Semiconductor lasers with low operating voltage and high power conversion efficiency
A technology of working voltage and conversion efficiency, which is applied in the direction of semiconductor lasers, lasers, laser components, etc., can solve the problems of high working voltage and low power conversion efficiency, reduce the working voltage, reduce the recombination rate, and suppress the generation of dark line defects Effect
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Embodiment 1
[0037] In this embodiment, the substrate 1 is a Si-doped GaAs (100) single crystal substrate with a 15° bias to the crystal orientation, and the doping concentration is 2×10 18 cm -3 ; The buffer layer 2 is Si-doped GaAs with a thickness of 300nm, and the doping concentration is 1×10 18 cm -3 ; The lower confinement layer 3 is Si doped with a thickness of 1.2 μm (Al 0.3 Ga 0.7 ) 0.5 In 0.5 P, the doping concentration is 1×10 18 cm -3 ; The lower waveguide layer 4 is weak N-type Si-doped Ga with a thickness of 500nm 0.5 In 0.5 P, the doping concentration is 8×10 16 cm -3 ; The quantum well 5 is GaAsP with a thickness of 10nm; the upper waveguide layer 6 is non-doped Ga with a thickness of 300nm 0.5 In 0.5 P; The band gap gradient transition layer 7 is (Al 0.05 Ga 0.95 ) 0.5 In 0.5 The P composition gradually changes to (Al 0.3 Ga 0.7 ) 0.5 In 0.5 P; the upper confinement layer 8 is Mg doped with a thickness of 1.2 μm (Al 0.3 Ga 0.7 ) 0.5 In 0.5 P, the d...
Embodiment 2
[0040] The difference between this embodiment and Embodiment 1 is that the bandgap transition layer 10 has two layers, which are Ga 0.5 In 0.5 P and Ga with a thickness of 20nm 0.75 In 0.25 As 0.5 P 0.5 . The conduction band structure of the P-type region of the semiconductor laser of this embodiment is as image 3 shown.
[0041] Ga 0.5 In 0.5 As a band gap transition layer, P can reduce the energy band discontinuity value of the heterojunction interface. But Ga 0.5 In 0.5 The bandgap difference between P and GaAs is still close to 0.5eV, especially its valence band is above 0.3eV. Due to the limitation of the material system, Ga 0.5 In 0.5 The P / GaAs interface cannot use a bandgap gradient transition layer, and can only achieve a step change in the bandgap by inserting an intermediate bandgap layer to reduce its energy band discontinuity. Ga 0.75 In 0.25 As 0.5 P 0.5 The band gap is about 1.66eV, which happens to be in the Ga 0.5 In 0.5 The gap between P ...
Embodiment 3
[0043] The difference between this embodiment and Embodiment 1 is that the bandgap transition layer 10 has four layers, which are respectively Ga 0.5 In 0.5 P, Ga with a thickness of 20nm 0.625 In 0.375 As 0.25 P 0.75 , Ga with a thickness of 20nm 0.75 In 0.25 As 0.5 P 0.5 and Ga with a thickness of 20nm 0.875 In 0.125 As 0.75 P 0.25 . The conduction band structure of the P-type region of the semiconductor laser of this embodiment is as Figure 4 shown. Ga 0.5 In 0.5 A three-layer GaInAsP structure is inserted between P and GaAs, which are Ga 0.625 In 0.375 As 0.25 P 0.75 (1.77eV), Ga 0.75 In 0.25 As 0.5 P 0.5 (1.66eV) and Ga 0.875 In 0.125 As 0.75 P0.25 (1.54eV), which can further reduce the Ga 0.5 In 0.5 Band discontinuity values at the P / GaAs heterojunction interface.
[0044] The semiconductor lasers in the above three embodiments all use the bandgap graded structure to reduce the energy band discontinuity value of the AlGaInP / GaInP heterojun...
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