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@ARTICLE{Ji:866007,
author = {Ji, W. H. and Yin, L. and Zhu, W. M. and Kumar, C. M. N.
and Li, Cheng and Li, H.-F. and Jin, W. T. and Nandi, S. and
Sun, Xiao and Su, Y. and Brückel, Th. and Lee, Y. and
Harmon, B. N. and Ke, L. and Ouyang, Z. W. and Xiao, Y.},
title = {{N}oncollinear magnetic structure and anisotropic
magnetoelastic coupling in cobalt pyrovanadate {C}o 2 {V} 2
{O} 7g4},
journal = {Physical review / B},
volume = {100},
number = {13},
issn = {2469-9950},
address = {Woodbury, NY},
publisher = {Inst.},
reportid = {FZJ-2019-05267},
pages = {134420},
year = {2019},
abstract = {Co2V2O7 was recently reported to exhibit remarkable
magnetic-field-induced magnetization plateaus and
ferroelectricity [R. Chen et al., Phys. Rev. B 98, 184404
(2018)], but its magnetic ground state remains ambiguous.
Magnetometry measurements and time-of-flight neutron powder
diffraction (NPD) have been employed to study the structural
and magnetic properties of Co2V2O7, which includes two
nonequivalent Co sites. Upon cooling below the Néel
temperature TN=6.0(2) K, we observe magnetic Bragg peaks at
2 K in NPD, which indicates the formation of long-range
magnetic order of Co2+ moments. After symmetry analysis and
magnetic structure refinement, we demonstrate that Co2V2O7
possesses a complicated noncollinear magnetic ground state
with Co moments mainly located in the b-c plane and forming
a noncollinear spin-chain-like structure along the c-axis.
The ab initio calculations demonstrate that the noncollinear
magnetic structure is more stable than various ferromagnetic
states at low temperature. The noncollinear magnetic
structure with a canted ↑↑↓↓ spin configuration is
considered to be the origin of magnetoelectric coupling in
Co2V2O7 because the inequivalent exchange striction induced
by the spin-exchange interaction between the neighboring
spins could be the driving force of ferroelectricity. It is
also found that the deviation of lattice parameters a and b
is opposite below TN, while the lattice parameter c and β
stay almost constant below TN, evidencing the anisotropic
magnetoelastic coupling in Co2V2O7.},
cin = {JCNS-2 / PGI-4 / JARA-FIT / JCNS-FRM-II},
ddc = {530},
cid = {I:(DE-Juel1)JCNS-2-20110106 / I:(DE-Juel1)PGI-4-20110106 /
$I:(DE-82)080009_20140620$ /
I:(DE-Juel1)JCNS-FRM-II-20110218},
pnm = {144 - Controlling Collective States (POF3-144) / 524 -
Controlling Collective States (POF3-524) / 6212 - Quantum
Condensed Matter: Magnetism, Superconductivity (POF3-621) /
6213 - Materials and Processes for Energy and Transport
Technologies (POF3-621) / 6G4 - Jülich Centre for Neutron
Research (JCNS) (POF3-623)},
pid = {G:(DE-HGF)POF3-144 / G:(DE-HGF)POF3-524 /
G:(DE-HGF)POF3-6212 / G:(DE-HGF)POF3-6213 /
G:(DE-HGF)POF3-6G4},
experiment = {EXP:(DE-MLZ)External-20140101},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000489820500006},
doi = {10.1103/PhysRevB.100.134420},
url = {https://juser.fz-juelich.de/record/866007},
}