[Wien] Convergence problem

tran at theochem.tuwien.ac.at tran at theochem.tuwien.ac.at
Tue Dec 30 10:52:30 CET 2014


Hi,

The struct file that I used is attached. For my purpose, the size of
the unit cell was large enough to avoid spurious interactions between
neighbouring cells. Note that a, b and c are different in order to avoid
to high symmetry.

F. Tran

On Mon, 29 Dec 2014, Muhammad Sajjad wrote:

> Dear Prof. Marks and F. TranThank you so much for your helpful suggestions. I was already doing the spin polarization calculations. I have got the convergence
> by using
> mixing factor 0.1, starting calculation with PRATT and then switched to MSR1 after 7 cycles, and the command runsp_lapw -cc 0.00001 -in1ef -i 150
> The obtained magnetic moment was 2.00009.
> 
> Dear Tran I would really appreciate if you share some more details about case.struct file. It will definitely be helpful for me as well as for others. 
> 
> Kind Regards
> Dr. Sajjad
> 
> On Mon, Dec 29, 2014 at 3:50 AM, <tran at theochem.tuwien.ac.at> wrote:
>       The calculation for an isolated atom with a code which uses periodic
>       boundary conditions (like WIEN2k) is not trivial. This is what I have done
>       recently for most atoms of the periodic table (excluding f-systems), and
>       for some of the transition-metal atoms this was extremely difficult to
>       achieve convergence.
>
>       A few hints (that I used):
>
>       1) It is important (and necessary depending on the atom) to reduce the
>       symmetry from cubic to, e.g., orthorhombic to be able to access the
>       electronic configuration with the lowest energy (this is the procedure
>       followed by several research groups like VASP for instance).
>       If necessary I can give more details about the case.struct that I used.
>
>       2) lapw0 requires a lot of memory, while lapw1 requires both
>       memory and time. To reduce computer time for lapw1, I was using
>       iterative digonalization (this was my command for all atoms):
>       runsp_lapw -ec 0.0001 -cc 0.0001 -it -i 1000 -NI
>
>       3) For the Ni atom the magnetic moment should be 2:
>       :MMTOT:  SPIN MAGNETIC MOMENT IN CELL     =    2.00238
>
>       4) I was using the default setting for mixer.
>
>       F. Tran
>
>       On Sun, 28 Dec 2014, Laurence Marks wrote:
> 
>
>             Also, only 1 k-point (Gamma), an RMT and RKMax similar to what you use for
>             bulk Ni, particularly as I assume you are doing the calculation to get an
>             enthalpy of formation. You may have to use the mpi versions as it is
>             probably too large for a non-mpi run.
>
>             If you are doing WC+U (or -ineece) the U (or on-site hybrid) removes the
>             phase transition so convergence should be simple.
>
>             Straight WC is not a simple calculation because the physics for an isolated
>             Ni atom is wrong. With wrong physics there is in fact no guarantee that the
>             calculation will ever converge!
>
>             ___________________________
>             Professor Laurence Marks
>             Department of Materials Science and Engineering
>             Northwestern University
>             www.numis.northwestern.edu
>             MURI4D.numis.northwestern.edu
>             Co-Editor, Acta Cryst A
>             "Research is to see what everybody else has seen, and to think what nobody
>             else has thought"
>             Albert Szent-Gyorgi
>
>             On Dec 28, 2014 11:47 AM, "Laurence Marks" <L-marks at northwestern.edu> wrote:
>
>                   You almost certainly need to run spin polarized, probably MSR1
>                   (GREED 0.1), TEMPS (room temp). The convergence is complicated
>                   for WC (& simple GGAs) due to an electronic phase transition
>                   between sp & d occupation near the fixed point.
>
>                   ___________________________
>                   Professor Laurence Marks
>                   Department of Materials Science and Engineering
>                   Northwestern University
>                   www.numis.northwestern.edu
>                   MURI4D.numis.northwestern.edu
>                   Co-Editor, Acta Cryst A
>                   "Research is to see what everybody else has seen, and to think
>                   what nobody else has thought"
>                   Albert Szent-Gyorgi
>
>                   On Dec 28, 2014 10:47 AM, "Muhammad Sajjad" <sajjadpu at gmail.com>
>                   wrote:
>                         Dear Users I am running SCF calculation for Ni with
>                         lattice constant of 30 Bohr and using WC-GGA. The
>                         calculation is not converging even upto 100
>                         iterations and more. To solve the problem I have
>                         performed following steps
>
>             switched to TEMPS = 0.005 from TETRA
>             Changed MSR1 to PRATT
>             changed mixing factor (increase and decrease from 0.2)
>
>             Thanking in advance. 
>
>             Dr. Sajjad
> 
> 
> 
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> 
> 
>
-------------- next part --------------
Ni                                                                             
P   LATTICE,NONEQUIV.ATOMS:  1                                                 
MODE OF CALC=RELA unit=ang                                                     
 18.897269 18.991755 19.086241 90.000000 90.000000 90.000000                   
ATOM  -1: X=0.00000000 Y=0.00000000 Z=0.00000000
          MULT= 1          ISPLIT= 8
Ni         NPT=  781  R0=0.00005000 RMT=    1.8000   Z: 28.0                   
LOCAL ROT MATRIX:    1.0000000 0.0000000 0.0000000
                     0.0000000 1.0000000 0.0000000
                     0.0000000 0.0000000 1.0000000
   8      NUMBER OF SYMMETRY OPERATIONS
-1 0 0 0.00000000
 0-1 0 0.00000000
 0 0-1 0.00000000
       1
-1 0 0 0.00000000
 0-1 0 0.00000000
 0 0 1 0.00000000
       2
-1 0 0 0.00000000
 0 1 0 0.00000000
 0 0-1 0.00000000
       3
-1 0 0 0.00000000
 0 1 0 0.00000000
 0 0 1 0.00000000
       4
 1 0 0 0.00000000
 0-1 0 0.00000000
 0 0-1 0.00000000
       5
 1 0 0 0.00000000
 0-1 0 0.00000000
 0 0 1 0.00000000
       6
 1 0 0 0.00000000
 0 1 0 0.00000000
 0 0-1 0.00000000
       7
 1 0 0 0.00000000
 0 1 0 0.00000000
 0 0 1 0.00000000
       8


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