Syntax
atomList = atom(obj)
Description
atomList = atom(obj)
generates all atomic positions using the symmetry
operators stored in obj.lattice.sym
and the symmetry inequivalent
atomic positions in obj.unit_cell.r
. If no symmetry is defined (denoted
\(P0\) symmetry) or the symmetry is \(P1\) the function returns simply the
positions stored in obj.unit_cell.r
.
Examples
Here we create a new space group, that contains all the translations of
the FCC lattice. Then create a crystal with an atom at [0 0 0]
position.
The cryst.atom
lists all 4 symmetry equivalent positions generated using
the FCC symmetry operators:
cryst = spinw
opStr = 'x+1/2,y+1/2,z;x+1/2,y,z+1/2;x,y+1/2,z+1/2';
cryst.genlattice('lat_const',[8 8 8],'spgr',opStr,'label','FCC')
cryst.addatom('r',[0 0 0],'label','Atom1')
atomList = cryst.atom
atomList.r
Output
0 0.5000 0.5000 0
0 0.5000 0 0.5000
0 0 0.5000 0.5000
Input Arguments
obj
- spinw object.
Output Arguments
atomList
is a structure with the following fields:
r
Positions of the atoms in lattice units stored in matrix with dimensions of \([3\times n_{atom}]\).idx
Indices of the atoms in the spinw.unit_cell field stored in a matrix with dimensions of \([1\times n_{atom}]\).mag
Vector of logical variables,true
if the spin of the atom is non-zero, dimensions are \([1\times n_{atom}]\).
See Also
spinw | spinw.matom | swsym.add | spinw.genlattice | spinw.addatom