This is tricky, particularly as something in your email triggered
gmail's spam filter.

More information than you want to know. A change was made in Wien2k 11
was made to improve the orthogonality of the orbitals, to get rid of
what I call "ghost forces" that showed up with MSR1a. These are
sudden, anomalously large valence forces that occurred. When this
change was made Peter was concerned that this might lead to a "LOPW
plane wave exhausted" problem that you are seeing for very high
symmetry structures.

Probably you can solve this by just increasing RKMAX to 8 or 9 from
the default of 7. This increases the number of plane waves so should
cure the problem.

On Tue, Jul 26, 2011 at 4:49 AM, pascal boulet
<pascal.boulet at univ-provence.fr> wrote:
>
> -----BEGIN PGP SIGNED MESSAGE-----
>
>
> Dear all,
>
> I am trying to set up calculations on a Gamma brass structure. The
> problem is that W2K (version 11) stops with the error 'LOPW plane waves
> exhausted' in lapw1. The topic has already been reported on the list
> (Feb. 2011) but the answers there are not very clear to me. Here is what
> I am doing.
>
> So, I am starting with Copper with a gamma brass structure (group number
> 217). ?The structure generated by W2K from a CIF file (4 inequivalent
> positions) looks correct. The local symmetry of the atomic sites agrees
> with that given on the Bilbao website.
>
> Now comes the generation of the atomic densities. According to the
> electronic structure of Cu which is:
>
> ? ? ? ? E-up(Ry) ? ? ?E-dn(Ry) ? Occupancy ? q/sphere ?core-state
> ?1S ? ?-650.760163 ? -650.760146 ?1.00 ?1.00 ? ?1.0000 ?T
> ?2S ? ? -78.505196 ? ?-78.461906 ?1.00 ?1.00 ? ?1.0000 ?T
> ?2P* ? ?-68.813819 ? ?-68.782078 ?1.00 ?1.00 ? ?1.0000 ?T
> ?2P ? ? -67.308434 ? ?-67.275562 ?2.00 ?2.00 ? ?1.0000 ?T
> ?3S ? ? ?-8.856436 ? ? -8.771764 ?1.00 ?1.00 ? ?0.9999 ?F
> ?3P* ? ? -5.848176 ? ? -5.764727 ?1.00 ?1.00 ? ?0.9996 ?F
> ?3P ? ? ?-5.655968 ? ? -5.573289 ?2.00 ?2.00 ? ?0.9995 ?F
> ?3D* ? ? -0.747458 ? ? -0.672780 ?2.00 ?2.00 ? ?0.9718 ?F
> ?3D ? ? ?-0.725704 ? ? -0.651398 ?3.00 ?2.00 ? ?0.9708 ?F
> ?4S ? ? ?-0.433190 ? ? -0.420827 ?1.00 ?1.00 ? ?0.4335 ?F
>
> I choose the core-valence energy separation to be -10 Ry because the
> default -6.0 Ry would separate the 3s and the 3p states which does not
> seem wise to me. I think this is what is done in the example for Zn in
> the manual. Is it correct to choose -10 Ry?
>
> Here is a sample of the file case.in1c obtained automatically using w2web:
>
> WFFIL ?EF= 0.50000 ? ? ? (WFFIL, WFPRI, ENFIL, SUPWF)
> ?7.00 ? ? ? 10 ? ?4 (R-MT*K-MAX; MAX L IN WF, V-NMT
> ?0.30 ? ?5 ?0 ? ? ?(GLOBAL E-PARAMETER WITH n OTHER CHOICES, global
> APW/LAPW)
> ?0 ? ?0.30 ? ? ?0.000 CONT 1
> ?0 ? -8.56 ? ? ?0.001 STOP 1
> ?1 ? ?0.30 ? ? ?0.000 CONT 1
> ?1 ? -5.36 ? ? ?0.001 STOP 1
> ?2 ? ?0.30 ? ? ?0.005 CONT 1
> etc. for the other 3 atoms.
>
> which I changed to:
>
> WFFIL ?EF= 0.50000 ? ? ? (WFFIL, WFPRI, ENFIL, SUPWF)
> ?7.00 ? ? ? 10 ? ?4 (R-MT*K-MAX; MAX L IN WF, V-NMT
> ?0.30 ? ?5 ?0 ? ? ?(GLOBAL E-PARAMETER WITH n OTHER CHOICES, global
> APW/LAPW)
> ?0 ? ?0.30 ? ? ?0.000 CONT 0
> ?0 ? -8.56 ? ? ?0.001 STOP 0
> ?1 ? ?0.30 ? ? ?0.000 CONT 0
> ?1 ? -5.36 ? ? ?0.001 STOP 0
> ?2 ? ?0.30 ? ? ?0.005 CONT 1
>
> in order to match the example for TiO2. Whether I change the file or not
> does not change the final result anyway, I mean the crash!
>
> In the mailing-list it is suggested to increase RKmax, which I did up to
> 9. No change.
>
> For information here is the cif file of the structure:
> data_generated_by_bilbao_crystallographic_server
>
> _cell_length_a ? ? ? ? ? ? ? ? ? 8.878
> _cell_length_b ? ? ? ? ? ? ? ? ? 8.878
> _cell_length_c ? ? ? ? ? ? ? ? ? 8.878
> _cell_angle_alpha ? ? ? ? ? ? ? ?90
> _cell_angle_beta ? ? ? ? ? ? ? ? 90
> _cell_angle_gamma ? ? ? ? ? ? ? ?90
> _symmetry_space_group_name_H-M ? 'I-43m'
> _symmetry_Int_Tables_number ? ? ?217
>
> loop_
> _symmetry_equiv_pos_site_id
> _symmetry_equiv_pos_as_xyz
> 1 ? ?'x,y,z'
> 2 ? ?'-x,-y,z'
> 3 ? ?'-x,y,-z'
> 4 ? ?'x,-y,-z'
> 5 ? ?'z,x,y'
> 6 ? ?'z,-x,-y'
> 7 ? ?'-z,-x,y'
> 8 ? ?'-z,x,-y'
> 9 ? ?'y,z,x'
> 10 ? '-y,z,-x'
> 11 ? 'y,-z,-x'
> 12 ? '-y,-z,x'
> 13 ? 'y,x,z'
> 14 ? '-y,-x,z'
> 15 ? 'y,-x,-z'
> 16 ? '-y,x,-z'
> 17 ? 'x,z,y'
> 18 ? '-x,z,-y'
> 19 ? '-x,-z,y'
> 20 ? 'x,-z,-y'
> 21 ? 'z,y,x'
> 22 ? 'z,-y,-x'
> 23 ? '-z,y,-x'
> 24 ? '-z,-y,x'
> 25 ? 'x+1/2,y+1/2,z+1/2'
> 26 ? '-x+1/2,-y+1/2,z+1/2'
> 27 ? '-x+1/2,y+1/2,-z+1/2'
> 28 ? 'x+1/2,-y+1/2,-z+1/2'
> 29 ? 'z+1/2,x+1/2,y+1/2'
> 30 ? 'z+1/2,-x+1/2,-y+1/2'
> 31 ? '-z+1/2,-x+1/2,y+1/2'
> 32 ? '-z+1/2,x+1/2,-y+1/2'
> 33 ? 'y+1/2,z+1/2,x+1/2'
> 34 ? '-y+1/2,z+1/2,-x+1/2'
> 35 ? 'y+1/2,-z+1/2,-x+1/2'
> 36 ? '-y+1/2,-z+1/2,x+1/2'
> 37 ? 'y+1/2,x+1/2,z+1/2'
> 38 ? '-y+1/2,-x+1/2,z+1/2'
> 39 ? 'y+1/2,-x+1/2,-z+1/2'
> 40 ? '-y+1/2,x+1/2,-z+1/2'
> 41 ? 'x+1/2,z+1/2,y+1/2'
> 42 ? '-x+1/2,z+1/2,-y+1/2'
> 43 ? '-x+1/2,-z+1/2,y+1/2'
> 44 ? 'x+1/2,-z+1/2,-y+1/2'
> 45 ? 'z+1/2,y+1/2,x+1/2'
> 46 ? 'z+1/2,-y+1/2,-x+1/2'
> 47 ? '-z+1/2,y+1/2,-x+1/2'
> 48 ? '-z+1/2,-y+1/2,x+1/2'
>
> loop_
> _atom_site_label
> _atom_site_type_symbol
> _atom_site_symmetry_multiplicity
> _atom_site_Wyckoff_symbol
> _atom_site_fract_x
> _atom_site_fract_y
> _atom_site_fract_z
> Cu1 ? Cu ? 8c ? ? 0.10890 ?0.10890 ?0.10890
> Cu2 ? Cu ? 8c ? ? 0.82800 ?0.82800 ?0.82800
> Cu3 ? Cu ? 12e ? ?0.35580 ?0.00000 ?0.00000
> Cu4 ? Cu ? 24g ? ?0.31280 ?0.31280 ?0.03660
>
> I can provide additional information from W2K output files if necessary.
>
> Thank you for your help
> Best regards
> Pascal
>
> ? ?* Anglais - d?tect?
> ? ?* Anglais
> ? ?* Fran?ais
>
> ? ?* Anglais
> ? ?* Fran?ais
>
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-- 
Laurence Marks
Department of Materials Science and Engineering
MSE Rm 2036 Cook Hall
2220 N Campus Drive
Northwestern University
Evanston, IL 60208, USA
Tel: (847) 491-3996 Fax: (847) 491-7820
email: L-marks at northwestern dot edu
Web: www.numis.northwestern.edu
Chair, Commission on Electron Crystallography of IUCR
www.numis.northwestern.edu/
Research is to see what everybody else has seen, and to think what
nobody else has thought
Albert Szent-Gyorgi

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