
CALCULATION OF STATIC PARAMETERS OF SILICON DIODE CONTAINING δ-LAYER OF TRIPLE-CHARGED POINT DEFECTS IN SYMMETRIC p–n-JUNCTION
Author(s) -
Н. А. Поклонский,
А. И. Ковалев,
Н. И. Горбачук,
С. В. Шпаковский
Publication year - 2018
Publication title -
pribory i metody izmerenij
Language(s) - English
Resource type - Journals
eISSN - 2414-0473
pISSN - 2220-9506
DOI - 10.21122/2220-9506-2018-9-2-130-141
Subject(s) - diode , materials science , semiconductor , electron , silicon , crystallographic defect , current density , step recovery diode , atomic physics , condensed matter physics , depletion region , optoelectronics , physics , schottky diode , quantum mechanics
The study of semiconductor materials and devices containing a narrow layer of impurity atoms and/or intrinsic point defects of the crystal lattice is of fundamental and practical interest. The aim of the study is to calculate the electric parameters of a symmetric silicon diode, in the flat p–n- junction of which a δ-layer of point triple-charged t -defects is formed. Such a diode is called p–t–n -diode, similarly to p–i–n- diode. Each t- defect can be in one of the three charge states (−1, 0, and +1; in the units of the elementary charge). It is assumed that at room temperature all hydrogen-like acceptors in p -region and hydrogen-like donors in n- region are ionized. It was assumed that the cross-section for v- band hole capture on t- defects is greater than the cross-section for c -band electron capture on t- defects. The system of stationary nonlinear differential equations, which describe in the drift-diffusion approximation a migration of electrons and holes in semiconductors, is solved numerically. The static capacityvoltage and current-voltage characteristics of the silicon diode with nondegenerate regions of p and n- type of electrical conductivity are calculated for forward and reverse electric bias voltage. It is shown by calculation that in the p–t–n -diode containing the δ-layer of t -defects, at the forward bias a region of current density stabilization occurs. At the reverse bias the current density in such a diode is much greater than the one in a p–n -diode without t- defects. With the reverse bias the capacitance of the p–t–n- diode, in contrast to the p–n- diode, increases at first and then decreases.