Average positions and magnetic moments of all atoms in unit cell, with magnetic moment relations explicitly given:
Average atomic positions of symmetry independent atomsMagnetic atoms:
Set of atoms in the unit cell related by symmetry with the magnetic atom Cr1_1:
Average atomic positions
| Atom | x | y | z |
| 1 | 0.00000 | 0.00000 | 0.00000 |
| 2 | 0.50000 | 0.50000 | 0.00000 |
| 3 | 0.00000 | 0.00000 | 0.50000 |
| 4 | 0.50000 | 0.50000 | 0.50000 |
Magnetic moment modulation parametersWave vector 1
| Atom | Magnetic moment Fourier Cos coeffs | Magnetic moment Fourier Sin coeffs |
|---|
| Symmetry constraints | Numerical values | Symmetry constraints | Numerical values |
|---|
| x | y | z | x | y | z | x | y | z | x | y | z |
|---|
| 1 | Mxcos1 | Mycos1 | Mzcos1 | 1.55000 | 0.0 | 0.0 | Mxcos1+Mysin1 | Mycos1+Mysin1 | Mzcos1+Mysin1 | 0.0 | 0.0 | -1.55000 |
| 2 | -Mxcos1 | Mycos1 | Mzcos1 | -1.55000 | 0.0 | 0.0 | Mxcos1+Mysin1 | -Mycos1-Mysin1 | -Mzcos1-Mysin1 | 0.0 | 0.0 | 1.55000 |
| 3 | -Mxcos1 | -Mycos1 | Mzcos1 | -1.55000 | 0.0 | 0.0 | Mxcos1+Mysin1 | Mycos1+Mysin1 | -Mzcos1-Mysin1 | 0.0 | 0.0 | 1.55000 |
| 4 | Mxcos1 | -Mycos1 | Mzcos1 | 1.55000 | 0.0 | 0.0 | Mxcos1+Mysin1 | -Mycos1-Mysin1 | Mzcos1+Mysin1 | 0.0 | 0.0 | -1.55000 |
Set of atoms in the unit cell related by symmetry with the magnetic atom Cr2_1:
Average atomic positions
| Atom | x | y | z |
| 1 | 0.49500 | 0.23200 | 0.75000 |
| 2 | 0.99500 | 0.26800 | 0.25000 |
Magnetic moment modulation parametersWave vector 1
| Atom | Magnetic moment Fourier Cos coeffs | Magnetic moment Fourier Sin coeffs |
|---|
| Symmetry constraints | Numerical values | Symmetry constraints | Numerical values |
|---|
| x | y | z | x | y | z | x | y | z | x | y | z |
|---|
| 1 | 0 | 0 | Mzcos1 | 0.0 | 0.0 | -2.75000 | Mxcos1+Mysin1 | Mycos1+Mysin1 | 0 | -2.75000 | 0.0 | 0.0 |
| 2 | 0 | 0 | Mzcos1 | 0.0 | 0.0 | -2.75000 | Mxcos1+Mysin1 | -Mycos1-Mysin1 | 0 | -2.75000 | 0.0 | 0.0 |
Set of atoms in the unit cell related by symmetry with the magnetic atom Cr2_2:
Average atomic positions
| Atom | x | y | z |
| 1 | 0.00500 | 0.73200 | 0.75000 |
| 2 | 0.50500 | 0.76800 | 0.25000 |
Magnetic moment modulation parametersWave vector 1
| Atom | Magnetic moment Fourier Cos coeffs | Magnetic moment Fourier Sin coeffs |
|---|
| Symmetry constraints | Numerical values | Symmetry constraints | Numerical values |
|---|
| x | y | z | x | y | z | x | y | z | x | y | z |
|---|
| 1 | 0 | 0 | Mzcos1 | 0.0 | 0.0 | 2.75000 | Mxcos1+Mysin1 | Mycos1+Mysin1 | 0 | 2.75000 | 0.0 | 0.0 |
| 2 | 0 | 0 | Mzcos1 | 0.0 | 0.0 | 2.75000 | Mxcos1+Mysin1 | -Mycos1-Mysin1 | 0 | 2.75000 | 0.0 | 0.0 |
Non-magnetic atoms:
Set of atoms in the unit cell related by symmetry with the atom Be1_1:
| Atom | x | y | z |
| 1 | 0.93100 | 0.40600 | 0.75000 |
| 2 | 0.43100 | 0.09400 | 0.25000 |
Set of atoms in the unit cell related by symmetry with the atom Be1_2:
| Atom | x | y | z |
| 1 | 0.56900 | 0.90600 | 0.75000 |
| 2 | 0.06900 | 0.59400 | 0.25000 |
Set of atoms in the unit cell related by symmetry with the atom O1_1:
| Atom | x | y | z |
| 1 | 0.27700 | 0.40700 | 0.75000 |
| 2 | 0.77700 | 0.09300 | 0.25000 |
Set of atoms in the unit cell related by symmetry with the atom O1_2:
| Atom | x | y | z |
| 1 | 0.22300 | 0.90700 | 0.75000 |
| 2 | 0.72300 | 0.59300 | 0.25000 |
Set of atoms in the unit cell related by symmetry with the atom O2_1:
| Atom | x | y | z |
| 1 | 0.73100 | 0.06100 | 0.75000 |
| 2 | 0.23100 | 0.43900 | 0.25000 |
Set of atoms in the unit cell related by symmetry with the atom O2_2:
| Atom | x | y | z |
| 1 | 0.76900 | 0.56100 | 0.75000 |
| 2 | 0.26900 | 0.93900 | 0.25000 |
Set of atoms in the unit cell related by symmetry with the atom O3_1:
| Atom | x | y | z |
| 1 | 0.25700 | 0.16200 | 0.02200 |
| 2 | 0.75700 | 0.33800 | 0.97800 |
| 3 | 0.25700 | 0.16200 | 0.47800 |
| 4 | 0.75700 | 0.33800 | 0.52200 |
Set of atoms in the unit cell related by symmetry with the atom O3_2:
| Atom | x | y | z |
| 1 | 0.24300 | 0.66200 | 0.47800 |
| 2 | 0.74300 | 0.83800 | 0.52200 |
| 3 | 0.24300 | 0.66200 | 0.02200 |
| 4 | 0.74300 | 0.83800 | 0.97800 |
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