| ... | ... | @@ -10,14 +10,14 @@ as usual. The following steps are needed: |
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## Changes in the inputcard
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The options *NEWSOSOL* and *fullBZ* have to be set in the inputcard.
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The options `NEWSOSOL` and `fullBZ` have to be set in the inputcard.
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This tells the program to use the new solver and to forget about all
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symmetries previously found for the current setup. This is needed since
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SOC may break some symmetries. In addition some parameters for the
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newsolver have to be set. These are *NPAN_LOG*, *NPAN_EQ*,
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*NCHEB* and *R_LOG*. Also do not forget to do spin-polarized
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calculations for full potential (*NSPIN=2, KSHAPE=2*). If you started
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with a calculation without spin-polarization, i.e. *NSPIN=1*, you can
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newsolver have to be set. These are `NPAN_LOG`, `NPAN_EQ`,
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`NCHEB` and `R_LOG`. Also do not forget to do spin-polarized
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calculations for full potential (`NSPIN= 2, KSHAPE= 2`). If you started
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with a calculation without spin-polarization, i.e. `NSPIN= 1`, you can
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[adopt your already converged potential](change_nspin_1_to_2).
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```
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RUNOPT
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| ... | ... | @@ -55,7 +55,7 @@ Since the new solver does also deal with non-collinear calculations we |
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have to specify the non-collinear angles of each atom in the inputcard
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in the file [nonco_angle.dat](nonco_angle.dat_file). If
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this file is not given then the angles are fixed to theta=phi=0 (i.e.
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the z-direction).
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the *z*-direction).
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## Examples
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| ... | ... | @@ -63,9 +63,9 @@ the z-direction). |
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As an example the difference between bulk Au with and without SOC should
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be calculated. The test system consists of bulk Au (fcc lattice) with a
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LMAX cutoff set to 2 and a k-mesh of 15x15x15, for the sake of speed of
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`LMAX= 2` cutoff and a *k*-mesh of 15x15x15, for the sake of speed of
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the calculation.
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`{{:jumu/examples:au_bulk_nosoc_cos.tar.gz|Here}}`{=mediawiki} the input
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[Here](uploads/c9fb791a2f0f81c59ce73e77346fddbf/au_bulk_nosoc_cos.tar.gz) the input
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files of both cases with the different inputcards can be found. Using
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the [QDOS](jumu/qdos) the change in the band structure can be
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investigated.
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