I CONSTRAINED M: Difference between revisions
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VASP offers the possibility to add a penalty contribution to the total energy expression (and consequently a penalty functional to the Hamiltonian) that drives the local magnetic moment (integral of the magnetization in a site centered sphere of radius ''r''={{TAG|RWIGS}}) into a direction given by the {{TAG|M_CONSTR}}-tag. | VASP offers the possibility to add a penalty contribution to the total energy expression (and consequently a penalty functional to the Hamiltonian) that drives the local magnetic moment (integral of the magnetization in a site centered sphere of radius ''r''={{TAG|RWIGS}}) into a direction given by the {{TAG|M_CONSTR}}-tag. | ||
*{{TAG|I_CONSTRAINED_M}}=1 | *{{TAG|I_CONSTRAINED_M}}=1: Constrain the ''direction'' of the magnetic moments. | ||
:Constrain the direction of the magnetic moments. The total energy is given by | :The total energy is given by | ||
::<math>E=E_0+ \sum_I\lambda \left[ \vec{M}_I-\hat{M}^0_I \left( \hat{M}^0_I \cdot \vec{M_I}\right)\right]^2</math> | ::<math>E=E_0+ \sum_I\lambda \left[ \vec{M}_I-\hat{M}^0_I \left( \hat{M}^0_I \cdot \vec{M_I}\right)\right]^2</math> | ||
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:where <math>\vec{\sigma}=(\sigma_x,\sigma_y,\sigma_z)</math> are the Pauli spin-matrices. | :where <math>\vec{\sigma}=(\sigma_x,\sigma_y,\sigma_z)</math> are the Pauli spin-matrices. | ||
*{{TAG|I_CONSTRAINED_M}}=2 | *{{TAG|I_CONSTRAINED_M}}=2: Constrain the ''size and direction'' of the magnetic moments. | ||
:The total energy is given by | |||
::<math>E=E_0+ \sum_I\lambda \left( \vec{M}_I-\vec{M}^0_I \right)^2</math> | |||
:where <math>\vec{M}^0_I</math> is the desired magnetic moment at site ''I'' (as specified using {{TAG|M_CONSTR}}). | |||
:The additional potential that arises from the penalty contribution to the total energy is given by | |||
::<math>V_I (\mathbf{r})=2\lambda \left( \vec{M}_I-\vec{M}^0_I \right)\cdot \vec{\sigma} F_I(|\mathbf{r}|)</math> | |||
== Related Tags and Sections == | == Related Tags and Sections == |
Revision as of 16:32, 16 February 2011
I_CONSTRAINED_M = 1 | 2
Default: I_CONSTRAINED_M = none
Description: I_CONSTRAINED_M switches on the constrained local moments approach.
VASP offers the possibility to add a penalty contribution to the total energy expression (and consequently a penalty functional to the Hamiltonian) that drives the local magnetic moment (integral of the magnetization in a site centered sphere of radius r=RWIGS) into a direction given by the M_CONSTR-tag.
- I_CONSTRAINED_M=1: Constrain the direction of the magnetic moments.
- The total energy is given by
- where E0 is the usual DFT energy, and the second term on the right-hand-side represents the penalty. The sum is taken over all atomic sites I, is the desired direction of the magnetic moment at site I (as specified using M_CONSTR), and is the integrated magnetic moment inside a sphere ΩI (the radius must be specified by means of RWIGS) around the position of atom I,
- where FI(|r|) is a function of norm 1 inside ΩI, that smoothly goes to zero towards the boundary of ΩI.
- The penalty term in the total energy introduces an additional potential inside the aforementioned spheres centered at the atomic sites I, given by
- where are the Pauli spin-matrices.
- I_CONSTRAINED_M=2: Constrain the size and direction of the magnetic moments.
- The total energy is given by
- where is the desired magnetic moment at site I (as specified using M_CONSTR).
- The additional potential that arises from the penalty contribution to the total energy is given by
Related Tags and Sections
M_CONSTR, LAMBDA, RWIGS, LNONCOLLINEAR