Merge pull request #2714 from julient31/STT2
Improvement of the SPIN package by removing a limitation
This commit is contained in:
@ -12,7 +12,7 @@ Syntax
|
||||
|
||||
* ID, group are documented in :doc:`fix <fix>` command
|
||||
* precession/spin = style name of this fix command
|
||||
* style = *zeeman* or *anisotropy* or *cubic*
|
||||
* style = *zeeman* or *anisotropy* or *cubic* or *stt*
|
||||
|
||||
.. parsed-literal::
|
||||
|
||||
@ -22,12 +22,12 @@ Syntax
|
||||
*anisotropy* args = K x y z
|
||||
K = intensity of the magnetic anisotropy (in eV)
|
||||
x y z = vector direction of the anisotropy
|
||||
|
||||
.. parsed-literal::
|
||||
|
||||
*cubic* args = K1 K2c n1x n1y n1x n2x n2y n2z n3x n3y n3z
|
||||
K1 and K2c = intensity of the magnetic anisotropy (in eV)
|
||||
n1x to n3z = three direction vectors of the cubic anisotropy
|
||||
*stt* args = J x y z
|
||||
J = intensity of the spin-transfer torque field
|
||||
x y z = vector direction of the field
|
||||
|
||||
Examples
|
||||
""""""""
|
||||
@ -125,6 +125,11 @@ axis along the :math:`(1 1 1)`-type cube diagonals). :math:`K_2^c >
|
||||
diagonals. See chapter 2 of :ref:`(Skomski) <Skomski1>` for more
|
||||
details on cubic anisotropies.
|
||||
|
||||
Style *stt* is used to simulate the interaction between the spins and
|
||||
a spin-transfer torque.
|
||||
See equation (7) of :ref:`(Chirac) <Chirac1>` for more details about the
|
||||
implemented spin-transfer torque term.
|
||||
|
||||
In all cases, the choice of :math:`(x y z)` only imposes the vector
|
||||
directions for the forces. Only the direction of the vector is
|
||||
important; its length is ignored (the entered vectors are
|
||||
@ -132,6 +137,16 @@ normalized).
|
||||
|
||||
Those styles can be combined within one single command line.
|
||||
|
||||
.. note::
|
||||
|
||||
The norm of all vectors defined with the precession/spin command
|
||||
have to be non-zero. For example, defining
|
||||
"fix 1 all precession/spin zeeman 0.1 0.0 0.0 0.0" would result
|
||||
in an error message.
|
||||
Since those vector components are used to compute the inverse of the
|
||||
field (or anisotropy) vector norm, setting a zero-vector would result
|
||||
in a division by zero.
|
||||
|
||||
----------
|
||||
|
||||
Restart, fix_modify, output, run start/stop, minimize info
|
||||
@ -162,11 +177,6 @@ is only enabled if LAMMPS was built with this package, and if the
|
||||
atom_style "spin" was declared. See the :doc:`Build package
|
||||
<Build_package>` doc page for more info.
|
||||
|
||||
The *precession/spin* style can only be declared once. If more than
|
||||
one precession type (for example combining an anisotropy and a Zeeman
|
||||
interactions) has to be declared, they have to be chained in the same
|
||||
command line (as shown in the examples above).
|
||||
|
||||
Related commands
|
||||
""""""""""""""""
|
||||
|
||||
@ -184,3 +194,9 @@ none
|
||||
|
||||
**(Skomski)** Skomski, R. (2008). Simple models of magnetism.
|
||||
Oxford University Press.
|
||||
|
||||
.. _Chirac1:
|
||||
|
||||
**(Chirac)** Chirac, Théophile, et al. Ultrafast antiferromagnetic
|
||||
switching in NiO induced by spin transfer torques.
|
||||
Physical Review B 102.13 (2020): 134415.
|
||||
|
||||
Reference in New Issue
Block a user