2004
DOI: 10.1364/opex.12.003967
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Monolithically-integrated long vertical cavity surface emitting laser incorporating a concave micromirror on a glass substrate

Abstract: We present a fully monolithically integrated long vertical cavity surface emitting laser using an InGaAs/GaAs/AlGaAs gain medium directly bonded to a glass substrate with a concave micromirror. The lasing wavelength is 980nm with a threshold of 20mA for a 52microm mesa, differential quantum efficiency of 58%, and maximum output power of 39mW.

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Cited by 22 publications
(9 citation statements)
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“…Achieving lateral optical confinement could lead to smaller current apertures than ever before. The beam shape formed on the plane mirror in this type of cavity can be calculated using the following formula based on classical Gaussian optics 19 , where σ is the standard deviation of the Gaussian profile, n is the equivalent refractive index of the cavity medium, L is the cavity length, and R is the radius of curvature of the curved mirrors. Thus formula predict a beam waist can be controlled by L and R of a cavity.…”
Section: Introductionmentioning
confidence: 99%
“…Achieving lateral optical confinement could lead to smaller current apertures than ever before. The beam shape formed on the plane mirror in this type of cavity can be calculated using the following formula based on classical Gaussian optics 19 , where σ is the standard deviation of the Gaussian profile, n is the equivalent refractive index of the cavity medium, L is the cavity length, and R is the radius of curvature of the curved mirrors. Thus formula predict a beam waist can be controlled by L and R of a cavity.…”
Section: Introductionmentioning
confidence: 99%
“…The single-pulse laser ablation was carried out in c-Si and ChHG samples S with laser pulses of different energy Ep varying from 5 to 30 μJ at different positions   (± 400 μm) of the focal plane of the lens L relative to the surface of the sample S ( Fig.1a). Specific pulse energy was set by rotating the polarization plane of the laser beam with a /2 retardation plate placed before the Glan prism G. Apart from the angular position of the crystal axis of the 2 plate, the pulse total energy and energy distribution at the focal spot of the lens L (3.7×, 0.11 NA, F  3.4 cm), (so called Airy pattern, which is formed as a result of diffraction on the aperture A [17]) depend on the diameter D of the aperture A (varied from 1 to 3 mm) before the lens L. The radial intensity distribution I(r) in the Airy pattern is described by the square of the Bessel function of the first kind J1 as I(r)  (2J1(x)/x) 2 ,where x rD/F with D as the aperture diameter,  -wavelength, and F  3.4 cm -focal distance of the lens. The central part of the distribution I(r) between the first zeros of the Bessel function contains  95% of the total energy of the pulse.…”
Section: Resultsmentioning
confidence: 99%
“…They trap micro-particles, particularly biological cells, in focal spot area, increasing thereby the speed and performance of the relevant studies [1]. Microlaser resonators can be built using concave micromirrors [2], making them an important constituent of adaptive optics, telecom systems and matrix laser displays [3].…”
Section: Introductionmentioning
confidence: 99%
“…Much longer cavities may be reached in vertical extended−cavity surface−emitting lasers with monolithic integration of dielectric DBR micromirrors [48][49][50], how− ever, those devices are beyond the scope of the present paper.…”
Section: Diffraction Lossesmentioning
confidence: 99%