Origin and enhancement of the second-order non-linear optical susceptibility induced in bismuth borate glasses by thermal poling

被引:28
作者
Deparis, O
Mezzapesa, FP
Corbari, C
Kazansky, PG
Sakaguchi, K
机构
[1] Fac Polytech Mons, Electromagnetism & Telecommun Dept, B-7000 Mons, Belgium
[2] Univ Southampton, Optoelect Res Ctr, Southampton SO17 1BJ, Hants, England
[3] Nippon Sheet Glass Co Ltd, Tech Res Lab, Itami, Hyogo 6648520, Japan
关键词
D O I
10.1016/j.jnoncrysol.2005.06.004
中图分类号
TQ174 [陶瓷工业]; TB3 [工程材料学];
学科分类号
0805 ; 080502 ;
摘要
The second-order non-linear optical susceptibility of thermally poled glasses, chi((2)), should be enhanced in proportion to the intrinsic third-order susceptibility chi((3)), for a given frozen-in electric field (i.e. chi((2)) = 3E(dc)chi((3))). In order to test this prediction, bismuth-borate (Bi2O3-ZnO-B2O3) glasses, for which chi((3)) increased with increasing Bi2O3 content, were thermally poled and the second-order non-linear coefficient was determined. Poling conditions and current dynamics turned out to be very different from those in silica. Poling temperatures had to be relatively close to glass transition temperatures and the glass-electrode contact had to be intimate in order to induce the non-linearity which was located in a near-surface layer at the anode side. A poling mechanism was proposed which relied on proton migration, took into account ion injection and glass ionization, and was able to explain most of the experimental results. The chi((2)) values increased with increasing chi((3)) as predicted but did not exceed 0.7 pm/V. By comparison with silica, it was inferred that the dielectric breakdown strength E-b was lower in bismuth borate and decreased with increasing Bi2O3 content. This latter result demonstrated the importance to select glass compositions on the basis of both chi((3)) and E-b for the purpose of enhancing chi((2)). (c) 2005 Elsevier B.V. All rights reserved.
引用
收藏
页码:2166 / 2177
页数:12
相关论文
共 34 条
[11]   Practical technique for measurement of second-order nonlinearity in poled glass [J].
Corbari, C ;
Deparis, O ;
Klappauf, BG ;
Kazansky, PG .
ELECTRONICS LETTERS, 2003, 39 (02) :197-198
[12]   Enhanced stability of the second-order optical nonlinearity in poled glasses [J].
Deparis, O ;
Corbari, C ;
Kazansky, PG ;
Sakaguchi, K .
APPLIED PHYSICS LETTERS, 2004, 84 (24) :4857-4859
[13]   Dynamics of the second-order nonlinearity in thermally poled silica glass [J].
Faccio, D ;
Pruneri, V ;
Kazansky, PG .
APPLIED PHYSICS LETTERS, 2001, 79 (17) :2687-2689
[14]   ELECTROOPTIC MODULATION IN GERMANOSILICATE FIBER WITH UV-EXCITED POLING [J].
FUJIWARA, T ;
WONG, D ;
ZHAO, Y ;
FLEMING, S ;
POOLE, S ;
SCEATS, M .
ELECTRONICS LETTERS, 1995, 31 (07) :573-575
[15]   Inducing a large second-order optical nonlinearity in soft glasses by poling [J].
Garcia, FC ;
Carvalho, ICS ;
Hering, E ;
Margulis, W ;
Lesche, B .
APPLIED PHYSICS LETTERS, 1998, 72 (25) :3252-3254
[16]   Optical nonlinearity in fused silica by proton implantation [J].
Henry, LR ;
McGrath, BV ;
Alley, TG ;
Kester, JJ .
JOURNAL OF THE OPTICAL SOCIETY OF AMERICA B-OPTICAL PHYSICS, 1996, 13 (05) :827-836
[17]   MAKER FRINGES - A DETAILED COMPARISON OF THEORY AND EXPERIMENT FOR ISOTROPIC AND UNIAXIAL CRYSTALS [J].
JERPHAGNON, J ;
KURTZ, SK .
JOURNAL OF APPLIED PHYSICS, 1970, 41 (04) :1667-+
[18]   Glass fiber poling and applications [J].
Kazansky, PG ;
Russell, PS ;
Takebe, H .
JOURNAL OF LIGHTWAVE TECHNOLOGY, 1997, 15 (08) :1484-1493
[19]   THERMALLY POLED GLASS - FROZEN-IN ELECTRIC-FIELD OR ORIENTED DIPOLES [J].
KAZANSKY, PG ;
RUSSEL, PS .
OPTICS COMMUNICATIONS, 1994, 110 (5-6) :611-614
[20]   HIGH 2ND-ORDER NONLINEARITIES INDUCED IN LEAD SILICATE GLASS BY ELECTRON-BEAM IRRADIATION [J].
KAZANSKY, PG ;
KAMAL, A ;
RUSSELL, PSJ .
OPTICS LETTERS, 1993, 18 (09) :693-695