Material:

Y

ID:

MMD-855

Explore database:

Compounds with the same formula: Y (4 entries found)
Compounds with the same elements: Y (4 entries found)

Navigation:
Space group | Lattice parameters | Thermodynamic properties | Phase diagram | Magnetic properties | Atomic positions and site-specific magnetic data | Pair-wise magnetic data | Methods | References

Space group:

Crystal system

trigonal

Space group number

166

Hermann-Mauguin

R-3m

Hall

-R 3 2"

Point group

-3m

Structure data:

Normalized formula

Y

The number of formula units per unit cell

9

The total number of atoms per unit cell

9

The number of inequivalent sites per unit cell

2

Structure search

MP


Lattice parameters:

a (Å)

3.6020

b (Å)

3.6020

c (Å)

26.0048

α (deg.)

90.000

β (deg.)

90.000

γ (deg.)

120.000

Volume (Å3)

292.189

Density (g/cm3)

4.547

Crystal structure visualization:


Thermodynamic properties:

DFT calculations (details)

Formation energy (vs. elemental phases)

4.8 meV/atom

Formation energy above hull

4.8 meV/atom

Phase diagram:


Phase diagram is not available for this entry.

Related structures:

Compounds with the same formula: Y

4 entries found

Compounds with the same elements: Y

4 entries found


Magnetic properties:

DFT calculations (details)

Magnetic ordering

Ferromagnetic

Total magnetic moment

0.01 μB/cell

Averaged magnetic moment

0.00 μB/atom

Magnetic polarization, Js = μ0Ms

0.00 T (= 0.0 emu/cm3)

LMTO-GF calculations (details)

Curie temperature, TC

DFT calculations (details)

Magnetic easy axis

Magnetic hardness parameter, κ


Atomic positions (fractional coordinates) and site-specific magnetic data:

index species w x y z m (μB) Esoc100 (meV) Esoc001 (meV)
1 Y 3a 0.000000 0.000000 0.000000 -0.00 . .
2 Y 3a 0.000000 0.000000 0.221823 0.00 . .
3 Y 3a 0.666667 0.333333 0.111511 0.00 . .
4 Y 6c 0.666667 0.333333 0.333333 -0.00 . .
5 Y 6c 0.666667 0.333333 0.555156 -0.00 . .
6 Y 6c 0.333333 0.666667 0.444844 -0.00 . .
7 Y 6c 0.333333 0.666667 0.666667 -0.00 . .
8 Y 6c 0.333333 0.666667 0.888489 0.00 . .
9 Y 6c 0.000000 0.000000 0.778177 0.00 . .
w: site multiplicity (the number of equivalent positions) and Wyckoff letter (a label for site symmetry)
m: local magnetic moment
Esoc100 (001): Spin-orbit coupling energy for the magnetization oriented along the crystallographic a (c) axis
(Individual Esoc values are temporarily not available while we perform maintenance.)

Site-resolved magnetic moments:

Local magnetic moments

Pair-wise magnetic data:

site i site j distance (Å) Jij (meV)
1 Y 3a 2 Y 3a 5.77 .
1 Y 3a 3 Y 3a 3.57 .
1 Y 3a 4 Y 6c 8.91 .
1 Y 3a 5 Y 6c 11.75 .
1 Y 3a 6 Y 6c 11.75 .
1 Y 3a 7 Y 6c 8.91 .
1 Y 3a 8 Y 6c 3.57 .
1 Y 3a 9 Y 6c 5.77 .
2 Y 3a 3 Y 3a 3.54 .
2 Y 3a 4 Y 6c 3.57 .
2 Y 3a 5 Y 6c 8.91 .
2 Y 3a 6 Y 6c 6.16 .
2 Y 3a 7 Y 6c 11.75 .
2 Y 3a 8 Y 6c 8.91 .
2 Y 3a 9 Y 6c 11.54 .
3 Y 3a 4 Y 6c 5.77 .
3 Y 3a 5 Y 6c 11.54 .
3 Y 3a 6 Y 6c 8.91 .
3 Y 3a 7 Y 6c 11.75 .
3 Y 3a 8 Y 6c 6.16 .
3 Y 3a 9 Y 6c 8.91 .
4 Y 6c 5 Y 6c 5.77 .
4 Y 6c 6 Y 6c 3.57 .
4 Y 6c 7 Y 6c 8.91 .
4 Y 6c 8 Y 6c 11.75 .
4 Y 6c 9 Y 6c 11.75 .
5 Y 6c 6 Y 6c 3.54 .
5 Y 6c 7 Y 6c 3.57 .
5 Y 6c 8 Y 6c 8.91 .
5 Y 6c 9 Y 6c 6.16 .
6 Y 6c 7 Y 6c 5.77 .
6 Y 6c 8 Y 6c 11.54 .
6 Y 6c 9 Y 6c 8.91 .
7 Y 6c 8 Y 6c 5.77 .
7 Y 6c 9 Y 6c 3.57 .
8 Y 6c 9 Y 6c 3.54 .
Jij: magnetic exchange parameter between site i and j (Individual Jij values are temporarily not available while we perform maintenance.)
Terms and conditions

Pair-resolved magnetic exchange parameters:


Diagram is not available for this entry.

Individual exchange parameters:


Diagram is not available for this entry.

Methods:

DFT calculations

  • exchange-correlation energy functional: GGA-PBE
  • pseudopotential type: PAW
  • cutoff energy: 65.0 Ry
  • k-point grid: (kx, ky, kz) = (None, None, None) for magnetic anisotropy calculations
  • package: QE (v6.3)

LMTO-GF calculations

  • k-point grid: (kx, ky, kz) =
  • energy mesh: 41 points on an elliptical contour
  • package: Questaal (v7)

References:

References

Materials Project: mp-1187739


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