Research/Sitter/MAGNDATA / 2.62_TbCrO3.mcif

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Spin lattice of TbCrO3Spin lattice of TbCrO3

TbCrO3

MAGNDATA entry 2.62 · source
noncoplanar magnet
Spins pointing in three dimensions, not confined to a plane.
ordered ≤ 3.1 K (−270 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP m′ n′ 21 BNS 31.127
Parent space groupP b n m No. 62
Spinsnoncoplanar · net moment 0 μB per cell
Propagation[0 1/2 0] · [0 0 0] 2k
Cella 5.291 · b 11.026 · c 7.557 Å · α 90° · β 90° · γ 90°
Transition3.05 K (−270 °C)
Measured at1.5 K
Magnetic ionsCr, Tb
Largest moment component7.76 μB
MethodNPD

Symmetry

Stereogram of the magnetic point group: each operation applied to one direction. Filled = upper hemisphere, ring = lower; red operations include time reversal. Lines are mirrors; polygons are 2/3/4/6-fold axes; the centre ring is inversion.

Every structure in P m′ n′ 21 →
Atom sites · 14 sites · CSV
siteelementxyzmambmc|m| (μB)
Tb1_1Tb0.9890.0320.257.763.1708.3825
Tb1_2Tb0.4890.2180.75−7.763.1708.3825
Tb1_3Tb0.0110.9680.75−7.76−3.1708.3825
Tb1_4Tb0.5110.2820.257.76−3.1708.3825
Cr1_1Cr0.500002.852.85
Cr1_2Cr00.25000−2.852.85
O1_1O0.0960.2350.25
O1_2O0.5960.0150.75
O1_3O0.9040.7650.75
O1_4O0.4040.4850.25
O2_1O0.6970.15050.049
O2_2O0.1970.09950.951
O2_3O0.3030.84950.549
O2_4O0.8030.40050.451

Moment components are along the crystal axes a, b, c (μB), as magCIF writes them. Symmetry generates the rest of the cell from these sites.

Source

E.F. Bertaut et al. J. Phys. Chem. Solids (1967) · doi:10.1016/0038-1098(67)90276-1

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 2.62_TbCrO3.mcif from MAGNDATA · entry page

sha256 of this copy: 3effce61f5282590c0442cd4f29c7f8b52808e1f2b0235b9a49251f804a6241e
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.62_TbCrO3.mcif.