Description of spin spirals
Spin spirals are periodic magnetic structures that can be described by a vector field. For a rotation axis along the z direction their magnetization is given by:
where is the lattice vector pointing from the origin to unit cell , is the position of atom in the unit cell, is the so called spin-spiral vector, is the cone angle between the magnetic moment of atom and the rotation axis, and is an atom-dependent phase shift.
In general, the period length can be many times larger than a lattice period. Hence it is not feasible to simulate a spin spiral directly because one would need to use extremely large supercells. However, in the absence of spin-orbit coupling, the generalised Bloch theorem allows to overcome this problem. The theorem states that a wave function of a system featuring a spin spiral can be represented as
where and are unit-cell-periodic functions.
In Fleur the description of spin spirals is part of the code treating noncollinear magnetism . This implies that
one should invoke the input generator with the
-explicit command line switches to obtain
templates for the parametrization of calculations on noncollinear magnetism. Next, the treatment of noncollinear
magnetism has to be activated by setting
T. The angles
and are set in the
To finally switch on the calculation of a spin spiral by employing the generalized Bloch theorem also
has to be set to
T. The following example demonstrates such a setting.
<magnetism jspins="2" l_noco="T" l_ss="T">
<qss>0.25 0.25 0.0</qss>
The vector is set in the
qss tag enclosed by
calculationSetup/magnetism and measured in
reciprocal lattice vectors.
To ensure that the symmetry operations found for the unit cell are not incompatible to the vector, the inpgen
input should be extended by a line specifying the vector. For the here-considered this line
&qss 0.25 0.25 0.0 /.
Under the assumption that the setup in the example above belongs to an fcc unit cell with the Bravais matrix
the reciprocal unit cell would be defined by the matrix
which defines a bcc-like structure. This implies that the defined would point in z direction for this example.
The magnetic moment of an atom at position (internal coordinates) is rotated by . For the given example and this implies that an increase of the vector to would yield a layered structure with an antiferromagnetic alignment of the magnetization directions along z.
The following figure demonstrates different spin spirals that may be obtained with respective parametrizations in the Fleur input file.
In the absence of spin-orbit coupling (SOC) the direction of the rotation axis is energetically irrelevant, therefore the first and third spin-spiral in the figure are equivalent (the same applies to the second and fourth one). For convenience, if no SOC is considered the rotation axis is always set to point in z-direction. I.e., if the magnetization of an atom points along z, it will not rotate. If it points in x-direction (), it describes a flat spiral (second example of the figure).
The description of spin spirals in this way is incompatible to the inclusion of spin-orbit coupling in the calculation. If spin spirals have to be calculated under consideration of SOC this can be done by employing the magnetic force theorem.
Like all other calculations on noncollinear magnetism, spin-spiral calculations are incompatible to the
exact treatment of the core-electron tails reaching out of the MT spheres. Thus
to be set to
Since the number of basis functions changes (slightly) with , for consistent output quantities it is important that the basis cutoff () is not too small, typically increased by 0.5 - 1.0 as compared to normal non-collinear calculations. Also, a dense -grid is recommended when sampling space, usually twice as dense as the -grid works best .