2016
DOI: 10.1103/physrevb.94.104436
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Spin and orbital disordering by hole doping inPr1xCaxVO3<

Abstract: High-resolution powder x-ray diffraction and single-crystal neutron diffraction were used to investigate the crystal structure and magnetic ordering of the compound Pr 1−x Ca x VO 3 (0 x 0.3), which undergoes an insulator-to-metal transition for x ∼ 0.23. Since the ionic radii of Pr 3+ and Ca 2+ are almost identical and structural disorder is minimal, Pr 1−x Ca x VO 3 is a good model system for the influence of hole doping on the spin and orbital correlations in transition metal oxides. The end member PrVO 3 i… Show more

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Cited by 14 publications
(21 citation statements)
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References 42 publications
(96 reference statements)
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“…We point out that despite an antiferromagnetic spin order expected at low temperature, antisymmetric spin-spin interactions via Dzyaloshinskii-Moriya interactions promote a canted and uncompensated spin state [19,36,37]. Together with the spin imbalance of the V 3d-V 3d sublattices [38], V 3d-R 4 f magnetic exchange interactions [39][40][41] may also strengthen the ferromagneticlike signal as observed here for PVO compared to LVO, whose magnetization is about 100 times lower. Indeed, Pr 3+ has two electrons in the 4 f orbitals whereas LVO has none.…”
Section: Resultssupporting
confidence: 49%
“…We point out that despite an antiferromagnetic spin order expected at low temperature, antisymmetric spin-spin interactions via Dzyaloshinskii-Moriya interactions promote a canted and uncompensated spin state [19,36,37]. Together with the spin imbalance of the V 3d-V 3d sublattices [38], V 3d-R 4 f magnetic exchange interactions [39][40][41] may also strengthen the ferromagneticlike signal as observed here for PVO compared to LVO, whose magnetization is about 100 times lower. Indeed, Pr 3+ has two electrons in the 4 f orbitals whereas LVO has none.…”
Section: Resultssupporting
confidence: 49%
“…The combination of spin and orbital degrees of freedom triggers spin-orbital (SO) polarons [59][60][61][62]. We shall discuss in this work why small SO polarons in the insulating regime of cubic vanadates [58,63] are much more strongly bound to charge defects than spin polarons in high-T c materials [64,65]. The reduced mobility of doped holes or electrons inside the SO polarons implies a weaker screening of defect potentials by the doped charge carriers and thus provides an arXiv:1710.05171v1 [cond-mat.str-el] 14 Oct 2017 explanation for the shift of the insulator to metal transition towards high doping concentrations in the vanadates.…”
Section: Introductionmentioning
confidence: 99%
“…Naturally, vanadates are considered to be model canonical systems for investigating a rich variety of outstanding magnetic and electrical behaviors originating from the interconnected knot of spin, charge, orbital and lattice correlations of the V t 2g electrons [8][9][10][11][12][13] . The t 2g valence electrons of the V ions (V 3+ : t 2 2g /V 4+ : t 1 2g ) undergo significantly lower noncubic crystal field splitting, as compared to that of the e g manifold in isostructural manganites, resulting in the comparable energy separation of orbital levels to the spin interactions 7,11 .…”
Section: Introductionmentioning
confidence: 99%