2010
DOI: 10.1049/el.2010.8909
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10.7 W peak power picosecond pulses from high-brightness photonic band crystal laser diode

Abstract: Using a monolithic photonic band crystal laser, nearly diffraction limited laser pulses of 10.7 W peak power at 980 nm wavelength and brightness of 4 × 10 8 Wcm 22 sr 21 are generated. These pulses of about 100 ps FWHM have a variable repetition rate of up to 80 MHz, making them ideal seed sources for optical power amplifiers.

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Cited by 13 publications
(5 citation statements)
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“…Experimentally, the characteristics close to those predicted were achieved with current pulses of an amplitude significantly lower than that used in previous work, though still greater than 10 A, due to the lasers used having a modest injection efficiency of about 0.5 [15]- [17]. Gain-switched laser designs with large d a /Γ a have also been demonstrated by other teams [18].…”
Section: Introductionsupporting
confidence: 78%
“…Experimentally, the characteristics close to those predicted were achieved with current pulses of an amplitude significantly lower than that used in previous work, though still greater than 10 A, due to the lasers used having a modest injection efficiency of about 0.5 [15]- [17]. Gain-switched laser designs with large d a /Γ a have also been demonstrated by other teams [18].…”
Section: Introductionsupporting
confidence: 78%
“…Thus inexpensive and temperature stable QD lasers available between 1260 and 1310 nm are ideal future sources for road illumination and LIDAR. They can be based on novel HIBBEE high brightness laser structures being astigmatism-free and showing a round far field for as much as 4.2 W cw and 17.7 W pulsed output power at 1060 nm, needing no complex focusing optics [38][39][40]. The last generation of these lasers is based on QDs.…”
Section: High-frequency Directly Modulated Qd Lasersmentioning
confidence: 99%
“…In the case of bulk or Quantum Well (QW) edge-emitting lasers, the large equivalent spot size can in principle be achieved in markedly asymmetric waveguide structures, which also have the advantage of supporting only a single fundamental transverse mode for any stripe width. By comparison with alternative high-power transmitter designs based on master oscillator optical power amplifiers or photonic band crystal laser diodes [23], [24], this has the advantage of a much simpler construction as well as promising better pulse performance. Moreover, the principle referred to above ðd act =À )Þ is a general one, implying that it works with all types of laser diodes.…”
Section: Introductionmentioning
confidence: 99%