Patent ID: 7613220
Filing Date: 2009-11-03
Classification: H01S

Abstract:
1. A two-wavelength semiconductor laser device having, integrated on a common substrate, a first infrared semiconductor laser and a second red semiconductor laser, each comprising a first conductivity type buffer layer, a first conductivity type cladding layer, a quantum well active layer, and a second conductivity type cladding layer and having a stripe geometry used for carrier injection, with the quantum well active layers in the vicinity of the cavity facets being disordered by impurity diffusion, wherein the first and second conductivity type cladding layers in the first infrared semiconductor laser and the second red semiconductor laser arc composed of an AlGaInP material, the active lever of the first infrared semiconductor laser is composed of an AlGaAs material including GaAs and the active layer of the second red semiconductor laser is composed of an AlGaInP material including InGaP, the buffer lever is composed of an AlGaAs material, the impurity is Zn, the cladding layers have a concentration of p-type impurity of 1×10 the AlGaAs materials composing the buffer layers of the first infrared semiconductor laser and the second red semiconductor laser satisfy the relationships expressed by the formulas, where X 1 is defined as a compositional ratio of A 1 in the first infrared semiconductor laser and X 2 as a compositional ratio of A 1 in the second red semiconductor laser, relationships expressed by the following formulas arc satisfied, where λ 1 is defined as an emission wavelength of an active layer of the first infrared semiconductor laser, λ 2 as an emission wavelength of the second red semiconductor laser, E 1 as a band gap energy of the buffer layer in the first infrared semiconductor laser, E 2 as a band gap energy of the buffer layer in the second red semiconductor laser, λb 1 as a wavelength corresponding to the band gap energy of the buffer layer in the first semiconductor infrared laser, and λb 2 as a wavelength corresponding to the band gap energy of the buffer layer in the second red semiconductor laser, and a thermal history imparted to the first infrared semiconductor laser is longer than a thermal history imparted to the second red semiconductor laser.