We examine the effects of nonradiative losses on lasing in crystalline and amorphous organic thin films. In crystalline films, the dominant loss mechanism is singlet-singlet annihilation, and this must be avoided if lasing is to be achieved at practical current densities. The electrically pumped crystalline-tetracene laser structure of Sch\"on et al. [Science 289, 599 (2000)] is studied in detail. Optical and electrical confinement in the bulk structure appears unable to explain the spectral narrowing reported; consequently, we consider electron-hole plasmas, self-focusing at interfaces, and crystal defects as possible sources of the reported phenomena. In amorphous films, lasers are likely to have to operate at current densities J<1000A/cm² due to a combination of nonradiative losses. The performance of potential lasing materials is quantified by the external quantum efficiency-current--density product, ηEXTJ. Electrically pumped lasers require ηEXTJ~5A/cm²; the best amorphous devices currently posses ηEXTJ~0.3A/cm². However, we demonstrate that electrically pumped lasing in amorphous materials should be possible using indirect pumping techniques.
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Baldo et al. (2002) studied this question.
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