journal article·2018-10

Direct electrical switching of ferroelectric vortices by a sweeping biased tip

L.L. Ma, Ye Ji, W.J. Chen, J.Y. Liu, Y.L. Liu, Biao Wang, Yue Zheng

Acta Materialia· Volume 158
Publisher page

Abstract

Abstract The precise manipulation of ferroelectric vortices is one of the most important issues concerning its potential applications in functional electronic devices such as non-volatile memory. Despite investigations focusing on the switching of toroidization of vortex domain structure performed in recent years, there is still a lack of a simple and general method to realize vortex switching. In this work, we propose a direct electrical method to switch ferroelectric vortices by sweeping a biased tip, which is easy-to-operate in practice and is demonstrated to be feasible for various ferroelectric structures. It is the electric field gradient generated by the tip bias in conjunction with the time-reversal asymmetric tip-sweeping operation that induces the vortex switching. The influencing factors of this method, e.g., field profile, tip size, tip bias, tip displacement and surface screening conditions, etc., are systematically studied. As an implementation, we put forward a nanowire vortex memory system in which the information stored by vortex chirality can be successfully manipulated by the tip-sweeping method. The effects of temperature and nanowire structure on the feasibility of vortex switching are analyzed. Our findings provide an efficient control strategy on ferroelectric vortices and suggest broad device opportunities exploiting vortex domain structures.
Source: openaire · Quality: candidate unverified · Source record ↗

Research context

OpenAlex topics: Ferroelectric and Piezoelectric Materials · Acoustic Wave Resonator Technologies · Multiferroics and related materials

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

References (63)

Show source-provided references
1. Ferroelectric thin films: review of materials, properties, and applications10.1063/1.2336999 ↗
2. Size effects and depolarization field influence on the phase diagrams of cylindrical ferroelectric nanoparticles. Phys. B Condens
3. Ferroelectric phase transition in individual single-crystalline BaTiO3 nanowires10.1021/nl052538e ↗
4. Tagantsev · 2010
5. Curie temperature and critical thickness of ferroelectric thin films10.1063/1.1861517 ↗
6. Critical thickness for ferroelectricity in perovskite ultrathin films10.1038/nature01501 ↗
7. The depolarization field effect on the thin ferroelectric films properties10.1016/S0921-4526(02)01271-1 ↗
8. Above-bandgap voltages from ferroelectric photovoltaic devices10.1038/nnano.2009.451 ↗
9. Depolarization fields in thin ferroelectric films10.1063/1.1662770 ↗
10. Magnetic vortex core observation in circular dots of permalloy10.1126/science.289.5481.930 ↗
11. Theory of the motion of vortices in superconductors10.1103/PhysRev.140.A1197 ↗
12. Ferroelectricity in barium titanate quantum dots and wires10.1103/PhysRevLett.91.257601 ↗
13. Unusual phase transitions in ferroelectric nanodisks and nanorods10.1038/nature03107 ↗
14. Vortex ferroelectric domains10.1088/0953-8984/20/34/342201 ↗
15. Characteristics and controllability of vortices in ferromagnetics, ferroelectrics, and multiferroics10.1088/1361-6633/aa5e03 ↗
16. Nanoscale ferroelectrics: processing, characterization and future trends10.1088/0034-4885/69/8/R04 ↗
17. Applications of modern ferroelectrics10.1126/science.1129564 ↗
18. Vortex polarization states in nanoscale ferroelectric arrays10.1021/nl8036646 ↗
19. Unusual polarization patterns in flat epitaxial ferroelectric nanoparticles10.1103/PhysRevLett.101.107601 ↗
20. Direct observation of continuous electric dipole rotation in flux-closure domains in ferroelectric Pb(Zr,Ti)O310.1126/science.1200605 ↗
21. Toroidal ferroelectricity in PbTiO3 nanoparticles10.1103/PhysRevLett.106.137601 ↗
22. Enhanced electric conductivity at ferroelectric vortex cores in BiFeO310.1038/nphys2132 ↗
23. Observation of a periodic array of flux-closure quadrants in strained ferroelectric PbTiO3 films10.1126/science.1259869 ↗
24. Observation of polar vortices in oxide superlattices10.1038/nature16463 ↗
25. Stability of polar vortex lattice in ferroelectric superlattices10.1021/acs.nanolett.6b04875 ↗
26. Phase coexistence and electric-field control of toroidal order in oxide supperlattices10.1038/nmat4951 ↗
27. Controlling toroidal moment by means of an inhomogeneous static field: an ab initio study10.1103/PhysRevLett.96.237601 ↗
28. Vortex-to-polarization phase transformation path in ferroelectric Pb(ZrTi)O3 nanoparticles10.1103/PhysRevLett.98.077603 ↗
29. Cooperative response of Pb(ZrTi)O3 nanoparticles to curled electric fields10.1103/PhysRevLett.101.197601 ↗
30. Intrinsic switching of polarization vortex in ferroelectric nanotubes10.1103/PhysRevB.80.012101 ↗
31. Switching mechanism of polarization vortex in single-crystal ferroelectric nanodots10.1063/1.3515847 ↗
32. Vortex domain structure in ferroelectric nanoplatelets and control of its transformation by mechanical load10.1038/srep00796 ↗
33. Vortex domain structures of an epitaxial ferroelectric nanodot and its temperature-misfit strain phase diagram10.1039/c3cp00133d ↗
34. Strain induced vortex-to-uniform polarization transitions in soft-ferroelectric nanoparticles10.1063/1.4887068 ↗
35. Effects of the surface charge screening and temperature on the vortex domain patterns of ferroelectric nanodots10.1063/1.4766382 ↗
36. Discovery of stable skyrmionic state in ferroelectric nanocomposites10.1038/ncomms9542 ↗
37. Frustration and self-ordering of topological defects in ferroelectrics10.1103/PhysRevLett.116.117603 ↗
38. Coexistence of toroidal and polar domains in ferroelectric systems: a strategy for switching ferroelectric vortex10.1063/1.4881530 ↗
39. Control of vortices by homogeneous fields in asymmetric ferroelectric and ferromagnetic rings10.1103/PhysRevLett.100.047201 ↗
40. Vortex switching in ferroelectric nanodots and its feasibility by a homogeneous electric field: effects of substrate, dislocations and local clamping force10.1016/j.actamat.2015.01.041 ↗
41. Defect-mediated vortex multiplication and annihilation in ferroelectrics and the feasibility of vortex switching by stress10.1016/j.actamat.2018.01.018 ↗
42. Switching the chirality of a ferroelectric vortex in designed nanostructures by a homogeneous electric field10.1103/PhysRevB.96.134119 ↗
43. Phase-field models for microstructure evolution10.1146/annurev.matsci.32.112001.132041 ↗
44. Effect of electrical boundary conditions on ferroelectric domain structures in thin films
45. Thermodynamic modeling of critical properties of ferroelectric superlattices in nano-scale10.1007/s00339-009-5261-8 ↗
46. Landau expansion for ferroelectrics: which variable to use?10.1080/00150190802437746 ↗
47. Ultrathin films of ferroelectric solid solutions under a residual depolarizing field10.1103/PhysRevLett.93.196104 ↗
48. Atomistic treatment of depolarizing energy and field in ferroelectric nanostructures10.1103/PhysRevB.72.140102 ↗
49. Surface effects on phase transitions in ferroelectrics and dipolar magnets10.1103/PhysRevB.20.1065 ↗
50. Effect of mechanical boundary conditions on phase diagrams of epitaxial ferroelectric thin films10.1103/PhysRevLett.80.1988 ↗
51. A phenomenological thermodynamic potential for BaTiO3 single crystals10.1063/1.2042528 ↗
52. Effect of ferroelastic twin walls on local polarization switching: phase-field modeling10.1063/1.2993330 ↗
53. Phase field simulation of charged interface formation during ferroelectric switching10.1016/j.actamat.2016.04.026 ↗
54. Field enhancement of electronic conductance at ferroelectric domain walls10.1038/s41467-017-01334-5 ↗
55. a1 = 3.85(T-752) × 105, a11 = −7.3 × 107, a12 = 7.5 × 108, a111 = 2.6 × 108, a112 = 6.1 × 108, a123 = −3.7 × 109, C11 = 1.746 × 1011, C12 = 0.7937 × 1011, C44 = 1.1111 × 1011, Q11 = 0.089, Q12 = −0.026, Q44 = 0.0338, G11 = 3.46 × 10−10, G12 = 0, G44=G44'=1.73×10−10, DiS=3.46×10−10δieff=5×10−9, εb=4.425×10−10 (in SI units).
56. a1 = 4.124(T-388) × 105, a11 = −2.097 × 108, a12 = 7.974 × 108, a111 = 1.294 × 109, a112 = −1.950 × 109, a123 = −2.5 × 109, a1111 = 3.863 × 1010, a1112 = 2.529 × 1010, a1122 = 1.637 × 1010, a1123 = 1.367 × 1010, C11 = 2.75 × 1011, C12 = 1.79 × 1011, C44 = 5.43 × 1010, Q11 = 0.1104, Q12 = −0.0452, Q44 = 0.0295, G11 = 5.1 × 10−10, G12 = 0, G44=G44'=1.0×10−11, DiS=5.1×10−10, δieff=4.3×10−8, εb=4.425×10−10 (in SI units).
57. a1 = 405[Coth(54/T)-Coth(54/30)] × 105, a11 = 1.696 × 109, a12 = 3.918 × 109, C11 = 3.156 × 1011, C12 = 1.01 × 1011, C44 = 1.19 × 1011, Q11 = 0.0457, Q12 = −0.0135, Q44 = 0.0096, G11 = 1.0 × 10−11, G12 = 0.5 × 10−11, G44=G44'=1.0×10−11, DiS=1.0×10−11, δieff=5×10−9, εb=4.425×10−10 (in SI units).
58. High-density array of ferroelectric nanodots with robust and reversibly switchable topological domain states10.1126/sciadv.1700919 ↗
59. Large and tunable polar-toroidal coupling in ferroelectric composite nanowires toward superior electromechanical responses10.1038/srep11165 ↗
60. Deterministic control of magnetic vortex wall chirality by electric field10.1038/s41598-017-07944-9 ↗
61. Selective control of multiple ferroelectric switching pathways using a trailing flexoelectric field
62. Mechanical switching in ferroelectrics by shear stress and its implications on charged domain wall generation and vortex memory devices10.1039/C7RA12233K ↗
63. Deterministic control of ferroelastic switching in multiferroic materials10.1038/nnano.2009.293 ↗