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Mechanism of Current Performance in Thin-Film Heterojunctions n-CdS/p-Sb2Se3 Obtained by the CMBD Method

T.M. RazykovPhysical and Technical Institute of the Academy of Sciences of the Republic of Uzbekistan, Tashkent, UzbekistanК. M. KuchkarovPhysical and Technical Institute of the Academy of Sciences of the Republic of Uzbekistan, Tashkent, UzbekistanА.А. НасировNational University of Uzbekistan, University named after Mirzo Ulugbek, Tashkent, UzbekistanM. PirimmatovPhysical and Technical Institute of the Academy of Sciences of the Republic of Uzbekistan, Tashkent, UzbekistanР. ХуррамовPhysical and Technical Institute of the Academy of Sciences of the Republic of Uzbekistan, Tashkent, UzbekistanR. T. YuldoshovPhysical and Technical Institute of the Academy of Sciences of the Republic of Uzbekistan, Tashkent, UzbekistanD. Z. IsakovPhysical and Technical Institute of the Academy of Sciences of the Republic of Uzbekistan, Tashkent, UzbekistanM. A. MakhmudovPhysical and Technical Institute of the Academy of Sciences of the Republic of Uzbekistan, Tashkent, UzbekistanSh.M. BobomuradovPhysical and Technical Institute of the Academy of Sciences of the Republic of Uzbekistan, Tashkent, UzbekistanK.F. ShakhriyevPhysical and Technical Institute of the Academy of Sciences of the Republic of Uzbekistan, Tashkent, Uzbekistan; National University of Uzbekistan, University named after Mirzo Ulugbek, Tashkent, Uzbekistan
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Abstract

In this work, we analyzed the temperature dependence of the current-voltage characteristics of the structure of glass/Mo/p-Sb2Se3/n-CdS/In. From an analysis of the temperature dependences of the direct branches of the I-V characteristic of the heterojunction, it was established that the dominant mechanism of current transfer at low biases (3kT/e<V<0.8V) is multi-stage tunneling-recombination processes involving surface states at the Sb2Se3/CdS interface. At V>0.8 V, the dominant current transfer mechanism is Newman tunneling. In the case of reverse bias (3kT/e<V<1.0 eV), the main mechanism of charge carrier transfer through a heterojunction is tunneling through a potential barrier involving a deep energy level. At higher reverse voltages, a soft breakdown occurs.

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