Solid State Communications 149 (2009) 1818–1821
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Solid State Communications
journal homepage: www.elsevier.com/locate/ssc
Electron-nuclear double resonance study of V
4+
ions in VO
2
crystals
P.H. Bunton
a,∗
, D.B. Baker
a
, D.E. Engquist
a
, M. Klemm
b
, S. Horn
b
, Shan Yang
c
, S.M. Evans
c
,
L.E. Halliburton
c
a
Department of Physics, William Jewell College, Liberty, MO 64068, USA
b
Institute of Physics, University of Augsburg, D-86135 Augsburg, Germany
c
Department of Physics, West Virginia University, Morgantown, WV 26506, USA
article info
Article history:
Received 1 July 2009
Accepted 9 July 2009 by A.H. MacDonald
Available online 15 July 2009
PACS:
76.30.Fc
76.70.Dx
61.72.-y
71.30.+h
Keywords:
A. Semiconductors
C. Point defects
D. Electronic states (localized)
E. Electron paramagnetic resonance
abstract
Electron paramagnetic resonance (EPR) and electron-nuclear double resonance (ENDOR) are used to
identify and characterize V
4+
ions in a bulk single crystal of vanadium dioxide (VO
2
). These S = 1/2
defects are observed in the as-grown crystal because an adjacent nonmagnetic M
4+
impurity, e.g., a Si
4+
ion, has destroyed the normal antiferromagnetic coupling associated with the close pairs of V
4+
ions that
occur in the low-temperature monoclinic phase of VO
2
. EPR spectra taken near 5 K with the magnetic
field along the [110] and [001] axes show resolved hyperfine patterns due to one
51
V nucleus. ENDOR
spectra taken at 5 K with the magnetic field parallel to the [001] axis have large nuclear electric quadrupole
splittings as a result of a significant electric field gradient at the
51
V nucleus. Spin-Hamiltonian parameters
describing the electron Zeeman, hyperfine, and nuclear electric quadrupole interactions are reported.
© 2009 Elsevier Ltd. All rights reserved.
1. Introduction
The metal–insulator transition in vanadium dioxide (VO
2
) has
been widely studied, both theoretically and experimentally, since
its discovery in 1959 [1–3]. These continuing efforts are developing
a more complete understanding of the underlying fundamental
physical mechanisms and, at the same time, are introducing a
wide range of advanced applications (e.g., smart windows and
ultrafast optical switching). In general, VO
2
is a transition-metal
oxide with narrow d-electron bands, and thus represents a strongly
correlated electron system with physical responses dependent on
the interplay of long-range bandlike behavior and very strong
short-range electron–lattice and electron–electron correlations.
Below the 340 K transition temperature, VO
2
has a monoclinic
structure and is semiconducting with an energy gap of about
0.6 eV. Above the transition, it is rutile and metallic. Both Mott-
Hubbard and Peierls instabilities have been advanced to describe
the thermodynamics and energetics of the semiconducting and
metal phases of VO
2
[4], and various band and localized approaches
have been used to describe the transition (see the recent band-
theoretical approach by Eyert [5]).
∗
Corresponding author.
E-mail address: buntonp@william.jewell.edu (P.H. Bunton).
The low-temperature semiconducting phase of VO
2
is well
suited for study by electron paramagnetic resonance (EPR)
and electron-nuclear double resonance (ENDOR). Below the
metal–insulator transition, the V
4+
ions (each with one d electron)
form pairs that couple antiferromagnetically to give S = 0, and
EPR signals are not expected unless impurities or native defects
are present. Thus far, only a few EPR studies of VO
2
crystals have
been reported [6–11] and no ENDOR studies have been reported.
D’Haenens et al. [7,8] used the EPR spectra of substitutional
Cr
3+
ions with a V
5+
neighbor to investigate the M
1
, T, and M
2
phases [12] that form in chromium-doped VO
2
crystals. These
investigators showed that the T and M
2
phases in V
1−x
Cr
x
O
2
involved intermediate pairing and tilting interactions along the
vanadium chains and interpreted their EPR results as evidence of
electron localization in the form of a Mott insulator. More recently,
Misra et al. [11] fully characterized the temperature dependence
of the EPR spectra assigned to substitutional Fe
3+
ions with a V
5+
neighbor.
In the present paper, we describe a low-temperature EPR and
ENDOR study of defect-associated V
4+
ions in the monoclinic phase
of as-grown VO
2
crystals. These V
4+
ions, with S = 1/2 due to
the single d electron, are not strongly coupled to another V
4+
ion.
A nonmagnetic M
4+
impurity, most likely a Si
4+
ion, substitutes
for a V
4+
ion and leaves the remaining V
4+
ion of the original pair
without an adjacent electron spin with which to couple and form
0038-1098/$ – see front matter © 2009 Elsevier Ltd. All rights reserved.
doi:10.1016/j.ssc.2009.07.012