Altermagnets Database

High-throughput computational screening for altermagnetic materials

$\mathrm{Ca_{3}MnCoO_{6}}$

ID anyt:am-1-0163

R-3c | Collinear | Semiconducting

AM wave g

Identity

Elements
Ca, Mn, Co, O
Space group i Parent crystallographic space-group.
${\mathrm{R}3\mathrm{c}}$ (161), ${\mathrm{R}\overline{3}\mathrm{c}}$ (167)
MAGNDATA IDs i A screened entry may correspond to one or more entries in the MAGNDATA database.
ICSD IDs
93775
Parent space group(s) i Parent nonmagnetic space group(s) reported by the MAGNDATA-based symmetry analysis after Spglib standardisation.
${\mathrm{R}3\mathrm{c}}$ (161), ${\mathrm{R}\overline{3}\mathrm{c}}$ (167)

Properties

KS Gap i The band gap from Kohn-Sham DFT.
2.003 eV
KS Gap Type
Semiconducting
Min abundance i Minimum crustal abundance among the constituent elements, reported in ppm as a simple scarcity proxy.
25.0 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.
0.063 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.
0.051 eV
i Fraction of the sampled Brillouin zone and near-Fermi bands with appreciable spin splitting.
18.8%

Figures

0 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 figure has not been generated for this material yet.

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
0.13 Collinear AM g $10^{-5}$ ${\mathrm{R}3\mathrm{c}}$ (161.69) -3m -3
0.13 Collinear AM g $10^{-4}$ ${\mathrm{R}3\mathrm{c}}$ (161.69) -3m -3

MAGNDATA 0.13

$\mathrm{Ca_{3}Co_{2}-xMnxO_{6}}$

Open entry
Collinearity Collinear
Phase AM
Wave g
BNS (MCIF) i BNS setting indicated in the source MCIF file.
${\mathrm{R}3\mathrm{c}}$ (161.69)
BNS
${\mathrm{R}3\mathrm{c}^{\prime}}$ (161.71)
Parent SG
${\mathrm{R}3\mathrm{c}}$ (161)
SYMPREC i Spglib symmetry tolerance symprec, shown as an exponential base-10 value.
$10^{-5}$
Connecting element
$Cs$
G Laue class
-3m
H Laue class
-3
Spin-angle mismatch
0.0°

MAGNDATA 0.13

$\mathrm{Ca_{3}Co_{2}-xMnxO_{6}}$

Open entry
Collinearity Collinear
Phase AM
Wave g
BNS (MCIF) i BNS setting indicated in the source MCIF file.
${\mathrm{R}3\mathrm{c}}$ (161.69)
BNS
${\mathrm{R}3\mathrm{c}^{\prime}}$ (161.71)
Parent SG
${\mathrm{R}\overline{3}\mathrm{c}}$ (167)
SYMPREC i Spglib symmetry tolerance symprec, shown as an exponential base-10 value.
$10^{-4}$
Connecting element
$Cs$
G Laue class
-3m
H Laue class
-3
Spin-angle mismatch
0.0°

Notes and warnings

  • Spglib mcif symmetry mismatch
  • Spglib mcif symmetry mismatch