Orbitally driven spin pairing in the three-dimensional nonmagnetic Mott insulator <math display="inline"> <mrow> <msub> <mrow> <mi mathvariant="normal">BaVS</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> </mrow> <mo>:</mo> </math> Evidence from single-cry. Mihály, G., Kézsmárki, I., Zámborszky, F., Miljak, M., Penc, K., Fazekas, P., Berger, H., & Forró, L. Physical Review B, 61(12):R7831-R7834, 3, 2000.
Orbitally driven spin pairing in the three-dimensional nonmagnetic Mott insulator <math display="inline"> <mrow> <msub> <mrow> <mi mathvariant="normal">BaVS</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> </mrow> <mo>:</mo> </math> Evidence from single-cry [link]Website  abstract   bibtex   
Static electrical and magnetic properties of single crystal BaVS_3 were measured over the structural (T_S=240K), metal-insulator (T_MI=69K), and suspected orbital ordering (T_X=30K) transitions. The resistivity is almost isotropic both in the metallic and insulating states. An anomaly in the magnetic anisotropy at T_X signals a phase transition to an ordered low-T state. The results are interpreted in terms of orbital ordering and spin pairing within the lowest crystal field quasi-doublet. The disordered insulator at T_X
@article{
 title = {Orbitally driven spin pairing in the three-dimensional nonmagnetic Mott insulator <math display="inline"> <mrow> <msub> <mrow> <mi mathvariant="normal">BaVS</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> </mrow> <mo>:</mo> </math> Evidence from single-cry},
 type = {article},
 year = {2000},
 identifiers = {[object Object]},
 pages = {R7831-R7834},
 volume = {61},
 websites = {http://dx.doi.org/10.1103/PhysRevB.61.R7831,http://link.aps.org/doi/10.1103/PhysRevB.61.R7831},
 month = {3},
 day = {15},
 id = {3d66d65e-8c59-3088-881c-6aba9576bedb},
 created = {2016-12-15T10:02:51.000Z},
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 profile_id = {12182ba0-f80b-33ff-8da5-1813b38b682d},
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 last_modified = {2017-03-14T16:39:15.352Z},
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 abstract = {Static electrical and magnetic properties of single crystal BaVS_3 were measured over the structural (T_S=240K), metal-insulator (T_MI=69K), and suspected orbital ordering (T_X=30K) transitions. The resistivity is almost isotropic both in the metallic and insulating states. An anomaly in the magnetic anisotropy at T_X signals a phase transition to an ordered low-T state. The results are interpreted in terms of orbital ordering and spin pairing within the lowest crystal field quasi-doublet. The disordered insulator at T_X<T<T_MI is described as a classical liquid of non-magnetic pairs.},
 bibtype = {article},
 author = {Mihály, G. and Kézsmárki, I. and Zámborszky, F. and Miljak, Marko and Penc, K and Fazekas, P and Berger, H and Forró, L.},
 journal = {Physical Review B},
 number = {12}
}

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