Spin with PWscf
From version 2.26 of c2x, the Quantum Espresso support is sufficient for the following example.
FeO.in
&CONTROL calculation = 'scf', outdir = '.', pseudo_dir = '.' / &SYSTEM ibrav = 0, nat = 4, ntyp = 3, nspin = 2, starting_magnetization(1) = 0.000000, starting_magnetization(2) = 2.000000, starting_magnetization(3) = -2.000000, ! c2x default occupations = 'smearing', ! c2x default degauss = 0.05, ecutwfc = 30 / &ELECTRONS / CELL_PARAMETERS angstrom 0.0000000 4.3320000 4.3320000 2.1660000 0.0000000 2.1660000 2.1660000 2.1660000 0.0000000 ATOMIC_SPECIES O 1.0 O.UPF Fe 1.0 Fe.UPF Fe1 1.0 Fe.UPF ATOMIC_POSITIONS crystal O 0.250000000 0.500000000 0.500000000 O 0.750000000 0.500000000 0.500000000 Fe 0.000000000 0.000000000 0.000000000 Fe1 0.500000000 0.000000000 0.000000000 K_POINTS automatic 2 3 3 1 0 0
One can then download suitable pseudopotentials:
$ curl -o Fe.UPF https://pseudopotentials.quantum-espresso.org/upf_files/Fe.pz-nd-rrkjus.UPF $ curl -o O.UPF https://pseudopotentials.quantum-espresso.org/upf_files/O.pz-rrkjus.UPF
and run pwcsf
$ pw.x -in FeO.in > FeO.log
Visualisation
Now one can analyse and visualise the results. In this case we choose to expand the system back to a cubic cell.
$ c2x -sv -X='(8.664,0,0)(0,8.664,0)(0,0,8.664)' pwscf.xml FeO.spin.xsf QE binary reader called grid extent in file -20:20,-10:10,-10:10 FFT grid used 45x24x24 Cell volume 40.647642 natoms 4 Total ionic charge 28.000000 Requested cut-off energy 408.171 eV First FFT grid 45 24 24 spins=2 spinors=1 Found 3D data for Spin min=-4.31065 max=4.36473 sum=0.253148 int=0.000396986 int|s|=7.06716 (integral is e per cell for charge and spin densities) New cell volume 0.001538 (0.0625 times old) Warning: unable to convert k points to new cell New cell volume 650.362259 (16 times old) New FFT grid is 72 72 72
Note that the spin density has its maximum and minimum of almost equal magnitude, and opposite sign. The value of int|s| implies a magnetic moment per Fe atom of 3.53μB, which is consistent with the literature.
Again alternating layers of spin clearly seen, and this time the cubic nature of the lattice is more apparent.