Modulation of Metal–Insulator Transition in VO2 by Electrolyte Gating‐Induced Protonation

In this study, we investigated the effect of electrolyte gating on epitaxial VO 2 fi lms grown on MgF 2 substrates, unlike the TiO 2 and Al 2 O 3 substrates that were used in previous studies. [ 11,13,19–21 ] Like TiO 2 , MgF 2 has a rutile structure, but the lattice mismatch between VO 2 and MgF 2 is larger than that between VO 2 and TiO 2 . As a result, epitaxial VO 2 fi lms on MgF 2 substrates consist of grains with an average diameter of 50 nm, [ 22 ] so that there are many grain boundaries in the fi lms. We found that electrolyte gating induces proton migration into the VO 2 fi lms, whereas it induces no apparent change in oxygen content. The electrolyte gating-induced protonation caused reversible and nonvolatile changes in the electronic states of VO 2 . In addition, electrolyte gating of W-substituted VO 2 fi lms revealed that protonation induces a combined effect, involving of carrier doping and lattice deformation, on the suppression of the MIT. We deposited epitaxial VO 2 thin fi lms onto MgF 2 (001) substrates by pulsed laser deposition [ 23 ] and we fabricated VO 2 based EDL transistors (EDLTs) by standard optical lithography techniques. The fi lm thickness was set at 40 nm. Figure 1 a shows the temperature dependence of the sheet resistance ( R S ) at various values of the gate voltage ( V G ) for an EDLT. Gating was carried out at 360 K and V G was increased monotonically in 0.1 V steps. The pristine state ( V G = 0 V) exhibited a MIT at around 320 K, accompanied by a thermal hysteresis, characteristic of a fi rst-order phase transition. The value of R S in the low-temperature insulating phase gradually decreased with increasing V G , and an almost temperature-independent R S was observed at a V G of 0.8 V. We refer to this state as the gated metallic state. Note that the R S above the MIT temperature ( T MI ) increased with increasing V G . These behaviors are quite similar to those previously reported for EDLTs consisting of VO 2 fi lms on TiO 2 substrates. [ 19 ]

[1]  Y. Tokura,et al.  X-ray study of metal-insulator transitions induced by W doping and photoirradiation in VO 2 films , 2015 .

[2]  S. Parkin,et al.  Giant reversible, facet-dependent, structural changes in a correlated-electron insulator induced by ionic liquid gating , 2015, Proceedings of the National Academy of Sciences.

[3]  Heng Ji,et al.  Hydrogen diffusion and stabilization in single-crystal VO2 micro/nanobeams by direct atomic hydrogenation. , 2014, Nano letters.

[4]  Ziyu Wu,et al.  Depressed transition temperature of W(x)V(1-x)O2: mechanistic insights from the X-ray absorption fine structure (XAFS) spectroscopy. , 2014, Physical chemistry chemical physics : PCCP.

[5]  Y. Filinchuk,et al.  In situ diffraction study of catalytic hydrogenation of VO₂: stable phases and origins of metallicity. , 2014, Journal of the American Chemical Society.

[6]  Bin Wang,et al.  Hydrogen dynamics and metallic phase stabilization in VO2 , 2014 .

[7]  Y. Tokura,et al.  Gate-tunable gigantic lattice deformation in VO2 , 2014 .

[8]  A. Sawa,et al.  Epitaxial growth and structural transition of VO2/MgF2(001) , 2014 .

[9]  Y. Tokura,et al.  Infrared-sensitive electrochromic device based on VO2 , 2013 .

[10]  Tatsuo Hasegawa,et al.  Fabrication and Raman scattering study of epitaxial VO2 films on MgF2 (001) substrates , 2013 .

[11]  Masashi Kawasaki,et al.  Electrolyte‐Gated SmCoO3 Thin‐Film Transistors Exhibiting Thickness‐Dependent Large Switching Ratio at Room Temperature , 2013, Advances in Materials.

[12]  S. Parkin,et al.  Suppression of Metal-Insulator Transition in VO2 by Electric Field–Induced Oxygen Vacancy Formation , 2013, Science.

[13]  Ziyu Wu,et al.  Metal-insulator transition in V(1-x)W(x)O2: structural and electronic origin. , 2012, Physical chemistry chemical physics : PCCP.

[14]  M. Kawasaki,et al.  Collective bulk carrier delocalization driven by electrostatic surface charge accumulation , 2012, Nature.

[15]  Heng Ji,et al.  Hydrogen stabilization of metallic vanadium dioxide in single-crystal nanobeams , 2012 .

[16]  Heng Ji,et al.  Modulation of the electrical properties of VO₂ nanobeams using an ionic liquid as a gating medium. , 2012, Nano letters.

[17]  M. E. Kompan,et al.  Influence of hydrogenation on electrical conductivity of vanadium dioxide thin films , 2012 .

[18]  A. Sawa,et al.  Strain‐Mediated Phase Control and Electrolyte‐Gating of Electron‐Doped Manganites , 2011, Advanced materials.

[19]  Y. Tokura,et al.  Competition between instabilities of Peierls transition and Mott transition in W-doped VO 2 thin films , 2011 .

[20]  Ziyu Wu,et al.  Hydrogen-incorporation stabilization of metallic VO2(R) phase to room temperature, displaying promising low-temperature thermoelectric effect. , 2011, Journal of the American Chemical Society.

[21]  J. Misewich,et al.  Superconductor–insulator transition in La2 − xSrxCuO4 at the pair quantum resistance , 2011, Nature.

[22]  Shimpei Ono,et al.  Electric‐Field Control of the Metal‐Insulator Transition in Ultrathin NdNiO3 Films , 2010, Advanced materials.

[23]  Masashi Kawasaki,et al.  Tuning of the metal-insulator transition in electrolyte-gated NdNiO3 thin films , 2010 .

[24]  Hongtao Yuan,et al.  Liquid-gated interface superconductivity on an atomically flat film. , 2010, Nature materials.

[25]  Masashi Kawasaki,et al.  Metal-insulator transition in epitaxial V1−xWxO2(0≤x≤0.33) thin films , 2010 .

[26]  Masashi Kawasaki,et al.  Electric-field-induced superconductivity in an insulator. , 2008, Nature materials.

[27]  Silke Biermann,et al.  Effective band-structure in the insulating phase versus strong dynamical correlations in metallic VO2 , 2007, 0704.0902.

[28]  C. Ahn,et al.  Electric field effect in correlated oxide systems , 2003, Nature.

[29]  Vladislav V. Yakovlev,et al.  Raman microscopy analysis of phase transformation mechanisms in vanadium dioxide , 2002 .

[30]  P. Schilbe Raman scattering in VO2 , 2002 .

[31]  M. Armand,et al.  Issues and challenges facing rechargeable lithium batteries , 2001, Nature.

[32]  Ahn,et al.  Electrostatic modulation of superconductivity in ultrathin GdBa2Cu3O7-x films , 1999, Science.

[33]  Mathews,et al.  Ferroelectric Field Effect Transistor Based on Epitaxial Perovskite Heterostructures , 1997, Science.

[34]  Pouget,et al.  Comment on "VO2: Peierls or Mott-Hubbard? A view from band theory" , 1994, Physical Review Letters.

[35]  Allen,et al.  VO2: Peierls or Mott-Hubbard? A view from band theory. , 1994, Physical review letters.

[36]  W. Estrada,et al.  Electrochromism and thermochromism of LixVO2 thin films , 1991 .

[37]  J. Molenda Electronic structure and electrochemical properties of VO2 , 1989 .

[38]  Tang,et al.  Local atomic and electronic arrangements in WxV1-xO2. , 1985, Physical Review B (Condensed Matter).

[39]  Mats Nygren,et al.  Electrical and magnetic properties of V1−xWxO2, 0 ≤ x ≤ 0.060 , 1972 .

[40]  John B. Goodenough,et al.  The two components of the crystallographic transition in VO2 , 1971 .

[41]  F. J. Morin,et al.  Oxides Which Show a Metal-to-Insulator Transition at the Neel Temperature , 1959 .