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Commit Date  
[r305] by paulatz

Raise error when argument is expected but not present

2017-06-29 09:18:35 Tree
[r304] by paulatz

Two changes:
1. grid shift can now be specified in input (xk0 and xk0_in), as a fraction of half the grid step
2. progress of long calculations improved, it now prints time and percent istead of the list of points

2017-06-28 18:31:09 Tree
[r303] by paulatz

Added a small bash script that applies the sum rule directly to the fildyn files

Also, previous tools improved slightly

2017-06-28 07:57:16 Tree
[r302] by paulatz

Better stopping on error

2017-06-27 11:52:39 Tree
[r301] by paulatz

New debug option to write D3 matrices that do not match after imag part of FCs has been stripped

2017-06-27 11:49:36 Tree
[r300] by paulatz

Possibility to do a calculation with nbnd_occ = nbnd, added as debug option

2017-06-27 11:49:04 Tree
[r299] by paulatz

alignment fix

2017-06-26 14:52:36 Tree
[r298] by paulatz

quick return of the ij term when the fermi shift is zero (i.e.e high symmetry crystal)

2017-06-26 14:52:29 Tree
[r297] by paulatz

better code alignment

--This line, and thos below, will be ignored--

M incdrhoscf2.f90

2017-06-26 14:51:41 Tree
[r296] by paulatz

Tentative try to get the same result with nbnd_occ = nbnd and without, also without breaking the code in the insulating case when nbnd>nelec/2

I'm relatively convinced that the correct nbnd_occ to use in solve linter is the one at ik_wfc (i.e. at k) and not at ik_prj (i.e. k-q in the simple case), but I'm not 100% sure. However, it does go much better like this

Also, it is still not perfect, and there are more residualse in the FFT when using this with respect to using nbnd_occ=nbnd

2017-06-26 14:51:12 Tree
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