Table 1 Comparative analysis of sliding ferroelectric materials, including phase, stacking type, number of layers, space/point group, polarization intensity, strategies for breaking inversion symmetry, characterization techniques used
From: Emerging frontiers in two-dimensional sliding ferroelectrics
Material | Phase | Stacking | Number of layers | Space/point group | Polarization intensity | Strategy | Characterization techinique | Ref. |
|---|---|---|---|---|---|---|---|---|
hBN |  | parallel | 2 |  | P2D = 2.25 (0.37) × 10-12 C m-1 | noncentrosymmetric stacking | vertical PFM | |
hBN |  | parallel | 2 |  | PZ/A = 0.33 Debye/nm2 | noncentrosymmetric stacking | KPFM | |
hBN | Â | Bernal-type | multi | Â | 3.01 Debye/nm2 | noncentrosymmetric stacking | KPFM, PUND | |
graphene | Â | Bernal and rhombohedral | >3 | Â | 0.32 pC/m | noncentrosymmetric stacking | Â | |
hBN |  |  | 7/90 nm |  |  | twist | PFM | |
hBN/graphene |  | rhombohedral | 3 |  | 1.76 μC/cm2 | heterostructure | device | |
graphene | Â | Bernal | 2 | Â | 5 pC/m | Â | FTJ | |
MoS2 | 2H |  | 2 |  | d33 = 37.54 pm/V | strain | PFM, FTJ, C-AFM | |
MoS2 | 3 R | rhombohedral | 2 | P3m1 | 0.8-1.5 pC/m | photoexcitation |  | |
MoS2/WS2 |  | 3R-like and 2H-like | 2 | 3 m | d33 = 1.95-2.09 pm/V | heterostructure | PFM | |
MoS2 | 3 R | rhombohedral | 2 | C3v |  | stacking | device | |
CCC |  |  |  | P21 | 0.3-0.4 μC/cm2 | hybrid crystal | PFM | |
HgI2 |  |  |  | Cmc21 | 0.16 μC/cm2 |  | theoretical | |
NbI4 |  |  |  | Cmc21 | 0.11 μC/cm2 |  | theoretical | |
kagome-B2X3 (X = S, Se, Te) |  |  | 2 | \(P\bar{6}2m\), P1, P321, Cm, C2 |  |  | theoretical | |
ZrI2 |  |  | 2 | Pmn21 | 0.39 μC/cm2 |  | theoretical | |
β-ZrI2 |  |  |  | C1h |  |  | theoretical |