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Second-order nonlinearity of doped H:SiO2 films prepared by Matrix Distributed Electron Cyclotron Resonance and irradiated by electron beam

Q. LIU1,* , X. LU1, B. POUMELLEC2, G. GIRARD3, J.-E. BOURÉE3, P. BULKIN3, B. DREVILLON3, A. KUDLINSKI4, Y. QUIQUEMPOIS4, H. ZEGHLACHE4, G. MARTINELLI4

Affiliation

  1. Key Laboratory of Silicate Materials Science and Engneering (Wuhan University of Technology), Ministry of Education, Wuhan, Hubei 430070, P.R. China
  2. Laboratoire de Physico-Chimie de l'Etat Solide, UMR CNRS-UPS 8648, Université de Paris Sud, Bât. 414, 91405, Orsay Cedex, France
  3. Laboratoire de Physique des interfaces et couches minces, Ecole polytechnique, 91128 Palaiseau France
  4. Laboratoire de Physique, Laser, Atomes et Molécules, UMR CNRS-USTL , UMR CNRS-USTL 8523, Bât. P5, Université des Sciences et Technologies de Lille, 59655 Villeneuve d'Ascq, France

Abstract

Amorphous N-doped H:SiO2 films on silica prepared by Matrix Distributed Electron Cyclotron Resonance method were irradiated by electron-beam with different doses. With Maker fringe measurements, second-harmonic generation was observed in the irradiated regions and the films exhibited a maximum second-harmonic signal under the 5 μA/cm2, 480s irradiation condition. The magnitude of the induced second order nonlinear coefficient d33 is of the order of 0.003 pm/V. The d33 is small but the striking feature is the observation of a surface level shift connected to electron-beam poling with topography measurements. The surface level shifts increased with the increasing of electron doses in both X and Y directions, which fact was related to the implanted electron, dose. With different temperature for an annealing time of 1/2h, the surface level shifts in both X and Y directions increases firstly and got the maximum change at 300 °C, and then decreases when the temperature was increased. In the same time, the second-harmonics (SH) signal decreased to zero. The surface was recovered at the temperature of 1250 °C, which means that there was no matter loss with electron-beam writing in the films. The second harmonic generation in the films is caused by the frozen-in electric field induced by the charge implantation from the electron-beam (second order non linear coefficient χ(2) is proportional to this electric field). The strength of the electric field is determined by two conditions: the trapping centers (numbers, depth) and the remaining conductivity under large electric field.

Keywords

Amorphous films, Electron irradiation, Second-harmonic generation, optical switching.

Citation

Q. LIU, X. LU, B. POUMELLEC, G. GIRARD, J.-E. BOURÉE, P. BULKIN, B. DREVILLON, A. KUDLINSKI, Y. QUIQUEMPOIS, H. ZEGHLACHE, G. MARTINELLI, Second-order nonlinearity of doped H:SiO2 films prepared by Matrix Distributed Electron Cyclotron Resonance and irradiated by electron beam, Optoelectronics and Advanced Materials - Rapid Communications, 1, 5, May 2007, pp.197-201 (2007).

Submitted at: Feb. 28, 2007

Accepted at: April 5, 2007