Research/Sitter/MAGNDATA / 0.851_C7H14NFeCl4.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of C7H14Cl4FeNSpin lattice of C7H14Cl4FeN

C7H14Cl4FeN

MAGNDATA entry 0.851 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
ordered ≤ 3 K (−270 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 21′21′21 BNS 19.27
Point group2′2′2
Parent space groupP b c a No. 61
Spinscoplanar · net moment 0.4 μB per cell
Propagation[0 0 0] 1k
Cella 13.0547 · b 12.5671 · c 14.6 Å · α 90° · β 90° · γ 90°
Transition3 K (−270 °C)
Measured at2 K
Magnetic ionsFe
Largest moment component3.5 μB
MethodNeutron single-crystal on the D19 in Institut Laue-Langevin

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 21′21′21 →
Atom sites · 54 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1_1Fe0.28310.04260.2491−1.23−3.50.053.7102
Fe1_2Fe0.71690.95740.75091.81−3.20.053.6768
Cl4_1Cl0.20130.98870.3713
Cl4_2Cl0.79870.01130.6287
Cl2_1Cl0.44190.98530.2559
Cl2_2Cl0.55820.01470.7441
Cl1_1Cl0.21620.97850.1221
Cl1_2Cl0.78370.02150.8779
Cl3_1Cl0.27850.21750.2424
Cl3_2Cl0.72150.78250.7576
N1_1N0.09750.29610.0821
N1_2N0.90250.70390.9179
C7_1C0.98130.33580.9534
C7_2C0.01870.66420.0466
H71_1H0.90110.36310.9503
H71_2H0.09890.63690.0497
H72_1H0.01830.36440.8904
H72_2H0.98170.63560.1096
C3_1C0.09810.18040.9456
C3_2C0.90190.81960.0544
H31_1H0.1250.19240.8768
H31_2H0.8750.80760.1232
H32_1H0.10590.09540.9608
H32_2H0.89410.90460.0392
C2_1C0.16510.24460.0113
C2_2C0.83490.75540.9887
H21_1H0.21980.19510.0481
H21_2H0.78020.80490.9519
H22_1H0.20540.30910.9764
H22_2H0.79460.69090.0236
C6_1C0.02780.21550.1253
C6_2C0.97220.78450.8747
H61_1H0.99240.25250.1855
H61_2H0.00760.74750.8145
H62_1H0.07460.15080.1492
H62_2H0.92540.84920.8508
C4_1C0.98630.21480.9581
C4_2C0.01370.78520.0419
H4_1H0.93950.17980.9043
H4_2H0.06050.82020.0957
C5_1C0.95030.1780.0525
C5_2C0.04970.8220.9475
H51_1H0.87360.21070.0677
H51_2H0.12640.78930.9323
H52_1H0.93960.09250.0574
H52_2H0.06040.90750.9426
C8_1C0.03520.38290.0374
C8_2C0.96480.61710.9626
H81_1H0.08920.44620.0204
H81_2H0.91080.55380.9796
H82_1H0.98250.41160.0893
H82_2H0.01750.58840.9107
H1_1H0.14240.33180.1318
H1_2H0.85760.66820.8682

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

P. Gonzalez-Izquierdo et al. J. Mater. Chem. C (2020) · doi:10.1039/d0tc02341h

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.851_C7H14NFeCl4.mcif from MAGNDATA · entry page

sha256 of this copy: 65f803fbb9a2a9f971be7a2650b57a960145cc39a1752cb1a2994280780bcb59
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.851_C7H14NFeCl4.mcif.