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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Baldo, M. A.
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article
Prospects for electrically pumped organic lasers
Abstract
<p>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 Schön 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 < 1000 A/cm<sup>2</sup> due to a combination of nonradiative losses. The performance of potential lasing materials is quantified by the external quantum efficiency-current-density product, η<sub>EXT</sub>J. Electrically pumped lasers require η<sub>EXT</sub>J∼5 A/cm<sup>2</sup>; the best amorphous devices currently posses η<sub>EXT</sub>J∼0.3 A/cm<sup>2</sup>. However, we demonstrate that electrically pumped lasing in amorphous materials should be possible using indirect pumping techniques.</p>