High-power external-cavity optically-pumped semiconductor lasers

Inactive Publication Date: 2002-02-28
COHERENT INC
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  • Abstract
  • Description
  • Claims
  • Application Information

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Problems solved by technology

While one of these characteristic wavelengths may be adequate for a particular application, it may not be the optimum wavel

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  • High-power external-cavity optically-pumped semiconductor lasers
  • High-power external-cavity optically-pumped semiconductor lasers
  • High-power external-cavity optically-pumped semiconductor lasers

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radiation having a wavelength half of the fundamental wavelength.

[0013] The laser-resonator, the optically nonlinear-crystal, the OPS-structure, the heat-sink arrangement and the optical pump-light-delivering arrangement are selected and arranged such that the resonator delivers the frequency-doubled radiation as output-radiation having a wavelength between about 212 nanometers and 900 nanometers at an output-power greater than about 100 milliwatts. The laser preferably has a resonator length greater than about 5.0 cm

[0014] In one embodiment of a high-power OPS-laser in accordance with the present invention, stable, single axial-mode, CW laser output-power of about 4.0 W at 488 nm wavelength is achieved by intracavity frequency-doubling 976 nm radiation from a single OPS-structure using an optically-nonlinear crystal of lithium triborate (LBO) in a resonator having a length of about twenty-five centimeters (cm). The OPS-structure has active layers of an In.sub.0.18Ga.sub.0.82As comp...

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Abstract

External-cavity optically-pumped semiconductor lasers (OPS-lasers) including an OPS-structure having a mirror-structure surmounted by a surface-emitting, semiconductor multilayer (periodic) gain-structure are disclosed. The gain-structure is pumped by light from diode-lasers. The OPS-lasers can provide fundamental laser output-power of about two Watts (2.0 W) or greater. Intracavity frequency-converted arrangements of the OPS-lasers can provide harmonic laser output-power of about one-hundred milliwatts (100 mW) or greater, even at wavelengths in the ultraviolet region of the electromagnetic spectrum. These high output powers can be provided even in single axial-mode operation. Particular features of the OPS-lasers include a heat sink-assembly for cooling the OPS-structure, a folded resonator concept for providing optimum beam size at optically-nonlinear crystals used for frequency conversion, preferred selection of optically-nonlinear materials for frequency-conversion, and compound resonator designs for amplifying second harmonic-radiation for subsequent conversion to third or fourth harmonic radiation.

Description

[0001] The present invention relates in general to external-cavity optically-pumped semiconductor lasers (hereinafter, OPS-lasers) including a surface-emitting, semiconductor multilayer (periodic) gain-structure. The invention relates in particular to arrangements of such lasers which can provide fundamental laser output-power of about two Watts (2.0 W) or greater, and intracavity frequency-converted arrangements of such lasers which can provide harmonic laser output-power of about one-hundred milliwatts (100 mW) or greater.DISCUSSION OF BACKGROUND ART[0002] The term OPS-lasers, as used herein, refers to a class of vertical-cavity surface-emitting semiconductor lasers wherein optical gain is provided by recombination of electrical carriers in very thin layers, for example, about 150 Angstrom units (.ANG.) or less, of a semiconductor material. These layers are generally termed quantum-well (QW) layers or active layers.[0003] In an OPS-laser, several QW layers, for example, about fift...

Claims

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Application Information

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IPC IPC(8): H01S3/08H01S3/108H01S3/109H01S5/024H01S5/04H01S5/06H01S5/14H01S5/183
CPCH01S3/07H01S3/0815H01S3/082H01S3/094053H01S3/09408H01S3/09415H01S3/105H01S3/1083H01S3/109H01S3/1095H01S3/139H01S5/02272H01S5/024H01S5/02423H01S5/02484H01S5/041H01S5/14H01S5/141H01S5/18383H01S5/0237
Inventor CAPRARA, ANDREACHILLA, JUAN L.SPINELLI, LUIS A.
Owner COHERENT INC
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