Altermagnets Database

High-throughput computational screening for altermagnetic materials

$\mathrm{Fe_{3}H_{4}(OF_{4})_{2}}$

ID anyt:am-1-0122

C2/m | Both | Semiconducting

AM wave d

Identity

Elements
Fe, H, O, F
Space group i Parent crystallographic space-group.
${\mathrm{C}2/\mathrm{m}}$ (12)
MAGNDATA IDs i A screened entry may correspond to one or more entries in the MAGNDATA database.
ICSD IDs
n/a
Parent space group(s) i Parent nonmagnetic space group(s) reported by the MAGNDATA-based symmetry analysis after Spglib standardisation.
${\mathrm{C}2/\mathrm{m}}$ (12)

Properties

KS Gap i The band gap from Kohn-Sham DFT.
2.686 eV
KS Gap Type
Semiconducting
Min abundance i Minimum crustal abundance among the constituent elements, reported in ppm as a simple scarcity proxy.
585.0 ppm

Spin-splitting metrics

$\Delta E^{\mathrm{max}}_{\mathrm{split}}$ i Largest spin splitting within ±3 eV of the Fermi level in the high-throughput calculation.
0.106 eV
$\Delta E^{\mathrm{avg}}_{\mathrm{split}}$ i Brillouin-zone average of the largest spin splitting at each k-point within the same energy window.
0.065 eV
i Fraction of the sampled Brillouin zone and near-Fermi bands with appreciable spin splitting.
22.9%

Figures

1 of 3 detail figures available from the mounted calculation archive.

Band structure

Band structure has not been generated for this material yet.

Crystal structure

Crystal structure view

Brillouin zone and path

Reciprocal-space box with labelled special points and the reported Δmax location when available.

Brillouin-zone figure has not been generated for this material yet.

Symmetry screening

The summary table shows one row per linked MAGNDATA record and symmetry-precision variant. If a MAGNDATA ID has multiple Spglib symprec values in the source data, it appears on multiple rows. The cards below keep the same expanded per-variant detail view, including wave classification and mismatch metrics.

MAGNDATA ID Collinearity i Whether the magnetic configuration was collinear in MAGNDATA or constructed from a noncollinear entry. Phase i Some materials also have non-altermagnetic (AM) phases predicted; AM for altermagnet and FiM for ferrimagnet. Wave i Symmetry wave-class shorthand derived from the parent and halving-subgroup Laue classes used in the altermagnetism analysis. SYMPREC i Spglib symmetry tolerance symprec, shown as an exponential base-10 value. BNS (MCIF) i BNS setting indicated in the source MCIF file. G H
0.582 Collinear AM d $10^{-5}$ ${\mathrm{C}2^{\prime}/\mathrm{m}^{\prime}}$ (12.62) 2/m -1
2.61 Based on noncollinear AM d $10^{-5}$ ${\mathrm{C}2^{\prime}/\mathrm{m}^{\prime}}$ (12.62) 2/m -1

MAGNDATA 0.582

$\mathrm{Fe_{3}F_{8}(H_{2}O)_{2}}$

Open entry
Collinearity Collinear
Phase AM
Wave d
BNS (MCIF) i BNS setting indicated in the source MCIF file.
${\mathrm{C}2^{\prime}/\mathrm{m}^{\prime}}$ (12.62)
BNS
${\mathrm{C}2^{\prime}/\mathrm{m}^{\prime}}$ (12.62)
Parent SG
${\mathrm{C}2/\mathrm{m}}$ (12)
SYMPREC i Spglib symmetry tolerance symprec, shown as an exponential base-10 value.
$10^{-5}$
Connecting element
$C_{21}$
G Laue class
2/m
H Laue class
-1
Spin-angle mismatch
0.0°

MAGNDATA 2.61

$\mathrm{Fe_{3}F_{8}(H_{2}O)_{2}}$

Open entry
Collinearity Based on noncollinear
Phase AM
Wave d
BNS (MCIF) i BNS setting indicated in the source MCIF file.
${\mathrm{C}2^{\prime}/\mathrm{m}^{\prime}}$ (12.62)
BNS
${\mathrm{C}2^{\prime}/\mathrm{c}^{\prime}}$ (15.89)
Parent SG
${\mathrm{C}2/\mathrm{m}}$ (12)
SYMPREC i Spglib symmetry tolerance symprec, shown as an exponential base-10 value.
$10^{-5}$
Connecting element
$C_{21}$
G Laue class
2/m
H Laue class
-1
Spin-angle mismatch
72.7°