2021
DOI: 10.1039/d0mh01863e
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Layer-dependent ferroelectricity in 2H-stacked few-layer α-In2Se3

Abstract: Atomically thin two-dimensional (2D) van der Waals materials have exhibited many exotic layer-dependent physical properties including electronic structure, magnetic order, etc. Here, we report a striking even-odd layer dependent oscillation...

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Cited by 42 publications
(35 citation statements)
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“…1c and Fig. S2 show the clear IP and OOP PFM phase contrast after writing two square patterns by applying ±5 V direct current (DC) tip bias consecutively, indicating the polarization reversal and interlocked ferroelectricity [16,17]. The same results also exist in a 19-nm-thick 2H α-In 2 Se 3 (Fig.…”
Section: Resultssupporting
confidence: 58%
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“…1c and Fig. S2 show the clear IP and OOP PFM phase contrast after writing two square patterns by applying ±5 V direct current (DC) tip bias consecutively, indicating the polarization reversal and interlocked ferroelectricity [16,17]. The same results also exist in a 19-nm-thick 2H α-In 2 Se 3 (Fig.…”
Section: Resultssupporting
confidence: 58%
“…At present, emerging 2D van der Waals (vdW) ferroelectrics may avert the above issues and enable nondestructive data reading and indefatigable data writing, thanks to their clean vdW interfaces and narrow-band-gap nature [12]. Among the known 2D vdW ferroelectric semiconductors, α-In 2 Se 3 possesses robust room-temperature ferroelectricity even down to the monolayer limit, and large-area samples can be grown using simple and low-cost preparation methods [14][15][16]. Moreover, the α-In 2 Se 3 ferroelectric has two different stacking constructions, namely hexagonal (2H) and rhombohedral (3R) structures [17][18][19].…”
Section: Introductionmentioning
confidence: 99%
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“…[34] According to the literature, IP ferroelectricity is thought to play a dominant role in this case. [35] In contrast, in this study, α-In 2 Se 3 was transferred after the electrodes were prepared in order to form vdW contacts. The currents in stages 2 and 3 of the hysteresis loops are higher than those in stages 1 and 4 (Figure S5, Supporting Information, and Figure 5a).…”
Section: Resultsmentioning
confidence: 96%
“…The α‐phase is ferroelectric with different ferroelectric properties for hexagonal (2H) and rhombohedral (3R) structures with AB and ABC stacking of the individual quintuple layer, respectively. [ 17–25 ] On the other hand, β‐In 2 Se 3 (3R) is not ferroelectric and can emerge under thermal annealing of α‐In 2 Se 3 . [ 26,27 ] Furthermore, superconductivity was reported in β‐In 2 Se 3 under high pressure due to phonon softening.…”
Section: Introductionmentioning
confidence: 99%