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Orbital reformation with vanadium trimerization in d2 triangular lattice LiVO2 revealed by 51V NMR

Takaaki Jin-no, Yasuhiro Shimizu, Masayuki Itoh, Seiji Niitaka, and Hidenori Takagi
Phys. Rev. B 87, 075135 – Published 22 February 2013

Abstract

LiVO2 is a model system of a valence bond solid (VBS) in a 3d2 triangular lattice. The origin of VBS formation has remained controversial. We investigate the microscopic mechanism by elucidating the d orbital character via on-site 51V NMR measurements in a single crystal up to 550 K across a structural transition temperature Tc. The Knight shift, K, and nuclear quadrupole frequency, δν, show that the 3d orbitals with local trigonal symmetry are reconstructed into a dyzdzx orbital order below Tc. Together with the NMR spectra with threefold rotational symmetry, we confirm a vanadium trimerization with d-d σ bonds. The Knight shift extracts the large Van Vleck orbital susceptibility, χVV=3.6×104, in a paramagnetic state above Tc, which is comparable to the spin susceptibility. The results suggest that the orbitally induced Peierls transition in the proximity of the frustrated itinerant state is the dominant driving force of the trimerization transition.

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  • Received 21 October 2012

DOI:https://doi.org/10.1103/PhysRevB.87.075135

©2013 American Physical Society

Authors & Affiliations

Takaaki Jin-no1, Yasuhiro Shimizu1,*, Masayuki Itoh1, Seiji Niitaka2, and Hidenori Takagi2

  • 1Department of Physics, Graduate School of Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan
  • 2RIKEN Advanced Science Institute, 2-1 Hirosawa, Wako, Saitama 351-0198, Japan

  • *Corresponding author: yasuhiro@iar.nagoya-u.ac.jp

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Issue

Vol. 87, Iss. 7 — 15 February 2013

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Images

  • Figure 1
    Figure 1
    (a) Layered triangular lattice of LiVO2 viewed from the c axis with an orbital texture obtained in the present study; only two of four leaves in dyz and dzx orbitals are shown for clarity. Thick solid and dotted lines represent unit cells of an original R3¯m lattice above Tc and a 3a×3a superlattice below Tc, respectively.[12, 14] (b) VO6 unit trigonally elongated along the c axis above Tc. (c) d levels in a trigonal field: lowest a1g singlet, middle eg doublet, and higher eg doublet. (d) Minority dxy orbitals dominate the anisotropy of NMR spectra below Tc. The x, y, and z directions are taken parallel to the VO bond directions and identical to the YX, X+Y, and Z axes, where X, Y, and Z are the principal axes of the local symmetry that determines the K and δν tensor. The b* axis is defined perpendicular to the a and c axes. The b axis is located 30 from the a axis.Reuse & Permissions
  • Figure 2
    Figure 2
    Frequency-swept 51V NMR spectra in LiVO2 (300 K, B0 = 6.105 T). The magnetic field is rotated around the (a) a, (b) b*, and (c) b axes. Dotted guidelines show the sinusoidal fitting[28] at the bottom of the peak position by taking the vertical axis as a rotation angle. Blue, red, and green lines are assigned to V1, V2, and V3 in Fig. 1c, respectively.Reuse & Permissions
  • Figure 3
    Figure 3
    Angle dependence of (a)–(c) the nuclear quadrupole splitting frequency δν and (d)–(f) the Knight shift K obtained for the b*c, ca, and bc rotations. X and Z are defined by a maximum and minimum of K and δν, respectively. Experimental data are well fitted into the Volkov's sinusoidal formula, y=y0α+y1αcos2(θϕα) (y=δν, K), with fitting parameters y0α, y1α, and ϕ for the rotation axes α=a,b*, and b.[28]Reuse & Permissions
  • Figure 4
    Figure 4
    Temperature dependence of the 51V NMR spectra measured at (a) the c axis and (b) 54 from the c axis in LiVO2. The spectrum pointed out by the arrow comes from the impurity LiV2O4.Reuse & Permissions
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