Gain properties of dye-doped polymer thin films

I. Gozhyk, M. Boudreau, H. Rabbani Haghighi, N. Djellali, S. Forget, S. Chénais, C. Ulysse, A. Brosseau, R. Pansu, J.-F. Audibert, S. Gauvin, J. Zyss, and M. Lebental
Phys. Rev. B 92, 214202 – Published 8 December 2015

Abstract

Hybrid pumping appears as a promising compromise in order to reach the much coveted goal of an electrically pumped organic laser. In such configuration the organic material is optically pumped by an electrically pumped inorganic device on a chip. This engineering solution requires therefore an optimization of the organic gain medium under optical pumping. Here, we report a detailed study of the gain features of dye-doped polymer thin films. In particular we introduce the gain efficiency K, in order to facilitate comparison between different materials and experimental conditions. The gain efficiency was measured with a variety of experimental methods (pump-probe amplification, variable stripe length method, laser thresholds) in order to study several factors which modify the actual gain of a layer, namely the confinement factor, the pump polarization, the molecular anisotropy, and the re-absorption. For instance, for a 600-nm-thick 5-wt % DCM doped poly(methyl methacrylate) (PMMA) layer, the different experimental approaches give a consistent value of K80cmMW1. On the contrary, the usual model predicting the gain from the characteristics of the material leads to an overestimation by two orders of magnitude, which raises a serious problem in the design of actual devices. In this context, we demonstrate the feasibility to infer the gain efficiency from the laser threshold of well-calibrated devices. Temporal measurements at the picosecond scale were carried out to support the analysis.

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  • Received 16 July 2015

DOI:https://doi.org/10.1103/PhysRevB.92.214202

©2015 American Physical Society

Authors & Affiliations

I. Gozhyk1,2, M. Boudreau1,6, H. Rabbani Haghighi3, N. Djellali1, S. Forget3, S. Chénais3, C. Ulysse4, A. Brosseau5, R. Pansu5, J.-F. Audibert5, S. Gauvin6, J. Zyss1, and M. Lebental1

  • 1Laboratoire de Photonique Quantique et Moléculaire, ENS Cachan, CentraleSupélec, CNRS, Université Paris-Saclay, 94235 Cachan, France
  • 2Surface du Verre et Interfaces, UMR 125 CNRS/Saint-Gobain Recherche, 39 quai Lucien Lefranc, 93303 Aubervilliers, France
  • 3Laboratoire de Physique des Lasers, Université Paris 13 and CNRS UMR 7538, 99 Avenue Jean-Baptiste Clement, F-93430 Villetaneuse, France
  • 4Laboratoire de Photonique et Nanostructures, CNRS UPR20, Route de Nozay, F-91460 Marcoussis, France
  • 5Laboratoire de Photophysique et Photochimie Supramoléculaires et Macromoléculaires, CNRS UMR 8531, Institut d'Alembert FR 3242, Ecole Normale Supérieure de Cachan, F-94235 Cachan, France
  • 6Groupe de Recherche sur les Couches Minces et la Photonique, Département de Physique et d'Astronomie, Université de Moncton, Moncton, New Brunswick, Canada E1A 3E9

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Vol. 92, Iss. 21 — 1 December 2015

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