2023
DOI: 10.1021/acsnano.3c02406
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Robust Threshold-Switching Behavior Assisted by Cu Migration in a Ferroionic CuInP2S6 Heterostructure

Abstract: The two-dimensional layered material CuInP 2 S 6 (CIPS) has attracted significant research attention due to its nontrivial physical properties, including room-temperature ferroelectricity at the ultrathin limit and substantial ionic conductivity. Despite many efforts to control its ionic conductance and develop electronic devices, such as memristors, improving the stability of these devices remains a challenge. This work presents a highly stable threshold-switching device based on the Cu/CIPS/graphene heterost… Show more

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Cited by 17 publications
(7 citation statements)
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“…To gain insight into the mechanism of resistive switching in the In/CuCrS 2 /Au device, we perform the temperature-dependent I–V sweep of an In/CuCrS 2 /Au device (Figure S6). As one can see, the on/off ratio becomes evident when heating to 200 K. When the temperature is <200 K, Cu ions are frozen in fixed sites by a potential well of [CuS 6 ] units, while Cu ions acquire enough energy to escape when it comes above 200 K. This is similar to the behavior of the Cu ion in ferroionic CuInP 2 S 6 . CuInP 2 S 6 has been proven to activate its ionic conductance pathways at 250 K. Consequently, we can attribute the sudden shift in conductivity (Figure c) to the defrosting of Cu ions. On the basis of the results presented above, we can see that the performance of the device is closely related to the movement of Cu ions.…”
mentioning
confidence: 59%
“…To gain insight into the mechanism of resistive switching in the In/CuCrS 2 /Au device, we perform the temperature-dependent I–V sweep of an In/CuCrS 2 /Au device (Figure S6). As one can see, the on/off ratio becomes evident when heating to 200 K. When the temperature is <200 K, Cu ions are frozen in fixed sites by a potential well of [CuS 6 ] units, while Cu ions acquire enough energy to escape when it comes above 200 K. This is similar to the behavior of the Cu ion in ferroionic CuInP 2 S 6 . CuInP 2 S 6 has been proven to activate its ionic conductance pathways at 250 K. Consequently, we can attribute the sudden shift in conductivity (Figure c) to the defrosting of Cu ions. On the basis of the results presented above, we can see that the performance of the device is closely related to the movement of Cu ions.…”
mentioning
confidence: 59%
“…Therefore, we have measured highresolution I-V switching curves of the Ag/SF/Au memristor (Figure 2g) and obtained an SS of less than 0.01 mV dec −1 , which is the smallest SS to the best of our knowledge (benchmarked in Figure 2h). [43][44][45][46][47][48][49][50][51][52] The pulse-mode measurement further showed a sub-100 ns resistive switching speed (Figure 2i), corresponding to a low operation energy of ≈14 pJ. The switching speed of Agbased memristors is mainly limited by the Ag ions' transport velocity in the insulating layer, which was controlled by the applied electric field.…”
Section: Resultsmentioning
confidence: 96%
“…These insights will help in strain engineering the ferroelectric properties , by tuning the CIPS composition. Furthermore, lattice strain can be an effective way to control the high ionic mobility of the Cu + ions under fields and, thereby, expand the breadth of device applications based on this unique and highly interesting layered ferroelectric material.…”
Section: Discussionmentioning
confidence: 99%