Research/Sitter/MAGNDATA / 0.1071_Fe2SiO4.mcif

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Spin lattice of Fe2Si1O4Spin lattice of Fe2Si1O4

Fe2Si1O4

MAGNDATA entry 0.1071 · source
d-wave altermagnet
No net magnetisation, yet the electron bands are spin-split: the up and down spin sublattices are related only by a rotation or mirror, never by a shift or inversion. d-wave: the splitting changes sign twice around the Fermi surface (2 nodal planes).
Spin group ²m²m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 65.4 K (−208 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP n m a . 1 BNS 62.441
Point groupmmm
Parent space groupP n m a No. 62
Spinscollinear · 2 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 4.81654 · b 10.44887 · c 6.08256 Å · α 90° · β 90° · γ 90°
Transition65.4 K (−208 °C)
Measured at40 K
Magnetic ionsFe
Largest moment component4.28 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 n m a . 1 →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1Fe000002.382.38
Fe2Fe0.98590.27980.25004.284.28
Si1Si0.43070.09720.25
O1O0.76870.0920.25
O2O0.20880.45290.25
O3O0.28890.16580.4642

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

Evangelia K. Tripoliti et al. Mineralogical Magazine (2023) · doi:10.1180/mgm.2023.66

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1071_Fe2SiO4.mcif from MAGNDATA · entry page

sha256 of this copy: 3ae667fd11aaf2609cba127147ec15aaadf185cc27af6cf4acd11680989fde67
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1071_Fe2SiO4.mcif.