72 research outputs found

    Stability of densities for perturbed Diffusions and Markov Chains

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    We are interested in studying the sensitivity of diffusion processes or their approximations by Markov Chains with respect to a perturbation of the coefficients.Comment: 26 page

    Spin relaxation times of donor centers associated with lithium in monoisotopic 28Si

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    Β© (2016) Trans Tech Publications, Switzerland. We report a detailed study of electron longitudinal and transverse spin relaxation times for Li donors in monoisotopic 28Si over the temperature range 4–20 K using continuous wave and pulsed electron paramagnetic resonance. Comparison of the obtained spin-lattice relaxation times for the states of the isolated donor center and lithium complex LiO showed that due to the presence of orbital degeneracy, relaxation is faster for single lithium than for the LiO complexes with the nondegenerate ground state. For the isolated lithium center in silicon the relaxation is well described by Blume-Orbach process, with the parameters of the spin-orbit coupling ~ 1Β·10-6 meV compare to Orbach process for LiO complex with spin-orbit coupling parameter ~ 1.5Β·10-2 meV

    ВлияниС осаТдСния частиц ΠΊΠΎΠ±Π°Π»ΡŒΡ‚Π° Π½Π° ΠΊΠ²Π°Π½Ρ‚ΠΎΠ²Ρ‹Π΅ ΠΏΠΎΠΏΡ€Π°Π²ΠΊΠΈ ΠΊ проводимости Π”Ρ€ΡƒΠ΄Π΅ Π² твистированном CVD Π³Ρ€Π°Ρ„Π΅Π½Π΅

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    The use of graphene in electronics requires both an experimental study of the formation of high-quality low-resistance contacts and a deeper understanding of the mechanisms of electron carrier transport in graphene sheets and in the vicinity of metal / graphene interface. In this work, we studied the charge carrier transport in twisted CVD graphene, which was decorated with electrochemically deposited Co particles forming an ohmic contact with the graphene sheet. The temperature and magnetic field dependences of the sheet resistance R(T,B) in the pristine and decorated twisted graphene on silicon oxide substrate are compared. The coexistence of the negative (at magnetic fields with induction B below 1 T) and positive (B higher than 1 T) contributions to the magnetoresistive effect in both types of samples is shown. The R(T,B) dependences are analyzed in fraimwork of the theory of two-dimensional interference quantum corrections to Drude conductivity, taking into account the competition of the contribution from the hopping conduction mechanism. It has been shown that in the studied temperatures range (2-300 K) and magnetic fields (up to 8 T), when describing the transport of charge carriers in the studied samples, it is necessary to take into account at least three interference contributions to the conductivity: from weak localization, intervalley scattering, and breaking of pseudospin chirality, as well as warping of graphene due to thermal fluctuations.ИспользованиС Π³Ρ€Π°Ρ„Π΅Π½Π° Π² элСктроникС Ρ‚Ρ€Π΅Π±ΡƒΠ΅Ρ‚ ΠΊΠ°ΠΊ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ исслСдования процСсса формирования высококачСствСнных Π½ΠΈΠ·ΠΊΠΎΠΎΠΌΠ½Ρ‹Ρ… ΠΊΠΎΠ½Ρ‚Π°ΠΊΡ‚ΠΎΠ², Ρ‚Π°ΠΊ ΠΈ углублСния понимания ΠΌΠ΅Ρ…Π°Π½ΠΈΠ·ΠΌΠΎΠ² элСктронного пСрСноса Π² окрСстности ΠΊΠΎΠ½Ρ‚Π°ΠΊΡ‚Π° ΠΌΠ΅Ρ‚Π°Π»Π»/Π³Ρ€Π°Ρ„Π΅Π½. Π’ Ρ€Π°Π±ΠΎΡ‚Π΅ исслСдован транспорт носитСлСй заряда Π² твистированном CVD Π³Ρ€Π°Ρ„Π΅Π½Π΅, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΉ Π΄Π΅ΠΊΠΎΡ€ΠΈΡ€ΠΎΠ²Π°Π½ элСктрохимичСски осаТдСнными частицами Co, ΠΎΠ±Ρ€Π°Π·ΡƒΡŽΡ‰ΠΈΠΌΠΈ омичСский ΠΊΠΎΠ½Ρ‚Π°ΠΊΡ‚ с Π³Ρ€Π°Ρ„Π΅Π½ΠΎΠ²Ρ‹ΠΌ слоСм. Π‘ΠΎΠΏΠΎΡΡ‚Π°Π²Π»ΡΡŽΡ‚ΡΡ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½Ρ‹Π΅ ΠΈ ΠΌΠ°Π³Π½Π΅Ρ‚ΠΎΠΏΠΎΠ»Π΅Π²Ρ‹Π΅ зависимости слоСвого сопротивлСния R(T,B) исходного ΠΈ Π΄Π΅ΠΊΠΎΡ€ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ  твистированного Π³Ρ€Π°Ρ„Π΅Π½Π° Π½Π° ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠ΅ ΠΈΠ· оксида крСмния. Показано сосущСствованиС ΠΎΡ‚Ρ€ΠΈΡ†Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ (ΠΏΡ€ΠΈ ΠΈΠ½Π΄ΡƒΠΊΡ†ΠΈΠΈ ΠΌΠ°Π³Π½ΠΈΡ‚Π½ΠΎΠ³ΠΎ поля Π½ΠΈΠΆΠ΅ 1 Π’Π») ΠΈ ΠΏΠΎΠ»ΠΎΠΆΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ (индукция Π²Ρ‹ΡˆΠ΅ 1 Π’Π») Π²ΠΊΠ»Π°Π΄ΠΎΠ² Π² магниторСзистивный эффСкт Π² ΠΎΠ±ΠΎΠΈΡ… Ρ‚ΠΈΠΏΠ°Ρ… ΠΎΠ±Ρ€Π°Π·Ρ†ΠΎΠ². Зависимости R(T,B) Π°Π½Π°Π»ΠΈΠ·ΠΈΡ€ΡƒΡŽΡ‚ΡΡ Π½Π° основС Ρ‚Π΅ΠΎΡ€ΠΈΠΈ Π΄Π²ΡƒΠΌΠ΅Ρ€Π½Ρ‹Ρ… ΠΈΠ½Ρ‚Π΅Ρ€Ρ„Π΅Ρ€Π΅Π½Ρ†ΠΈΠΎΠ½Π½Ρ‹Ρ… ΠΊΠ²Π°Π½Ρ‚ΠΎΠ²Ρ‹Ρ… ΠΏΠΎΠΏΡ€Π°Π²ΠΎΠΊ ΠΊ проводимости Π”Ρ€ΡƒΠ΄Π΅ с ΡƒΡ‡Π΅Ρ‚ΠΎΠΌ ΠΊΠΎΠ½ΠΊΡƒΡ€Π΅Π½Ρ†ΠΈΠΈ Π²ΠΊΠ»Π°Π΄Π° ΠΎΡ‚ ΠΏΡ€Ρ‹ΠΆΠΊΠΎΠ²ΠΎΠ³ΠΎ ΠΌΠ΅Ρ…Π°Π½ΠΈΠ·ΠΌΠ° проводимости. Показано, Ρ‡Ρ‚ΠΎ Π² ΠΈΠ·ΡƒΡ‡Π΅Π½Π½ΠΎΠΉ области Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€ (2–300 К) ΠΈ ΠΌΠ°Π³Π½ΠΈΡ‚Π½Ρ‹Ρ… ΠΏΠΎΠ»Π΅ΠΉ (Π΄ΠΎ 8Β Π’Π») ΠΏΡ€ΠΈ описании транспорта носитСлСй заряда Π² исслСдованном Π³Ρ€Π°Ρ„Π΅Π½Π΅ Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎ ΡƒΡ‡ΠΈΡ‚Ρ‹Π²Π°Ρ‚ΡŒ Π½Π΅ ΠΌΠ΅Π½Π΅Π΅ Ρ‚Ρ€Π΅Ρ… ΠΈΠ½Ρ‚Π΅Ρ€Ρ„Π΅Ρ€Π΅Π½Ρ†ΠΈΠΎΠ½Π½Ρ‹Ρ… Π²ΠΊΠ»Π°Π΄ΠΎΠ² Π² ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠΌΠΎΡΡ‚ΡŒ: ΠΎΡ‚ слабой Π»ΠΎΠΊΠ°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ, ΠΌΠ΅ΠΆΠ΄ΠΎΠ»ΠΈΠ½Π½ΠΎΠ³ΠΎ рассСяния ΠΈ Π½Π°Ρ€ΡƒΡˆΠ΅Π½ΠΈΡ Ρ…ΠΈΡ€Π°Π»ΡŒΠ½ΠΎΡΡ‚ΠΈ псСвдоспина, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΊΠΎΡ€ΠΎΠ±Π»Π΅Π½ΠΈΠ΅ΠΌ Π³Ρ€Π°Ρ„Π΅Π½Π° вслСдствиС Ρ‚Π΅ΠΏΠ»ΠΎΠ²Ρ‹Ρ… Ρ„Π»ΡƒΠΊΡ‚ΡƒΠ°Ρ†ΠΈΠΉ
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