2021
DOI: 10.1088/1361-6528/ac1ebe
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Effect of ferroelectric and interface films on the tunneling electroresistance of the Al2O3/Hf0.5Zr0.5O2 based ferroelectric tunnel junctions

Abstract: Ferroelectric random-access memory (FRAM) based on conventional ferroelectric materials is a non-volatile memory with fast read/write operations, high endurance, and 10 years of data retention time. However, it suffers from destructive read-out operation and lack of CMOS compatibility. HfO 2 -based ferroelectric tunnel junctions (FTJ) may compensate for the shortcomings of FRAM by its CMOS compatibility, fast operation speed, and non-destructive readout operation. In this study, we investigate the effect of fe… Show more

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Cited by 4 publications
(3 citation statements)
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“…However, when the pulse interval was 1 s, the maximum value of the current returned to 92.70% of the initial set. Moreover, in the case of [84] HZO (12 nm) Al 2 O 3 (2 nm) Ti/p þ Si 5 Ryu et al [40] HZO (8.4 nm) Al 2 O 3 (1 nm) TiN/p þ Ge 14 Shekhawat et al [85] HZO (6 nm) None TiN/p þ Ge 30 Goh et al [25] HZO (12 nm) Al 2 O 3 (1 nm) TiN/p þ Ge 78 Shekhawat et al [85] HZO (4.5 nm) None TiN/p þ Si 80 Mikheev et al [86] HAO (8 nm) None TiN/n þ Si 120 This work 2 s, it returned to 97.26%. As the gap between pulses increased, it could be interpreted that local switching occurred, as the polarization vectors aligned by the first pulse were returned by the depolarization field (E dep ).…”
Section: Resultsmentioning
confidence: 99%
“…However, when the pulse interval was 1 s, the maximum value of the current returned to 92.70% of the initial set. Moreover, in the case of [84] HZO (12 nm) Al 2 O 3 (2 nm) Ti/p þ Si 5 Ryu et al [40] HZO (8.4 nm) Al 2 O 3 (1 nm) TiN/p þ Ge 14 Shekhawat et al [85] HZO (6 nm) None TiN/p þ Ge 30 Goh et al [25] HZO (12 nm) Al 2 O 3 (1 nm) TiN/p þ Ge 78 Shekhawat et al [85] HZO (4.5 nm) None TiN/p þ Si 80 Mikheev et al [86] HAO (8 nm) None TiN/n þ Si 120 This work 2 s, it returned to 97.26%. As the gap between pulses increased, it could be interpreted that local switching occurred, as the polarization vectors aligned by the first pulse were returned by the depolarization field (E dep ).…”
Section: Resultsmentioning
confidence: 99%
“…The majority of papers concentrate on methods for enhancing TER effects through the engineering of device structure, [51][52][53] ferroelectric barrier, [54][55][56] and interfacial characteristics. [51,[57][58][59][60][61] Additionally, some prospective uses for fluorite FTJ have been introduced. [62][63][64][65] However, the review paper that systematically organizes all fluorite ferroelectric FTJ in terms of physics, structure, applications, and device difficulties has not yet been published, despite the fact that there have been many investigations of fluorite FTJ.…”
Section: Introductionmentioning
confidence: 99%
“…Wang et al experimentally obtained quite an enhanced TER effect for a CB-FTJ system with the composite barrier consisting of a perovskite BaTiO 3 (BTO) ferroelectric and a nonpolar dielectric (quantum Para electric) SrTiO 3 (STO) [29]. A 12 nm thick Hf 0.5 Zr 0.5 O 2 in contact with a 1 nm Al 2 O 3 interface layer was reported to exhibit an ON/OFF current ratio of 78 [30]. A metalferroelectric-insulator-semiconductor (MFIS) composite structure in a Si-doped HfO 2 -based FTJ was proposed to maximize the TER effect [31].…”
Section: Introductionmentioning
confidence: 99%