1986
DOI: 10.1007/978-3-642-46580-2_36
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Optical Bistability in CdS and Related Materials

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1986
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Cited by 6 publications
(2 citation statements)
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“…8) this is quite hopeless in the excitonic spectral range, because saturation of absorption is dominating in CdS a t T = 300 K. The exciton broadening is so large that off-resonant operation and, by this, increasing absorption can be achieved only far away from the resonance (Urbach tail) and at high intensities. Increasing absorption hysteresis observed on cooled CdS (T = 7 K) a t intensity levels of 1 kW/cm2 has been attributed t o OB via a collosional broadening of the free exciton [122]. But this explanation is in contradiction with current theoretical results 1202, 1981.…”
mentioning
confidence: 72%
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“…8) this is quite hopeless in the excitonic spectral range, because saturation of absorption is dominating in CdS a t T = 300 K. The exciton broadening is so large that off-resonant operation and, by this, increasing absorption can be achieved only far away from the resonance (Urbach tail) and at high intensities. Increasing absorption hysteresis observed on cooled CdS (T = 7 K) a t intensity levels of 1 kW/cm2 has been attributed t o OB via a collosional broadening of the free exciton [122]. But this explanation is in contradiction with current theoretical results 1202, 1981.…”
mentioning
confidence: 72%
“…I n [113,120] closed hysteresis loops with sharp switch-on and -off have been observed a t intensities of 30 and 5 kW/cm2, respectively, consistent with the saturation intensity given before. I n [122] only switch-on has been found, but a t a much higher intensitiy of 1 MW/cm2. This is a result of the unreasonably long cavity length of 10 pm used.…”
Section: F Henkebercermentioning
confidence: 94%