By Vassilis L. Aravantinos
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See also Chapter 6 by Rupper, Kwong and Binder. Semiconductors should achieve a higher cooling power density than RE materials. The maximum cooling power density (rate of heat removal) is W N ~ kB T/τr , where N is the photoexcited electron (hole) density and τr is the radiative recombination time. In semiconductors, the optimal density N is limited due to many-body processes and does not exceed that of moderately doped RE systems. 8 (a) Cooling cycle in the laser refrigeration of a semiconductor in which the absorption of laser photons with energy hν creates a cold distribution of electron–hole carriers (only the electron distribution is shown for clarity).
A New Inscribed Kioniskos from Thebes by Vassilis L. Aravantinos