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On the basis of first-principles calculations, the structure, magnetism and ferroelectricity of VOBr2 monolayer are studied systematically in the present work. The calculation results indicate that a spontaneous ferroelectric distortion takes place at low temperature, causing the structure of VOBr2 to transform from a centrosymmetric paraelectric phase to a ferroelectric one. In contrast with its sister compound VOI2, the dimerization of V is unstable in VOBr2 and may quench the local magnetic moment on V ions. Additionally, the easy magnetization axis of VOBr2 monolayer is in-plane along the a-axis, and the magnetic coupling between adjacent local moments is antiferromagnetic both along the a-axis and along the b-axis. Moreover, the ferroelectric displacement of V ions occurs in the a-axis, along the V—O—V chains direction, resulting in a polarization of about 40 μC/cm2. Comparing with the ferro-to-paraelectric reversal pathway, the energy barrier can be effectively reduced for ferroelectric switching on partial or individual V—O—V chains. It is reasonable to believe that the dipole moment flipping on specific chain can be achieved through a moderate external field, thereby providing new direction for designing the low-energy-consumption and high-density ferroelectric memory device.
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Keywords:
- first-principles calculation /
- two-dimensional material /
- oxyhalide /
- magnetic and ferroelectric properties
[1] Novoselov K S, Jiang D, Schedin F, Booth T J, Khotkevich V V, Morozov S V, Geim A K 2005 P. Natl. Acad. Sci. USA 102 10451
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图 2 (a)单层VOBr2高对称相下2 × 2 × 1超胞的声子谱; (b), (c)声子谱虚频对应的两种二聚化畸变模式Dim1和Dim2; (d), (e)声子谱虚频对应的两种铁电畸变模式FE和AFE
Figure 2. (a) Calculated phonon spectrum of high symmetry VOBr2 2 × 2 × 1 supercell; (b), (c) two dimerization distortion modes Dim1 and Dim2; (d), (e) FE and AFE distortion modes, corresponding to the imaginary frequencies in the phonon spectrum.
图 5 (a)含磁优化计算考虑的4种常见磁序: FM表示近邻V离子自旋平行排列, 即铁磁序; aAbF表示近邻V离子自旋沿a轴反平行排列, 沿b轴平行排列; aFbA表示V离子自旋沿a轴平行排列, 沿b轴反平行排列; GAFM表示近邻V离子间自旋均反平行排列; (b) FE相GAFM磁基态下的投影态密度分布
Figure 5. (a) Four magnetic orders considered in the magnetic ground state calculations. FM denotes the spin parallel arrangement, aAbF denotes the antiferromagnetic (ferromagnetic) coupling between neighbouring V ions along a (b)-axis, aFbA represents the ferromagnetic (antiferromagnetic) coupling along a (b)-axis, and GAFM denotes the antiferromagnetic coupling between neighbouring V ions along both directions. (b) Projected DOS of the GAFM ground state within the FE structural phase.
表 1 含磁优化结果对比汇总表
Table 1. Summary of the main results of structural and magnetic optimization.
a, b/Å Ground state Local moment/μB Gap/eV Energy difference
/(eV·f.u.–1)FE 7.59, 7.15 GAFM 0.96 0.87 0.0 AFE 7.59, 7.16 aFbA 0.98 0.74 5.9 FE1 7.54, 6.83 — 0.00 0.46 71.7 AFE1 7.57, 6.82 — 0.00 0.44 84.8 -
[1] Novoselov K S, Jiang D, Schedin F, Booth T J, Khotkevich V V, Morozov S V, Geim A K 2005 P. Natl. Acad. Sci. USA 102 10451
Google Scholar
[2] Tang Q, Zhou Z 2013 Progr. Mat. Sci. 58 1244
Google Scholar
[3] Gupta A, Sakthivel T, Seal S 2015 Progr. Mat. Sci. 73 44
Google Scholar
[4] Duong D L, Yun S J, Lee Y H 2017 ACS Nano 11 11803
Google Scholar
[5] An M, Dong S 2020 APL Mater. 8 110704
Google Scholar
[6] Li P, Cai T Y 2020 J. Phys. Chem. C 124 12705
Google Scholar
[7] Li P, Cai T Y 2020 Phys. Chem. Chem. Phys. 22 549
Google Scholar
[8] Chang K, Liu J W, Lin H C, Wang N, Zhao K, Zhang A M, Jin F, Zhong Y, Hu X P, Duan W H, Zhang Q M, Fu L, Xue Q K, Chen X, Ji S H 2016 Science 353 274
Google Scholar
[9] Gong C, Li L, Li Z L, Ji H W, Stern A, Xia Y, Cao T, Bao W, Wang C Z, Wang Y, Qiu Z Q, Cava R J, Louie S G, Xia J, Zhang X 2017 Nature 546 265
Google Scholar
[10] Huang B, Clark G, Navarro-Moratalla E, Klein D R, Cheng R, Seyler K L, Zhong D, Schmidgall E, McGuire M A, Cobden D H, Yao W, Xiao D, Jarillo-Herrero P, Xu X D 2017 Nature 546 270
Google Scholar
[11] Hill N A 2000 J. Phys. Chem. B 104 6694
Google Scholar
[12] Liu X G, Pyatakov A P, Ren W 2020 Phys. Rev. Lett. 125 247601
Google Scholar
[13] Ju H, Lee Y, Kim K T, Choi I H, Roh C J, Son S, Park P, Kim J H, Jung T S, Kim J H, Kim K H, Park J G, Lee J S 2021 Nano Lett. 21 5126
Google Scholar
[14] Tan H X, Li M L, Liu H T, Liu Z R, Li Y C, Duan W H 2019 Phys. Rev. B 99 195434
Google Scholar
[15] Ding N, Chen J, Dong S, Stroppa A 2020 Phys. Rev. B 102 165129
Google Scholar
[16] Zhang Y, Lin L F, Moreo A, Alvarez G, Dagotto E 2021 Phys. Rev. B 103 L121114
Google Scholar
[17] You H P, Ding N, Chen J, Dong S 2020 Phys. Chem. Chem. Phys. 22 24109
Google Scholar
[18] Kresse G, Hafner J 1993 Phys. Rev. B 47 558
Google Scholar
[19] Kresse G, Furthmuller J 1996 Phys. Rev. B 54 11169
Google Scholar
[20] Perdew J P, Burke K, Ernzerhof M 1996 Phys. Rev. Lett. 77 3865
Google Scholar
[21] Monkhorst H J, Pack J D 1976 Phys. Rev. B 13 5188
Google Scholar
[22] Gonze X, Lee C 1997 Phys. Rev. B 55 10355
Google Scholar
[23] Togo A, Tanaka I 2015 Scr. Mater. 108 1
Google Scholar
[24] King-Smith R D, Vanderbilt D 1993 Phys. Rev. B 47 1651
Google Scholar
[25] Resta R 1994 Rev. Mod. Phys. 66 899
Google Scholar
[26] Orobengoa D, Capillas C, Aroyo M I, Perez-Mato J M 2009 J. Appl. Crystallogr. 42 820
Google Scholar
[27] Perez-Mato J M, Orobengoa D, Aroyo M I 2010 Acta Crystallogr. A 66 558
Google Scholar
[28] Goodenough J B 1958 J. Phys. Chem. Solids 6 287
Google Scholar
[29] Kanamori J 1959 J. Phys. Chem. Solids 10 87
Google Scholar
[30] Ogawa S 1960 J. Phys. Soc. Japan 15 1901
Google Scholar
[31] Poineau F, Johnstone E V, Czerwinski K R, Sattelberger A P 2014 Acc. Chem. Res. 47 624
Google Scholar
[32] McGuire M 2017 Crystals 7 121
Google Scholar
[33] Wieder H H 1955 Phys. Rev. 99 1161
Google Scholar
[34] Lin L F, Zhang Y, Moreo A, Dagotto E, Dong S 2019 Phys. Rev. Mater. 3 111401(R
Google Scholar
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