2009
DOI: 10.1364/oe.17.001178
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2 kW incoherent beam combining of four narrow-linewidth photonic crystal fiber amplifiers

Abstract: We report on beam combining of four narrow-linewidth fiber amplifier chains, running at different wavelengths and each delivering 500 W optical output power. The main amplifier stage consists of a large mode area photonic crystal fiber. The four output beams of the amplifier chains are spectrally (incoherent) combined using a polarization-independent dielectric reflective diffraction grating to form an output beam of 2 kW continuous-wave optical power with good beam quality (M(2)x = 2.0, M(2)y = 1.8).

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Cited by 90 publications
(30 citation statements)
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“…In this respect 522 W of average output power with a combining efficiency of 93% was reported when using a surface grating [12]. With a reduced combining efficiency of 61% even 2 kW of power was shown [13]. Reaching these high output powers makes the combination of fiber lasers very attractive for certain applications.…”
Section: Introductionmentioning
confidence: 95%
See 1 more Smart Citation
“…In this respect 522 W of average output power with a combining efficiency of 93% was reported when using a surface grating [12]. With a reduced combining efficiency of 61% even 2 kW of power was shown [13]. Reaching these high output powers makes the combination of fiber lasers very attractive for certain applications.…”
Section: Introductionmentioning
confidence: 95%
“…In both cases mentioned above [12,13], lasers emitting around 1060 nm and spectrally spaced 2.5 nm to 5 nm were used. Using comparable diode lasers this could cause a serious reduction of performance due to heat effects when tuning their wavelengths by changing the laser temperatures.…”
Section: Introductionmentioning
confidence: 99%
“…최근에 는 비선형 현상과 더불어 모드 불안정 현상 또한 광섬유 레 이저의 출력을 제한하는 요소가 될 수 있다고 보고되고 있는 데 [11,[40][41][42][43][44][45][46][47][48] , 이는 광신호의 평균 출력에 따라 출력 빔 모드 특 성이 심각하게 왜곡되는 현상으로, 특히 광섬유의 코어가 크 고 그 유효 개구수(Numerical Apeture)가 낮으며 상대적으로 펌프광 흡수율이 높은 막대형 이득 광섬유(Rod-Type Gain Fiber)에서 더욱 현저히 발생한다 [41][42][43][44][45][46][47] . [49][50][51][52][53][54][55][56][57] . 최종적으로 제5장 에서는 앞으로의 고출력 광섬유 레이저 기술에 대한 전망 및 발전 방향을 제시하며 본 논문의 논의를 마무리하고자 한다.…”
Section: 서 론unclassified
“…For example, YDFLs at wavelength ranges of 1010-1020 nm with narrow bandwidths can not only be frequency quadrupled to 25× nm for laser-induced fluorescence, optical refrigeration, semiconductor inspection and atomic trapping applications [3][4][5][6][7] but can also be used for tandem-pumping high-power C-band (1.06-1.12 µm) YDFLs, due to their smaller quantum defect which gives higher conversion efficiency and lower thermal load [8,9] . Moreover, as an outstanding pathway for achieving scalable high-power lasers with good beam quality, spectral beam combining (SBC) combines multiple lasers into a single beam for maximum output power [10][11][12][13][14][15][16][17] . To date, the most common wavelength range for SBC is from 1050 to 1080 nm.…”
Section: Introductionmentioning
confidence: 99%