Short‐wavelength infrared defect emission as a probe of degradation processes in 980 nm single‐mode diode lasers

Infrared emission from 980-nm single-mode high power diode lasers is recorded and analyzed in the wavelength range from 0.8 to 8.0 μm. A pronounced short-wavelength infrared (SWIR) emission band with a maximum at 1.3 μm originates from defect states located in the waveguide of the devices. The SWIR intensity is a measure of the non-equilibrium carrier concentration in the waveguide, allowing for a non-destructive waveguide mapping in spatially resolved detection schemes. The potential of this approach is demonstrated by measuring spatially resolved profiles of SWIR emission and correlating them with mid-wavelength infrared (MWIR) thermal emission along the cavity of devices undergoing repeated catastrophic optical damage. The enhancement of SWIR emission in the damaged parts of the cavity is due to a locally enhanced carrier density in the waveguide and allows for an analysis of the spatial damage patterns. The figure shows a side view of a diode laser during catastrophic degradation as recorded by a thermocamera within 5 successive current pulses. The geometry of the device is given in grayscale. The position of the laser chip is indicated by the dotted line. The thermal signatures of the internal degradation of the diode laser are overlaid in color. The bi-directional spread of the damage along the laser cavity is clearly visible.

[1]  Thomas Elsaesser,et al.  Near-field dynamics of broad area diode laser at very high pump levels , 2011 .

[2]  A. Moser,et al.  Arrhenius parameters for the rate process leading to catastrophic damage of AlGaAs‐GaAs laser facets , 1992 .

[3]  E. Calleja,et al.  Origin of the near infrared luminescence in n-type AlxGa1-xAs alloys , 1991 .

[4]  M. Bettiati,et al.  Very high power operation of 980 nm single-mode InGaAs/AlGaAs pump lasers , 2006, SPIE LASE.

[5]  Thomas Elsaesser,et al.  Defect evolution during catastrophic optical damage of diode lasers , 2011 .

[6]  S. Sweeney,et al.  Direct measurement of facet temperature up to melting point and COD in high-power 980-nm semiconductor diode lasers , 2003 .

[7]  Thomas Elsaesser,et al.  Mechanisms and fast kinetics of the catastrophic optical damage (COD) in GaAs‐based diode lasers , 2011 .

[8]  A. Moser Thermodynamics of facet damage in cleaved AlGaAs lasers , 1991 .

[9]  J. W. Tomm,et al.  Microscopic Origins of Catastrophic Optical Damage in Diode Lasers , 2013, IEEE Journal of Selected Topics in Quantum Electronics.

[10]  Thomas Elsaesser,et al.  High single-spatial-mode pulsed power from 980 nm emitting diode lasers , 2012 .

[11]  H. J. Eichler,et al.  Internal defect localization in 980 nm ridge waveguide lasers , 2006, SPIE Photonics Europe.

[12]  Aland K. Chin,et al.  Failure-mode analysis of high-power single-mode 980-nm pump laser diodes , 2003, SPIE OPTO.

[13]  Thomas Elsaesser,et al.  Catastrophic optical damage at front and rear facets of diode lasers , 2010 .

[14]  T. Elsaesser,et al.  Time‐resolved reconstruction of defect creation sequences in diode lasers , 2012 .

[15]  S. M. Abbott,et al.  Measurement of spatial distribution of long‐wavelength radiation from GaAlAs injection lasers , 1979 .

[16]  U. Zeimer,et al.  Defect Propagation in Broad-Area Diode Lasers , 2012 .

[17]  Hajime Imai,et al.  Deep level associated with the slow degradation of GaAlAs DH laser diodes , 1978 .

[18]  Frank Bugge,et al.  Infrared emission from the substrate of GaAs-based semiconductor lasers , 2008 .

[19]  Lorenzo Pavesi,et al.  Photoluminescence of AlxGa1−xAs alloys , 1994 .

[20]  W. Lu,et al.  Modulated photoluminescence spectroscopy with a step-scan Fourier transform infrared spectrometer , 2006 .