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Fizika i Tekhnika Poluprovodnikov, 2017 Volume 51, Issue 6, Pages 821–829 (Mi phts6141)

This article is cited in 8 papers

Semiconductor physics

$n$-ZnO/$p$-CuI barrier heterostructure based on zinc-oxide nanoarrays formed by pulsed electrodeposition and SILAR copper-iodide films

N. P. Klochkoa, V. R. Kopacha, G. S. Khrypunova, V. E. Korsuna, N. D. Volkovab, V. M. Lyubova, M. V. Kirichenkoa, A. V. Kopacha, D. O. Zhadana, A. N. Otchenashkoa

a Khar'kov Polytechnical University
b National Aerospace University "Kharkiv Aviation Institute"

Abstract: A $p$-CuI/$n$-ZnO barrier structure is investigated as a promising base diode structure for a semitransparent near-ultraviolet detector. We analyze the crystal structure and electrical and optical properties of zinc-oxide nanoarrays electrodeposited in the pulsed mode and copper-iodide films formed by the successive ionic layer adsorption and reaction (SILAR) method, which were used as the basis for an $n$-ZnO/$p$-CuI barrier heterostructure sensitive to ultraviolet radiation in the spectral range of 365–370 nm. Using the I–V characteristics, a shunting resistance of $R_{sh}\cdot S_c$ = 879 $\Omega$ cm$^2$, a series resistance of $R_s\cdot S_c$ = 8.5 $\Omega$ cm$^2$, a diode rectification factor of $K$ = 17.6, a rectifying $p$$n$-junction barrier height of $\Phi$ = 1.1 eV, and a diode ideality factor of $\eta$ = 2.4 are established. It is demonstrated that at low forward biases (0 $<U<$ 0.15 V), the effects of charge-carrier recombination and tunneling are equal. As the bias increases above 0.15 V, the tunneling–recombination transport mechanism starts working. The diode saturation current $J_0$ is found to be 6.4 $\times$ 10$^{-6}$ mA cm$^{-2}$ for recombination and tunneling charge-carrier transport and 2.7 $\times$ 10$^{-3}$ mA cm$^{-2}$ for tunneling–recombination charge-carrier transport.

Received: 16.11.2016
Accepted: 23.11.2016

DOI: 10.21883/FTP.2017.06.44563.8450


 English version:
Semiconductors, 2017, 51:6, 789–797

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