光折变InP:Fe在λ = 1.32µm时的净增益

J. Strait, J. D. Reed, A. Saunders, G. Valley, M. Klein
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引用次数: 9

摘要

增益是光折变效应中最吸引人的方面之一。当光折变增益超过吸收损耗时,相位共轭器和其他应用成为可能。半导体,如InP和GaAs,具有较小的电光系数,因此必须施加几kV/cm的电场才能实现大的增益。在InP:Fe中,首先用10 kV/cm的交流电场获得了3 cm-1的增益1,然后用8 kV/cm的直流电场获得了4 cm-1的增益2最近有报道称,在一个8kv /cm的直流电场中,增益可达6 cm-1虽然在没有应用领域的情况下不可能在InP:Fe中获得如此大的增益,但所需的高电压对于器件应用来说是不切实际的。
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Net Gain in Photorefractive InP:Fe at λ = 1.32 µm Without an Applied Field
Gain is one of the most attractive aspects of the photorefractive effect. Phase conjugators and other applications become possible when photorefractive gain exceeds absorption losses. Semiconductors, such as InP and GaAs, have small electro-optic coefficients, so it has been necessary to apply electric fields of several kV/cm to realize large gains. In InP:Fe, a gain of 3 cm-1 first was reported with a 10 kV/cm AC applied field1 and later a gain of 4 cm-1 was obtained with an 8 kV/cm DC field.2 Recently gains as large as 6 cm-1 have been reported for an 8 kV/cm DC field.3 While it is not possible to have such large gains in InP:Fe without an applied field, the high voltages required are not practical for device applications.
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