Gain‐current relation for In0.72Ga0.28As0.6P0.4 lasers

The optical gain coefficient is calculated as a function of the nominal current density for In0.72Ga0.28As0.6P0.4 (λg=1.3 μm) using a Gaussian fit to the Halperin‐Lax band tails and Stern’s matrix element. The calculation is done for p‐type, n‐type and undoped material at 297 and 350 K respectively. The results show that n‐type layers may give lower threshold currents than do comparable p‐type layers. The gain or loss at the lasing frequency is found to be a nonlinear function of the injected carrier density so that regions of strong carrier depletion may act as saturable absorbers. The results show that the effect of the Fermi factors alone cannot explain the observed temperature dependence of threshold.

[1]  H. Casey,et al.  Concentration‐dependent absorption and spontaneous emission of heavily doped GaAs , 1976 .

[2]  R. Nelson Near‐equilibrium LPE growth of low threshold current density In1−xGaxAsyP1−y(λ=1.35 μm) DH lasers , 1979 .

[3]  H. Casey,et al.  Heterostructure lasers , 1978 .

[4]  D. Rode How much Al in the AlGaAs–GaAs laser? , 1974 .

[5]  Frank Stern,et al.  Calculated spectral dependence of gain in excited GaAs , 1976 .

[6]  John A. Copeland,et al.  Semiconductor-laser self pulsing due to deep level traps , 1978 .

[7]  L. A. Koszi,et al.  Pulsations and absorbing defects in (Al,Ga)As injection lasers , 1979 .

[8]  N.E. Schumaker,et al.  Ambipolar transport in double heterostructure injection lasers , 1980, IEEE Electron Device Letters.

[9]  H. C. Casey,et al.  Room‐temperature threshold‐current dependence of GaAs‐AlxGa1−xAs double‐heterostructure lasers on x and active‐layer thickness , 1978 .

[10]  Niloy K. Dutta,et al.  Temperature dependence of threshold and electrical characteristics of InGaAsP-InP d.h. lasers , 1980 .

[11]  T. Pearsall,et al.  An experimental determination of the effective masses for GaxIn1−xAsyP1−y alloys grown on InP , 1979 .

[12]  R. Nicholas,et al.  Cyclotron resonance and the magnetophonon effect in GaxIn1−xAsyP1−y , 1980 .

[13]  R. L. Barns,et al.  Band gap versus composition and demonstration of Vegard’s law for In1−xGaxAsyP1−y lattice matched to InP , 1978 .

[14]  Charles Howard Henry,et al.  Measurement of gain and absorption spectra in AlGaAs buried heterostructure lasers , 1980 .

[15]  Charles Howard Henry,et al.  Theory of defect‐induced pulsations in semiconductor injection lasers , 1980 .

[16]  C. Hwang,et al.  Threshold behavior of (GaAl)As‐GaAs lasers at low temperatures , 1978 .

[17]  B. Miller,et al.  GaAs–AlxGa1−xAs Double Heterostructure Lasers—Effect of Doping on Lasing Characteristics of GaAs , 1972 .

[18]  M. Horiguchi,et al.  Spectral losses of low-OH-content optical fibres , 1976 .

[19]  W. J. Turner,et al.  Refractive Index of InP , 1965 .

[20]  T. Paoli Changes in the optical properties of CW (AlGa)As junction lasers during accelerated aging , 1977 .

[21]  M. Takusagawa,et al.  Theoretical and experimental study of threshold characteristics in InGaAsP/InP DH lasers , 1979 .

[22]  M. Lax,et al.  Impurity-Band Tails in the High-Density Limit. I. Minimum Counting Methods , 1966 .

[23]  W. Wiegmann,et al.  Low-temperature absorption spectrum in GaAs in the presence of optical pumping , 1977 .

[24]  F. Stern Gain-current relation for GaAs lasers with n-type and undoped active layers , 1973 .

[25]  H. C. Casey,et al.  Evidence for low surface recombination velocity on n‐type InP , 1977 .

[26]  M. Umeno,et al.  Measurement of Diffusion Coefficient and Surface Recombination Velocity for p-InGaAsP Grown on InP , 1980 .

[27]  James N. Walpole,et al.  Self‐sustained pulsations in GaInAsP diode lasers , 1980 .

[28]  D. Payne,et al.  Zero material dispersion in optical fibres , 1975 .

[29]  N. Basov,et al.  Dynamics of injection lasers , 1968 .

[30]  W. Joyce,et al.  A possible model for sustained oscillations (pulsations) in (Al,Ga)As double-heterostructure lasers , 1979 .

[31]  F. Stern Band-Tail Model for Optical Absorption and for the Mobility Edge in Amorphous Silicon , 1971 .

[32]  K. Alavi,et al.  Oscillatory magneto-transmission of In1−xGaxAsyP1−yalloys , 1979 .

[33]  H. Störmer,et al.  Cyclotron resonance in n‐type In1−xGaxAsyP1−y , 1979 .

[34]  Y. Horikoshi,et al.  Temperature Sensitive Threshold Current of InGaAsP–InP Double Heterostructure Lasers , 1979 .

[35]  P. Lawaetz,et al.  Valence-Band Parameters in Cubic Semiconductors , 1971 .