• 한국원자력학회:학술대회논문집
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• 한국원자력학회 1999년도 추계학술발표회요약집
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• pp.382.1-382
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• 1999

• 한국광학회:학술대회논문집
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• 한국광학회 1990년도 제5회 파동 및 레이저 학술발표회 5th Conference on Waves and lasers 논문집 - 한국광학회
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• pp.115-120
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• 1990

The spectroscopic properties of Cr3+-doped sapphire and Ti3+-doped sapphire fibers are reported. Tensile stress produces blue shifts of the R lines and changes in their radiative lifetimes and integrated intensities which can be correlated to stress-induced changes of the crystal-field parameters in a Cr3+-doped sapphire fiber. A net red shift of the zero phonon fluorescence line of 2Eg state and a decrease of the splittings of 2T2g state with uniaxial stress are observed in a Ti3+-doped sapphire. In excitation spectra the two peaks from the 2Eg state are shifted to the blue with different rates. The changes are attributed to the stress-induced changes of crystal field and Jahn-Teller effect.

• Journal of the Optical Society of Korea
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• 제6권2호
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• pp.48-54
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• 2002

Experimental study is performed on flashlamp-pumped Ti: sapphire lasers with single, double, and four-partial-ellipse-pump cavities aiming at improving the performance of the lasers. The output energy of 604 mJ per pulse with a width of 25 $\mu$s at a total laser efficiency of 0.13% is achieved in the laser pumped by a light pulse of 45$\mu$s without a fluorescent converter The laser output energy versus its Ti: sappy ire rod length, pumping-light pulse duration, and electrical input energy are discussed with or without using a fluorescent converter. The result shows that much more output energy is obtained il a longer Ti: sapphire-rod laser pumped by a shorter light pulse when its output coupler has an optimized transmittance. In addition, an enhancement of output energy by a factor of 7 is achieved. in the laser using a fluorescent converter LD490.

• 한국광학회지
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• 제7권4호
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• pp.390-396
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• 1996

Nd:YAG 레이저 제2고조파로 여기되는 Z자형 공진기 구조의 펄스동작 Ti:sapphire 레이저가 개발되었다. 반사율 18%의 출력거울을 사용하여 중심파장 790nm에서 27.4%의 발진효율로 822.mu.J의 레이저 출력에너지에 5ns의 펄스폭을 얻었다. 기울기 효율은 35%에 달하였다. 레이저빛살의 직경은 0.9mm, 발산각은 1.8mrad을 나타내었다. 반사율 18%의 출력거울과 3mJ의 여기에너지에서 출력스펙트럼은 90nm의 반치폭을 갖고, 740nm에서 860nm의 파장영역에 걸쳐 레이저가 출력되어 약 120nm에 이르는 파장 가변특성을 보였다.

• 대한전기학회:학술대회논문집
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• 대한전기학회 1990년도 하계학술대회 논문집
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• pp.451-454
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• 1990

Room temperature cw operations of a standing wave and a unidirectional Ti:Sapphire laser pumped by a $Ar^+$ laser have been demonstrated in the same pumping cavity configuration. Laser emission at 790 nm was excited with all-line $Ar^+$ laser pump for both cavities. The maximum output power was found to be 600 mW in the standing wave cavity and 210 mW in the ring cavity. Values of (83 ${\pm}$ 10) % for the internal quantum efficiency and (3.0 ${\pm}$ 0.5) % for the round-trip cavity loss for standing wave cavity are obtained from the thresholds and slope efficiencies measured with 2.4 and 11.2 % optput couplers. The measured cavity-loss value at 790 nm gives a meterial figure of merit (FOM) to be 146. Unidirectional operation of the ring Ti:Sapphire laser will be discussed.

• 한국광학회지
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• 제8권6호
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• pp.450-455
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• 1997

Nd:YAG 레이저 제2고조파로 여기되는 Z자형 공진기 구조의 펄스동작 Ti:sapphire 레이저가 개발되었다. 반사율 18%의 출력거울과 3mJ의 여기에너지에서 스펙트럼 반치폭은 90 nm, 파장 가변영역은 740~860 nm에 걸쳐 약 120 nm였다. 복굴절 필터를 설치하여 4 nm의 출력 스펙트럼 반치폭에 $\365mu$J의 출력에너지를 얻어 복구절 필터를 사용하지 않았을 경우보다 약 10배의 발진효율 개선효과를 얻었고, 파장 가변영역은 출력변동율이 $\pm$10%를 넘지 않는 범위에서 720~880 nm까지 약 160 nm로 넓어지는 결과를 얻었다.

• Journal of the Optical Society of Korea
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• 제7권3호
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• pp.135-138
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• 2003

A chirped-pulse amplification femtosecond Ti:sapphire laser operating at 1 KHz has been developed. The laser system consisted of a long-cavity femtosecond oscillator, a four-pass grating pulse stretcher, two multi-pass amplifiers and a double-pass grating pulse compressor. Thermal lensing at the amplifiers was reduced by cooling Ti:sapphire crystals using Peltier coolers. Gain narrowing and residual phase errors were compensated for by the use of an acousto-optic pulse shaper. The final laser output had an energy per pulse of 2.0 mJ and a pulse duration of 19.5 fs, reaching 0.1 TW at 1 KHz.

• 한국광학회:학술대회논문집
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• 한국광학회 2001년도 제12회 정기총회 및 01년도 동계학술발표회
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• pp.242-243
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• 2001

고출력 펨토초 레이저 기술은 커렌즈 모드록킹 기술, Ti：sapphire 이득매질의 개발, chirped pulse amplification (CPA) 등의 도움으로 1980년대 후반부터 급속히 발전해 왔다. 생성된 펨토초 펄스의 시간적 특성을 정확히 알아내기 위한 방법들도 많이 연구되어 주파수 분해 괌게이팅(FROG)이나 주파수위상 간섭계(SPIDER) 등의 방법들이 기존의 자체상관계를 대체하게 되었다. 극초단 레이저 펄스는 넓은 스펙트럼을 갖고 첨두출력이 높기 때문에 매질이나 광학계를 지나면서 군지연분산, 자체위상변조 등의 효과에 의한 시간적 위상변화가 쉽게 생긴다. (중략)

• Journal of the Optical Society of Korea
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• 제11권3호
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• pp.124-129
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• 2007

For the first time we compare two kinds of optical frequency combs, one of which is based on a Ti:sapphire femtosecond laser and the other is based on a mode-locked erbium-doped fiber laser. The comparison is performed by measuring an optical frequency standard with these two combs simultaneously. The two frequency measurements agree within 1.8 Hz ($3.8{\times}10^{-15}$) with the uncertainty of 17.2 Hz ($3.6{\times}10^{-14}$), from which it can be concluded that the Ti:sapphire-based frequency comb and the fiber-based frequency comb have no systematic discrepancy at this level of uncertainty.

• 한국군사과학기술학회지
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• 제17권5호
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• pp.672-679
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• 2014

To improve sensing capability of infrared, heat-resistance and mechanical properties, the $SiO_2$ and $TiO_2$ anti-reflective layers were coated on sapphire substrate by MOCVD. The standard wavelength was 4,600nm, and the thickness of anti-reflective layers were 379 and 758nm in case of ${\lambda}/4$ and ${\lambda}/2$ of incident angle($65^{\circ}$), respectively. The $SiO_2$ and $TiO_2$ anti-reflective layers were coated 12.6 and 9.7nm/min of deposition rates by increasing oxygen pressure to set the ideal refractive index of 1.283. In case of $SiO_2({\lambda}/2)$ coating, the transmittance increased from 55.0 to 62.7%. The transmittance of $TiO_2({\lambda}/2)$ anti-reflective layer also increased from 55.0 to 64.8%. The flexural strength of $SiO_2({\lambda}/2)$ and $TiO_2({\lambda}/2)$ layer coated sapphire increased from 337.8 to 362.9 and 371.8MPa, respectively. The flexural strength at $500^{\circ}C$ of these materials also increased respectively to 304.5, 358.2MPa from 265.9MPa. From these results, we confirmed these materials can be used as transmission window of infrared light.