1991
DOI: 10.1109/3.135167
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High power, nearly diffraction-limited output from a semiconductor laser with an unstable resonator

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Cited by 81 publications
(16 citation statements)
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“…In a single broad-area laser diode element, an unstable resonator LD can have a single-peak FFP, but the power output is about several hundred milliwatts [9,10]. In addition, an α-DFB LD that places a diffraction grating at an angle with respect to the direction of light propagation can have a single-peak FFP at 1 W or higher [11].…”
Section: Introductionmentioning
confidence: 99%
“…In a single broad-area laser diode element, an unstable resonator LD can have a single-peak FFP, but the power output is about several hundred milliwatts [9,10]. In addition, an α-DFB LD that places a diffraction grating at an angle with respect to the direction of light propagation can have a single-peak FFP at 1 W or higher [11].…”
Section: Introductionmentioning
confidence: 99%
“…['i] As depicted in the figure, these resonators are characterized by diverging wavefronts, which we hope will counter the focusing effects of fllamentation. While unstable resonators, when used in conventional near-infrared semiconductor lasers, have led to high single-mode power [19], there are concerns regarding their ability to counter the stronger filamentation tendency in a nitride gain medium. Fiagure 11 compares the unstable resonator field distribution with that of the plane-plane resonator with uncoated facets.…”
Section: Unstable Resonatorsmentioning
confidence: 99%
“…One technique adopted from traditional nondiode lasers is the unstable resonator concept, such as lasers with a curved mirror resonator [4], [5]. Lasers with multiple sections have also been explored to increase the brightness, including master oscillator power amplifier (MOPA) lasers [6], tapered lasers [7], and bow-tie lasers [8].…”
Section: B Approaches For High Power and Brightnessmentioning
confidence: 99%