Research/Sitter/MAGNDATA / 1.93_HoFe3(BO3)4.mcif

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Spin lattice of HoFe3(BO3)4Spin lattice of HoFe3(BO3)4

HoFe3(BO3)4

MAGNDATA entry 1.93 · source
p-wave magnet
Coplanar spins, no net moment, and a translation that reverses every spin: spin splitting that is odd in momentum (p-wave).
ordered ≤ 37 K (−236 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPS 1 BNS 1.3
Point group11′
Parent space groupP 3121 No. 152
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 1/2] 1k
Cella 9.5143 · b 9.5143 · c 15.0787 Å · α 90° · β 90° · γ 120°
Transition37 K (−236 °C)
Measured at6 K
Magnetic ionsFe, Ho
Largest moment component4.7 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 PS 1 →
Atom sites · 60 sites · CSV
siteelementxyzmambmc|m| (μB)
Ho1_1Ho0.335600.16674.7004.7
Ho1_2Ho00.33560.3333−4.7004.7
Ho1_3Ho0.66440.66440−4.7004.7
Fe1_1Fe0.883800.1667−4.2004.2
Fe1_2Fe00.88380.33334.2004.2
Fe1_3Fe0.11620.116204.2004.2
Fe2_1Fe0.78730.44960.1726−4.20−2.34.7885
Fe2_2Fe0.55040.33770.33934.202.34.7885
Fe2_3Fe0.66230.21270.506−4.20−2.34.7885
Fe2_4Fe0.44960.78730.8274−4.20−2.34.7885
Fe2_5Fe0.33770.55040.1607−4.20−2.34.7885
Fe2_6Fe0.21270.66230.9944.202.34.7885
O1_1O0.92500.4167
O1_2O00.9250.0833
O1_3O0.0750.0750.25
O2_1O0.4190.7220.0625
O2_2O0.2780.6970.2292
O2_3O0.3030.5810.3958
O2_4O0.7220.4190.9375
O2_5O0.6970.2780.2708
O2_6O0.5810.3030.1042
O3_1O0.8730.6940.4115
O3_2O0.3060.1790.5782
O3_3O0.8210.1270.7448
O3_4O0.6940.8730.5885
O3_5O0.1790.3060.9218
O3_6O0.1270.8210.7552
O4_1O0.8570.6390.0945
O4_2O0.3610.2180.2612
O4_3O0.7820.1430.4278
O4_4O0.6390.8570.9055
O4_5O0.2180.3610.2388
O4_6O0.1430.7820.0722
O5_1O0.4750.1440.4205
O5_2O0.8560.3310.5872
O5_3O0.6690.5250.7538
O5_4O0.1440.4750.5795
O5_5O0.3310.8560.9128
O5_6O0.5250.6690.7462
O6_1O0.18400.4167
O6_2O00.1840.0833
O6_3O0.8160.8160.25
O7_1O0.47520.4640.408
O7_2O0.5360.01120.5747
O7_3O0.98880.52480.7413
O7_4O0.4640.47520.592
O7_5O0.01120.5360.9253
O7_6O0.52480.98880.7587
B1_1B0.32900.4167
B1_2B00.3290.0833
B1_3B0.6710.6710.25
B2_1B0.5490.87740.0745
B2_2B0.12260.67160.2412
B2_3B0.32840.4510.4078
B2_4B0.87740.5490.9255
B2_5B0.67160.12260.2588
B2_6B0.4510.32840.0922
B3_1B0.77900.4167
B3_2B00.7790.0833
B3_3B0.2210.2210.25

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

C. Ritter et al. J. Phys.: Condens. Matter (2008) · doi:10.1088/0953-8984/20/36/365209

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.93_HoFe3(BO3)4.mcif from MAGNDATA · entry page

sha256 of this copy: 7cbfde85f648f8be69c2a730289e80d445f6aa3d2b47e045e79925d3118d7ef7
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.93_HoFe3(BO3)4.mcif.