势垒层作为深中心的谐振器

P. T. Oreshkin
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引用次数: 4

摘要

本文对巴曼和列别捷夫的论文作了回应。Vyssh。Uchebn。Zaved。SSSR,饮料。, No. 12, 88-90(1989)),并表明给出的论据是不令人满意的。在Si的n+-p结中获得了新的实验数据,其中观察到方形反偏置脉冲U < Ures使DLTS峰移位。这里的Ures是脉冲的大小,在这个脉冲中,所有的激活-漂移过程都变成了激活-传输过程,势垒层作为一个新制备的谐振器在深中心工作(参见P. T. Oreshkin, elektronaya Tekhnika, Ser. 3, Mikroelektronika, No. 4(128), 12-20(1988))。
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Barrier layers as resonators on deep centers
A response is given to the paper of L. S. Barman and A. A. Lebedev (Izv. Vyssh. Uchebn. Zaved. SSSR, Fiz., No. 12, 88–90 (1989)), and it is shown that the arguments given there are not satisfactory. New experimental data have been obtained for n+-p junctions in Si, where square reverse-bias pulses U < Ures are observed to shift the DLTS peaks. Here Ures is the magnitude of the pulse for which all activation-drift processes become activation-transit processes and the barrier layer operates as a freshly prepared resonator on deep centers (see the paper by P. T. Oreshkin, Elektronnaya Tekhnika, Ser. 3, Mikroelektronika, No. 4 (128), 12–20 (1988).
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