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Light-Emitting Diodes

          112   Photonic Devices





































          Figure 6.6. The emission spectrum of a heterostructure LED with a peak emission
          wavelength near 1600 nm. This diode is a laboratory specimen, and is not commercially
          available. The active region is approximately one-half wavelength in thickness, and is
          surrounded by wider-band gap window materials. This allows the light to escape with-
          out being absorbed. Note that the emission spectrum corresponds more closely to that
          predicted by our simple model. Careful control over impurities has limited the longer
          wavelength tail. The half width of the emission is 60 eV, which is significantly narrow-
          er than that measured for the diodes in Figs. 6.4 and 6.5.



                      1

                               probability of radiative recombination
                       rr
              	 =          =                                          (6.8)
                   1    1    probability for all kinds of recombination
                     +
                     rr    nr
            There is no straightforward way to estimate the radiative recombi-
          nation time and the nonradiative recombination times from funda-
          mental parameters. In particular, the nonradiative recombination
          time usually depends on the density of defects in the material, which
          is not related to fundamental materials characteristics.




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