Research/Sitter/MAGNDATA / 0.1057_Mn3Zn0.83Mn0.15N0.99.mcif

Mn_3.15Zn_0.83N_0.99

MAGNDATA entry 0.1057 · 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 ≤ 140 K (−133 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 11 properties

Magnetic group	R 3 m BNS 166.97
Point group	3m
Parent space group	P m 3 m No. 221
Spins	coplanar · net moment 0 μ_B per cell
Propagation	[0 0 0] 1k
Cell	a 3.9027 · b 3.9027 · c 3.9027 Å · α 90° · β 90° · γ 90°
Transition	140 K (−133 °C)
Measured at	10 K
Magnetic ions	Mn
Largest moment component	1.84 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 R 3 m →

Atom sites · 4 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Mn1	Mn	0	0.5	0.5	0	1.84	−1.84	2.6022
Zn1	Zn	0	0	0
Mn2	Mn	0	0	0
N1	N	0.5	0.5	0.5

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

S. Deng et al. J. Phys. Chem. C (2024) · doi:10.1021/acs.jpcc.5b07225

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1057_Mn3Zn0.83Mn0.15N0.99.mcif from MAGNDATA · entry page

sha256 of this copy: 4151b706e87d050cd318fe9995438e2f94aea527fc72cf8616802fda177998a0
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1057_Mn3Zn0.83Mn0.15N0.99.mcif.

Mn3.15Zn0.83N0.99

Symmetry

Source

Original file

Mn_3.15Zn_0.83N_0.99