΠΎΡ‚Π΅Ρ€ΠΌiΡ‡Π½ΠΎΠ³ΠΎ згасання люмiнСсцСнцiΡ—, Π²Π°Ρ€iювання ΡˆΠ²ΠΈΠ΄ΠΊΠΎΡΡ‚i Π½Π°Π³Ρ€iвання Ρ‚Π° Π°Π½Π°Π»iΠ·Ρƒ Ρ„ΠΎΡ€ΠΌΠΈ ΠΏiΠΊΠ°. ВисловлСно припущСння ΠΏΡ€ΠΎ наявнiΡΡ‚ΡŒ iΠ½Ρ‚Π΅Ρ€Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΠ³ΠΎ Π²Π·Π°Ρ”ΠΌΠΎΠ·Π²'язку ΠΌiΠ»ΠΊΠΈΡ… Ρ‚Π° Π΄ΠΎΠ·ΠΈΠΌΠ΅Ρ‚Ρ€ΠΈΡ‡Π½ΠΈΡ… пасток Ρƒ кристалах, Ρ‰ΠΎ дослiдТувалися
    corecore