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Electro-optic transceivers for terahertz-wave applications

✍ Scribed by Chen, Q.; Tani, M.; Jiang, Zhiping; Zhang, X.-C.


Book ID
115396357
Publisher
Optical Society of America
Year
2001
Tongue
English
Weight
353 KB
Volume
18
Category
Article
ISSN
0740-3224

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✦ Synopsis


Because of the reciprocal behavior of the optical rectification and the electro-optic effect in a nonlinear optical crystal, an electro-optic transceiver can alternately transmit pulsed electromagnetic radiation (optical rectification) and detect the return signal (electro-optic effect) in the same crystal. However, the optimal condition of the electro-optic transceiver may be very different from that of the spatially separated emitter and receiver. We present a detailed description of the crystal-orientation dependence of the electro-optic terahertz devices (transmitter, receiver, and transceiver). It is found that for a (110) zinc-blende electro-optical crystal, the efficiency of the electro-optic transceiver will be optimized when the angle between the polarization of the optical pump beam and the crystallographic z axis [0, 0, 1] is 26Β°. Meanwhile, for a (111) crystal, the angle between the optical beam and the crystallographic direction [Οͺ1, Οͺ1, 2] should be 23Β°. The experimental results from a (110) ZnTe transceiver verify theoretical calculations and demonstrate a direct way to optimize the working efficiency of an electro-optic terahertz transceiver.


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