Research/Sitter/MAGNDATA / 0.662_Mn3Sn2.mcif

Mn₃Sn₂

MAGNDATA entry 0.662 · source

s-wave ferromagnet

All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).

Spin group ¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.

ordered ≤ 262 K (−11 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 10 properties

Magnetic group	P n′ m a′ BNS 62.448
Parent space group	P n m a No. 62
Spins	collinear · net moment 12.76 μ_B per cell
Propagation	[0 0 0] 1k
Cell	a 7.5646 · b 5.5099 · c 8.5975 Å · α 90° · β 90° · γ 90°
Transition	262 K (−11 °C)
Measured at	235 K
Magnetic ions	Mn
Largest moment component	1.53 μ_B
Method	NPD

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′ →

Atom sites · 4 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Mn1	Mn	0.2245	0.0036	0.1229	0	0.83	0	0.83
Mn2	Mn	0.9079	0.25	0.1299	0	1.53	0	1.53
Sn1	Sn	0.5969	0.25	0.6426
Sn2	Sn	0.561	0.25	0.0932

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

Source

T. Mazet et al. PHYSICAL REVIEW B (2010) · doi:10.1103/PhysRevB.81.174427

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.662_Mn3Sn2.mcif from MAGNDATA · entry page

sha256 of this copy: d2e416e78448ec08040011cf52a3bb30c4d4a4f46659c8458a885b0e2a39a33d
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.662_Mn3Sn2.mcif.