122 research outputs found

    Высокомощный Π»Π°Π·Π΅Ρ€ Π½Π° кристаллС Yb3+:YAlO3, Ρ€Π°Π±ΠΎΡ‚Π°ΡŽΡ‰ΠΈΠΉ Π² Ρ€Π΅ΠΆΠΈΠΌΠ΅ синхронизации ΠΌΠΎΠ΄ Π½Π° основС ΠΏΠΎΠ»ΡƒΠΏΡ€ΠΎΠ²ΠΎΠ΄Π½ΠΈΠΊΠΎΠ²Ρ‹Ρ… Π·Π΅Ρ€ΠΊΠ°Π» с Π½Π°ΡΡ‹Ρ‰Π°ΡŽΡ‰ΠΈΠΌΡΡ ΠΏΠΎΠ³Π»ΠΎΡ‚ΠΈΡ‚Π΅Π»Π΅ΠΌ

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    Yttrium aluminium perovskite YAlO3 (YAP) crystal, doped with rare-earth ions, has been extensively studied as a diode-pumped laser host material. The wide interest to rare-earth ions doped YAP crystals is explained by its good thermal and mechanical properties, high natural birefringence, widely used Czochralski growth method. The aim of this work was to study the Yb3+:YAlO3 crystal as an active medium for high power mode-locked laser. Yb3+-doped perovskite-like aluminate crystals have unique spectroscopic and thermooptical properties that allowed using these crystals as an active medium of high power continuous wave (CW) and modelocked (ML) bulk lasers with diode pumping. In our work spectroscopic properties of Yb:YAP crystal and laser characteristics in CW and ML regimes are investigated. Maximum output power of 4 W with optical-to-optical efficiency of 16.3 % and 140 fs pulse duration have been obtained for Yb:YAP E //c-polarization with 10 % output coupler transmittance. Tunability range as wide as 67 nm confirms high promise of using Yb:YAP crystal for lasers working in wide spectral range

    Π Π΅Π³Π΅Π½Π΅Ρ€Π°Ρ‚ΠΈΠ²Π½Ρ‹ΠΉ ΡƒΡΠΈΠ»ΠΈΡ‚Π΅Π»ΡŒ Ρ‡ΠΈΡ€ΠΏΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠΎΠ² Π½Π° кристаллС Yb3+:LuAlO3 с усилСниСм ΠΎΡ‚Π΄Π΅Π»ΡŒΠ½Ρ‹Ρ… ΡΠΏΠ΅ΠΊΡ‚Ρ€Π°Π»ΡŒΠ½Ρ‹Ρ… ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚ для ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠΉ Π² Ρ‚Π΅Ρ€Π°Π³Π΅Ρ€Ρ†ΠΎΠ²ΠΎΠΉ области спСктра

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    Compact diode-pumped chirped pulse regenerative amplifier systems with pulse repetition rate of hundreds kilohertz based on Yb3+-doped crystals are of practical importance for wide range of applications such as materials processing, medicine, scientific research, etc. The aim of this work was to study the Yb3+:LuAlO3 crystal based dual wavelength chirped pulse regenerative amplifier. Perovskite-like aluminate crystals have unique spectroscopic properties that allowed to use amplifier active element gain spectrum as an amplitude filter for amplified pulse spectrum and even obtained dual wavelength amplification without any additional components. In our work a simple way to obtain dual-wavelength operation of chirped pulse regenerative amplifier by using the active medium gain spectrum as an amplitude filter for the formation of the amplified pulses spectrum demonstrated for the first time to our knowledge. Maximum output power of 5.4 W of chirped pulses (3.8 W after compression) and optical-to-optical efficiency of 22.5 % have been obtained for Yb:LuAP E//b-polarization at 200 kHz repetition rate. Compressed amplified pulse duration was about 708 fs while separate spectral components durations were 643 fs and 536 fs at 1018.3 nm and 1041.1 nm central wavelengths, respectively. Performed investigations show high potential of Yb3+:LuAP crystals as active elements of compact diode pumped chirped pulse regenerative amplifiers

    Thermo-optic characterization of Yb:CaGdAlO4 laser crystal

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    Principal thermo-optic coefficients (TOCs), dno/dT and dne/dT, are measured for Yb:CaGdAlO4 crystal, for the first time, to our knowledge. At the wavelength of ~1 ΞΌm, they equal –7.6 and –8.6 (Π§10-6 K-1), accordingly. Thermal coefficients of the optical path (TCOP) are determined for this crystal for the principal crystal cuts (a-cut and c-cut) and light polarizations (Ο€ or Οƒ). Thermo-optic dispersion formulas are evaluated for both TOC and TCOP coefficients. Optical power of thermal lens is measured for diode-pumped a-cut Yb:CaGdAlO4; it is also calculated on the basis of measured material parameters. Thermal conductivity of CaGdAlO4 crystal is measured versus Yb concentration. The results indicate that a-cut Yb:CaGdAlO4 can provide really "athermal" behavior

    ΠšΠΎΠΌΠΏΠ°ΠΊΡ‚Π½Ρ‹ΠΉ Π»Π°Π·Π΅Ρ€ Π½Π° кристаллС Yb3+:LuAlO3 с Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΠΉ модуляциСй добротности Ρ€Π΅Π·ΠΎΠ½Π°Ρ‚ΠΎΡ€Π°, ΠΈΠ·Π»ΡƒΡ‡Π°ΡŽΡ‰ΠΈΠΉ Π½Π° Π΄Π»ΠΈΠ½Π΅ Π²ΠΎΠ»Π½Ρ‹ 999,6 Π½ΠΌ для примСнСния Π² Π»Π°Π·Π΅Ρ€Π½ΠΎ-искровой эмиссионной спСктроскопии

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    Compact actively Q-switched diode-pumped lasers based on Yb3+-materials are of practical importance for wide range of scientific, industrial and biomedical applications. The aim of this work was to study the Yb3+:LuAlO3 actively Q-switched laser.One of the most promising crystalline hosts for rare-earth ions are Perovskite-like aluminate crystals. Yttrium aluminate crystal YAlO3 (YAP) is a well-known host with good thermal and mechanical properties (thermal conductivity for undoped crystal is about 11 W/mΒ·K and about 8 W/mΒ·K for Yb(5 at.%):YAP) similar to those of YAG. The reduction in the thermal conductivity of doped laser crystal in comparison with host materials is small in the case of ions with close atomic mass and ionic radii such as for Yb3+ and Lu3+. This feature makes LuAlO3 (LuAP) more promising host crystal for doping by Yb3+ ions in contrast to YAP especially for high output power laser systems.Β In our work, for the first time to the best of our knowledge actively Q-switching laser operation of Yb3+:LuAP single crystal was demonstrated. The maximum average output power of 4.9 W at 50 kHz pulse repetition frequency (PRF) with opt.-to-opt. efficiency of 21 % was obtained with 30 % OC transmittance. Output power as high as 3.3 W with 333 Β΅J-laser pulses with duration of about 11.5 ns was demonstrated at 10 kHz PRF the corresponding pulse peak power was 29 kW. 97 Β΅J second harmonic pulses obtained with 29 % conversion efficiency at 10 kHz PRF.Performed investigations show high potential of Yb3+:LuAP crystals as active elements of compact diode pumped actively Q-switched lasers due to high stimulated emission cross-section (β‰ˆ 3.74Ξ‡10-20Β cm2) at 999.6 nm wavelength and significant reduction of heat load on the active element when pumping around 980 nm and generation around 999 nm.ΠšΠΎΠΌΠΏΠ°ΠΊΡ‚Π½Ρ‹Π΅ Π»Π°Π·Π΅Ρ€Ρ‹ с Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΠΉ модуляциСй добротности Ρ€Π΅Π·ΠΎΠ½Π°Ρ‚ΠΎΡ€Π°, построСнныС Π½Π° ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π°Ρ…, Π»Π΅Π³ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… ΠΈΠΎΠ½Π°ΠΌΠΈ Yb3+, ΠΏΡ€Π΅Π΄ΡΡ‚Π°Π²Π»ΡΡŽΡ‚ практичСский интСрСс для ΡˆΠΈΡ€ΠΎΠΊΠΎΠ³ΠΎ ряда Π½Π°ΡƒΡ‡Π½Ρ‹Ρ…, ΠΏΡ€ΠΎΠΌΡ‹ΡˆΠ»Π΅Π½Π½Ρ‹Ρ… ΠΈ биомСдицинских ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠΉ. ЦСлью Π΄Π°Π½Π½ΠΎΠΉ Ρ€Π°Π±ΠΎΡ‚Ρ‹ являлось исслСдованиС Ρ€Π΅ΠΆΠΈΠΌΠ° Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΠΉ модуляции добротности Ρ€Π΅Π·ΠΎΠ½Π°Ρ‚ΠΎΡ€Π° Π»Π°Π·Π΅Ρ€Π° Π½Π° кристаллС Yb3+:LuAlO3.Одними ΠΈΠ· Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ пСрспСктивных ΠΌΠ°Ρ‚Ρ€ΠΈΡ† для лСгирования ΠΈΠΎΠ½Π°ΠΌΠΈ Ρ€Π΅Π΄ΠΊΠΎΠ·Π΅ΠΌΠ΅Π»ΡŒΠ½Ρ‹Ρ… элСмСнтов ΡΠ²Π»ΡΡŽΡ‚ΡΡ кристаллы Π°Π»ΡŽΠΌΠΈΠ½Π°Ρ‚ΠΎΠ² со структурой пСровскита. ΠšΡ€ΠΈΡΡ‚Π°Π»Π»Ρ‹ ΠΈΡ‚Ρ‚Ρ€ΠΈΠ΅Π²ΠΎΠ³ΠΎ Π°Π»ΡŽΠΌΠΈΠ½Π°Ρ‚Π° YAlO3 (YAP) ΡˆΠΈΡ€ΠΎΠΊΠΎ извСстны Π² качСствС ΠΌΠ°Ρ‚Ρ€ΠΈΡ† благодаря Ρ…ΠΎΡ€ΠΎΡˆΠΈΠΌ тСрмомСханичСским свойствам (Ρ‚Π΅ΠΏΠ»ΠΎΠΏΡ€ΠΎΠ²ΠΎΠ΄Π½ΠΎΡΡ‚ΡŒ Π½Π΅Π»Π΅Π³ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ кристалла ΠΎΠΊΠΎΠ»ΠΎ 11 Π’Ρ‚/м·К ΠΈ ΠΎΠΊΠΎΠ»ΠΎ 8 Π’Ρ‚/м·К для Yb(5 Π°Ρ‚.%):YAP), Π±Π»ΠΈΠ·ΠΊΠΈΠΌ ΠΊ кристаллам YAG. Π‘Π½ΠΈΠΆΠ΅Π½ΠΈΠ΅ тСплопроводности Π»Π°Π·Π΅Ρ€Π½ΠΎΠ³ΠΎ кристалла ΠΏΡ€ΠΈ Π»Π΅Π³ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠΈ ΠΏΠΎ ΡΡ€Π°Π²Π½Π΅Π½ΠΈΡŽ с чистой ΠΌΠ°Ρ‚Ρ€ΠΈΡ†Π΅ΠΉ ΠΌΠ°Π»ΠΎ Π² случаС Π½Π΅Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ ΠΎΡ‚Π»ΠΈΡ‡Π°ΡŽΡ‰ΠΈΡ…ΡΡ Π°Ρ‚ΠΎΠΌΠ½Ρ‹Ρ… масс ΠΈ ΠΈΠΎΠ½Π½Ρ‹Ρ… радиусов ΠΊΠ°ΠΊ Π² случаС с ΠΈΠΎΠ½Π°ΠΌΠΈ Yb3+ ΠΈ Lu3+. Данная ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡ‚ΡŒ Π΄Π΅Π»Π°Π΅Ρ‚ кристалл LuAlO3 (LuAP) Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ Π±ΠΎΠ»Π΅Π΅ пСрспСктивной ΠΌΠ°Ρ‚Ρ€ΠΈΡ†Π΅ΠΉ для ΠΈΠΎΠ½ΠΎΠ² Yb3+ ΠΏΠΎ ΡΡ€Π°Π²Π½Π΅Π½ΠΈΡŽ с YAP особСнно Π² случаС Π»Π°Π·Π΅Ρ€Π½Ρ‹Ρ… систСм с высокой срСднСй Π²Ρ‹Ρ…ΠΎΠ΄Π½ΠΎΠΉ ΠΌΠΎΡ‰Π½ΠΎΡΡ‚ΡŒΡŽ.Π Π΅ΠΆΠΈΠΌ Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΠΉ модуляции добротности Π»Π°Π·Π΅Ρ€Π° Π½Π° кристаллС Yb3+:LuAP исслСдован Π²ΠΏΠ΅Ρ€Π²Ρ‹Π΅ Π² нашСй Ρ€Π°Π±ΠΎΡ‚Π΅. Максимальная срСдняя выходная ΠΌΠΎΡ‰Π½ΠΎΡΡ‚ΡŒ 4,9 Π’Ρ‚ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π° ΠΏΡ€ΠΈ частотС слСдования ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠΎΠ² 50 ΠΊΠ“Ρ† ΠΈ оптичСской эффСктивности 21 % с ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ Π²Ρ‹Ρ…ΠΎΠ΄Π½ΠΎΠ³ΠΎ Π·Π΅Ρ€ΠΊΠ°Π»Π° пропусканиСм 30 %. Выходная ΠΌΠΎΡ‰Π½ΠΎΡΡ‚ΡŒ 3,3 Π’Ρ‚, Π΄Π»ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΡŒ ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ° 11,5 нс ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ ΠΏΡ€ΠΈ частотС слСдования ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠΎΠ² 10 ΠΊΠ“Ρ†, энСргия ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ° составила 333 ΠΌΠΊΠ”ΠΆ, пиковая ΠΌΠΎΡ‰Π½ΠΎΡΡ‚ΡŒ 29 ΠΊΠ’Ρ‚. Π˜ΠΌΠΏΡƒΠ»ΡŒΡΡ‹ энСргиСй 97 ΠΌΠΊΠ”ΠΆ ΠΏΡ€ΠΈ частотС слСдования 10 ΠΊΠ“Ρ† ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ Π½Π° частотС Π²Ρ‚ΠΎΡ€ΠΎΠΉ Π³Π°Ρ€ΠΌΠΎΠ½ΠΈΠΊΠΈ с ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒΡŽ прСобразования 29 %.Β ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½Π½Ρ‹Π΅ исслСдования ΠΏΠΎΠΊΠ°Π·Ρ‹Π²Π°ΡŽΡ‚, Ρ‡Ρ‚ΠΎ благодаря высокому ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎΠΌΡƒ ΡΠ΅Ρ‡Π΅Π½ΠΈΡŽ стимулированного излучСния (β‰ˆ 3,74Ξ‡10-20 см2 ) Π½Π° Π΄Π»ΠΈΠ½Π΅ Π²ΠΎΠ»Π½Ρ‹ 999,6 Π½ΠΌ, Π° Ρ‚Π°ΠΊΠΆΠ΅ сущСствСнному сниТСнию Ρ‚Π΅ΠΏΠ»ΠΎΠ²ΠΎΠΉ Π½Π°Π³Ρ€ΡƒΠ·ΠΊΡƒ Π½Π° Π°ΠΊΡ‚ΠΈΠ²Π½Ρ‹ΠΉ элСмСнт ΠΏΡ€ΠΈ Π½Π°ΠΊΠ°Ρ‡ΠΊΠ΅ Π² области 980 Π½ΠΌ ΠΈ Π³Π΅Π½Π΅Ρ€Π°Ρ†ΠΈΠΈ Π² области 999 Π½ΠΌ, кристаллы Yb3+:LuAP вСсьма пСрспСктивны Π² качСствС Π°ΠΊΡ‚ΠΈΠ²Π½Ρ‹Ρ… элСмСнтов ΠΊΠΎΠΌΠΏΠ°ΠΊΡ‚Π½Ρ‹Ρ… Ρ‚Π²Π΅Ρ€Π΄ΠΎΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… Π»Π°Π·Π΅Ρ€ΠΎΠ² с Π΄ΠΈΠΎΠ΄Π½ΠΎΠΉ Π½Π°ΠΊΠ°Ρ‡ΠΊΠΎΠΉ, Ρ€Π°Π±ΠΎΡ‚Π°ΡŽΡ‰ΠΈΡ… Π² Ρ€Π΅ΠΆΠΈΠΌΠ΅ Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΠΉ модуляции добротности. ΠΎΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… Π»Π°Π·Π΅Ρ€ΠΎΠ² с Π΄ΠΈΠΎΠ΄Π½ΠΎΠΉ Π½Π°ΠΊΠ°Ρ‡ΠΊΠΎΠΉ, Ρ€Π°Π±ΠΎΡ‚Π°ΡŽΡ‰ΠΈΡ… Π² Ρ€Π΅ΠΆΠΈΠΌΠ΅ Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΠΉ модуляции добротности

    Высокомощный Π»Π°Π·Π΅Ρ€ Π½Π° кристаллС Yb3+:YAlO3 ,Ρ€Π°Π±ΠΎΡ‚Π°ΡŽΡ‰ΠΈΠΉ Π² Ρ€Π΅ΠΆΠΈΠΌΠ΅ синхронизации ΠΌΠΎΠ΄ Π½Π° основС ΠΏΠΎΠ»ΡƒΠΏΡ€ΠΎΠ²ΠΎΠ΄Π½ΠΈΠΊΠΎΠ²Ρ‹Ρ… Π·Π΅Ρ€ΠΊΠ°Π» с Π½Π°ΡΡ‹Ρ‰Π°ΡŽΡ‰ΠΈΠΌΡΡ ΠΏΠΎΠ³Π»ΠΎΡ‚ΠΈΡ‚Π΅Π»Π΅ΠΌ

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    Yttrium aluminium perovskite YAlO3Β (YAP) crystal, doped with rare-earth ions, has been extensively studied as a diode-pumped laser host material. The wide interest to rare-earth ions doped YAP crystals is explained by its good thermal and mechanical properties, high natural birefringence, widely used Czochralski Β growth method. The aim of this work was to study the Yb3+:YAlO3 Β crystal as an active medium for high Β power mode-locked laser.Yb3+-doped perovskite-like aluminate crystals have unique spectroscopic and thermooptical properties that allowed using these crystals as an active medium of high power continuous wave (CW) and modelocked (ML) bulk lasers with diode pumping.growth method. The aim of this work was to study the Yb3+:YAlO3 Β crystal as an active medium for high Β power mode-locked laser.In our work spectroscopic properties of Yb:YAP crystal and laser characteristics in CW and ML regimes are investigated. Maximum output power of 4 W with optical-to-optical efficiency of 16.3 % and 140 fs pulse duration have been obtained for Yb:YAP Eβ€Š//c-polarization with 10 % output coupler transmittance. Tunability range as wide as 67 nm confirms high promise of using Yb:YAP crystal for lasers working in wide spectral range.Β ΠšΡ€ΠΈΡΡ‚Π°Π»Π»Ρ‹ ΠΈΡ‚Ρ‚Ρ€ΠΈΠΉ-алюминиСвого пСровскита YAlO3 (YAP), Π»Π΅Π³ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Π΅ ΠΈΠΎΠ½Π°ΠΌΠΈ Ρ€Π΅Π΄ΠΊΠΎΠ·Π΅ΠΌΠ΅Π»ΡŒΠ½Ρ‹Ρ… элСмСнтов интСнсивно ΠΈΠ·ΡƒΡ‡Π°Π»ΠΈΡΡŒ Π² качСствС Π°ΠΊΡ‚ΠΈΠ²Π½Ρ‹Ρ… срСд Π»Π°Π·Π΅Ρ€ΠΎΠ² с Π΄ΠΈΠΎΠ΄Π½ΠΎΠΉ Π½Π°ΠΊΠ°Ρ‡ΠΊΠΎΠΉ. Π˜Π½Ρ‚Π΅Ρ€Π΅Ρ ΠΊ Π΄Π°Π½Π½Ρ‹ΠΌ кристаллам обусловлСн ΠΈΡ… высокими тСплофизичСскими ΠΈ мСханичСскими свойствами, высоким Π΄Π²ΡƒΠ»ΡƒΡ‡Π΅ΠΏΡ€Π΅Π»ΠΎΠΌΠ»Π΅Π½ΠΈΠ΅ΠΌ, Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡ‚ΡŒΡŽ роста ΠΏΠΎ ΡˆΠΈΡ€ΠΎΠΊΠΎ распространённому ΠΌΠ΅Ρ‚ΠΎΠ΄Ρƒ Π§ΠΎΡ…Ρ€Π°Π»ΡŒΡΠΊΠΎΠ³ΠΎ. ЦСлью Π΄Π°Π½Π½ΠΎΠΉ Ρ€Π°Π±ΠΎΡ‚Ρ‹ Π±Ρ‹Π»ΠΎ ΠΈΠ·ΡƒΡ‡Π΅Π½ΠΈΠ΅ кристалла Yb3+:YAlO3Β  Π² качСствС Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΠΉ срСды Π»Π°Π·Π΅Ρ€Π°  с высокой срСднСй Π²Ρ‹Ρ…ΠΎΠ΄Π½ΠΎΠΉ ΠΌΠΎΡ‰Π½ΠΎΡΡ‚ΡŒΡŽ, Ρ€Π°Π±ΠΎΡ‚Π°ΡŽΡ‰Π΅Π³ΠΎ Π² Ρ€Π΅ΠΆΠΈΠΌΠ΅ синхронизации ΠΌΠΎΠ΄.ΠšΡ€ΠΈΡΡ‚Π°Π»Π»Ρ‹ YAlO3, Π»Π΅Π³ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Π΅ Ρ‚Ρ€Ρ‘Ρ…Π²Π°Π»Π΅Π½Ρ‚Π½Ρ‹ΠΌΠΈ ΠΈΠΎΠ½Π°ΠΌΠΈ иттСрбия ΠΈΠΌΠ΅ΡŽΡ‚ ΡƒΠ½ΠΈΠΊΠ°Π»ΡŒΠ½Ρ‹Π΅ спСктроскопичСскиС ΠΈ тСплофизичСскиС свойства, Ρ‡Ρ‚ΠΎ позволяСт ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΠΎΠ²Π°Ρ‚ΡŒ Π΄Π°Π½Π½Ρ‹Π΅ кристаллы Π² качСствС Π°ΠΊΡ‚ΠΈΠ²Π½Ρ‹Ρ… срСд Π»Π°Π·Π΅Ρ€ΠΎΠ² с высокой срСднСй Π²Ρ‹Ρ…ΠΎΠ΄Π½ΠΎΠΉ ΠΌΠΎΡ‰Π½ΠΎΡΡ‚ΡŒΡŽ ΠΈ Π΄ΠΈΠΎΠ΄Π½ΠΎΠΉ Π½Π°ΠΊΠ°Ρ‡ΠΊΠΎΠΉ, Ρ€Π°Π±ΠΎΡ‚Π°ΡŽΡ‰ΠΈΡ… Π² Ρ€Π΅ΠΆΠΈΠΌΠ°Ρ… Π½Π΅ΠΏΡ€Π΅Ρ€Ρ‹Π²Π½ΠΎΠΉ Π³Π΅Π½Π΅Ρ€Π°Ρ†ΠΈΠΈ ΠΈ пассивной синхронизации ΠΌΠΎΠ΄.Π’ Ρ€Π°Π±ΠΎΡ‚Π΅ исслСдованы спСктроскопичСскиС характСристики кристалла Yb:YAP, Π° Ρ‚Π°ΠΊΠΆΠ΅ Π²Ρ‹Ρ…ΠΎΠ΄Π½Ρ‹Π΅ характСристики Π»Π°Π·Π΅Ρ€ΠΎΠ² Π½Π° основС Π΄Π°Π½Π½ΠΎΠ³ΠΎ кристалла, Ρ€Π°Π±ΠΎΡ‚Π°ΡŽΡ‰ΠΈΡ… Π² Ρ€Π΅ΠΆΠΈΠΌΠ°Ρ… Π½Π΅ΠΏΡ€Π΅Ρ€Ρ‹Π²Π½ΠΎΠΉ Π³Π΅Π½Π΅Ρ€Π°Ρ†ΠΈΠΈ ΠΈ пассивной синхронизации ΠΌΠΎΠ΄. БрСдняя выходная ΠΌΠΎΡ‰Π½ΠΎΡΡ‚ΡŒ 4 Π’Ρ‚ с оптичСской ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒΡŽ 16.3 % ΠΈ Π΄Π»ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΡŒΡŽ ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ° 140 фс ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π° для E//c-поляризации ΠΏΡ€ΠΈ пропускании Π²Ρ‹Ρ…ΠΎΠ΄Π½ΠΎΠ³ΠΎ Π·Π΅Ρ€ΠΊΠ°Π»Π° 10 %. Π”ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½ пСрСстройки 67 Π½ΠΌ ΠΏΠΎΠ΄Ρ‚Π²Π΅Ρ€ΠΆΠ΄Π°Π΅Ρ‚ высокиС пСрспСктивы использования кристалла Yb:YAP Π² качСствС Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΠΉ срСды Π»Π°Π·Π΅Ρ€ΠΎΠ², Ρ€Π°Π±ΠΎΡ‚Π°ΡŽΡ‰ΠΈΡ… Π² ΡˆΠΈΡ€ΠΎΠΊΠΎΠΌ ΡΠΏΠ΅ΠΊΡ‚Ρ€Π°Π»ΡŒΠ½ΠΎΠΌ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅

    Radiation-balanced lasing and amplification

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    Quantum statistical theory of radiation-balanced laser is constructed within method of nonequilibrium statistical operator. System of equations is derived for number of phonons and collective population difference. Their numerical solutions are obtained and discussed

    Diode-pumped continuous Wave Tm:KLu(WO<inf>4</inf>)<inf>2</inf> and Tm:KY(WO<inf>4</inf>)<inf>2</inf> microchip lasers

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    Β© 2016 IEEE.Laser performance of Tm doped KLu(WO4)2 and KY(WO4)2 crystals was investigated in a microchip cavity configuration with fiber coupled laser diode as a pump source. The highest output power of 1013 mW with 51 % slope efficiency was obtained for Tm:KY(WO4)2 crystal. Using Tm:KLu(WO4)2 crystal output power of 912 mW and slope efficiency of 38 % were achieved

    Energy transfer in Tm,Ho:KYW crystal and diode-pumped microchip laser operation

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    Β© 2016 Optical Society of America.An investigation of Tm-Ho energy transfer in Tm(5at.%),Ho(0.4at.%):KYW single crystal by two independent techiques was performed. Based on fluorescence dynamics measurements, energy transfer parameters P71 and P28 for direct (Tmβ†’Ho) and back (Hoβ†’Tm) transfers, respectively, as well as equilibrium constant Θ were evaluated. The obtained results were supported by calculation of microscopic interaction parameters according to the FΓΆrster-Dexter theory for a dipoledipole interaction. Diode-pumped continuous-wave operation of Tm,Ho:KYW microchip laser was demonstrated, for the first time to our knowledge. Maximum output power of 77 mW at 2070 nm was achieved at the fundamental TEM00 mode

    Energy transfer in Tm,Ho:KYW crystal and diode-pumped microchip laser operation

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    Β© 2016 Optical Society of America.An investigation of Tm-Ho energy transfer in Tm(5at.%),Ho(0.4at.%):KYW single crystal by two independent techiques was performed. Based on fluorescence dynamics measurements, energy transfer parameters P71 and P28 for direct (Tmβ†’Ho) and back (Hoβ†’Tm) transfers, respectively, as well as equilibrium constant Θ were evaluated. The obtained results were supported by calculation of microscopic interaction parameters according to the FΓΆrster-Dexter theory for a dipoledipole interaction. Diode-pumped continuous-wave operation of Tm,Ho:KYW microchip laser was demonstrated, for the first time to our knowledge. Maximum output power of 77 mW at 2070 nm was achieved at the fundamental TEM00 mode

    In-band pumped room-temperature Er:KY(WO4)2 laser emitting around 1:6 mm

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    We present efficient continuous-wave operation of an Er:KY(WO 4)2 crystal under in-band pumping by a compact diode-pumped Er, Yb:GdAl3(BO3)4 laser. Maximum slope efficiency of 27% and output power of 35 mW at 1609.5 nm were obtained with beam propagation factor M2 < 1:2. Absorption and stimulated emission cross-section spectra, as well as the radiative lifetime of the 4I13=2 energy level, were determined
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