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. 2021 Jan 28;11(1):2417.
doi: 10.1038/s41598-021-82159-7.

Charge transport mechanism in the forming-free memristor based on silicon nitride

Affiliations

Charge transport mechanism in the forming-free memristor based on silicon nitride

Andrei A Gismatulin et al. Sci Rep. .

Abstract

Nonstoichiometric silicon nitride SiNx is a promising material for developing a new generation of high-speed, reliable flash memory device based on the resistive effect. The advantage of silicon nitride over other dielectrics is its compatibility with the silicon technology. In the present work, a silicon nitride-based memristor deposited by the plasma-enhanced chemical vapor deposition method was studied. To develop a memristor based on silicon nitride, it is necessary to understand the charge transport mechanisms in all states. In the present work, it was established that the charge transport in high-resistance states is not described by the Frenkel effect model of Coulomb isolated trap ionization, Hill-Adachi model of overlapping Coulomb potentials, Makram-Ebeid and Lannoo model of multiphonon isolated trap ionization, Nasyrov-Gritsenko model of phonon-assisted tunneling between traps, Shklovskii-Efros percolation model, Schottky model and the thermally assisted tunneling mechanisms. It is established that, in the initial state, low-resistance state, intermediate-resistance state and high-resistance state, the charge transport in the forming-free SiNx-based memristor is described by the space charge limited current model. The trap parameters responsible for the charge transport in various memristor states are determined.

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Conflict of interest statement

The authors declare no competing interests.

Figures

Figure 1
Figure 1
Ellipsometric mapping of refractive index n and thickness d of p+-Si/SiNx/Ni memristor structure (hν = 1.96 eV).
Figure 2
Figure 2
I–V characteristics of p+-Si/SiNx/Ni memristor cycles.
Figure 3
Figure 3
(a) Endurance of p+-Si/SiNx/Ni memristor cycles. (b) Retention of p+-Si/SiNx/Ni memristor cycles at 85 °C.
Figure 4
Figure 4
I–V characteristics of p+-Si/SiNx/Ni in VS, IRS, LRS and HRS at different temperatures in a double logarithmic scale.
Figure 5
Figure 5
I–V characteristics and of p+-Si/SiNx/Ni and simulation by SCLC model in (a) VS, (b) LRS, (c) IRS, (d) HRS.

References

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