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49 P by linear interpolation
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a = 1014 cm-3, the electrons are the center minority carrier. As the p-doping is increased, the low density lifetime initially increases. Eventually, the center minority carrier becomes the holes, and then the low density lifetime decreases as the p-doping is increased
-
a = 1014 cm-3, the electrons are the center minority carrier. As the p-doping is increased, the low density lifetime initially increases. Eventually, the center minority carrier becomes the holes, and then the low density lifetime decreases as the p-doping is increased.
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17
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78751558668
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h (z) is very small. This results in almost no radiative recombination from these layers. Rather then calculate Beh and Bdh for GaInP, we ignore the tiny amount of radiative recombination that comes from the GaInP layers
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h (z) is very small. This results in almost no radiative recombination from these layers. Rather then calculate Beh and Bdh for GaInP, we ignore the tiny amount of radiative recombination that comes from the GaInP layers.
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