[Wien] about Harmonic expansion
Peter Blaha
pblaha at zeus.theochem.tuwien.ac.at
Fri Jan 14 17:38:47 CET 2005
Hi,
These multipole moments are used to calculate the Coulomb potential.
First, the Multipole moments from the charge density inside the spheres
are calculated.
Second, the multipolemoments from a charge density represented by the
plane wave charge density inside these spheres are also calculated and
finally these two MP-moments are subtracted ("Pseudo-MPM") and later on
used to construct a "pseudo charge", which is represented by a Fourier
series having exactly these multipole moments, but is zero in the
interstital and can thus be added to the PW charge density of the
interstital.
One has then a Fourier expansion, which gives the correct density in the
interstital AND has correct multipole moments inside the spheres, thus you
can simply solve Poissons equation and obtain a Fourier series of the
potential (valid in the interstital).
This is described in the paper by M.Weinert 1981 ?, yo may find the exact
reference in the UG (References).
I want to know the detail of harmonic expansion used in wien2k.
> This is part of case.output0, I dont know its meaning, could you give me an explan?
> ------------------------------
> M U L T I P O L M O M E N T S
> ------------------------------
>
>
> ATOM= 1 Si1 Z=14.00 LM= 6 POSITION= 0.875 0.375 0.375
>
> L= 0 M= 0 SPHERE MM = 0.629969486 0.000000000
> L= 4 M= 0 SPHERE MM = 0.137908491 0.000000000
> L= 4 M= 4 SPHERE MM = 0.082416087 0.000000000
> L= 6 M= 0 SPHERE MM = -0.038451045 0.000000000
> L= 6 M= 4 SPHERE MM = 0.071935319 0.000000000
> L= -3 M= 2 SPHERE MM = 0.000000000 0.281234883
>
>
> ATOM= 1 Si1 Z=14.00 LM= 6 POSITION= 0.875 0.375 0.375
>
> L= 0 M= 0 PLANE WAVE MULTIPOLMOMENT = 0.552128554 0.000000000
> L= 4 M= 0 PLANE WAVE MULTIPOLMOMENT = -0.136937612 0.000000000
> L= 4 M= 4 PLANE WAVE MULTIPOLMOMENT = -0.081835876 0.000000000
> L= 6 M= 0 PLANE WAVE MULTIPOLMOMENT = 0.038123303 0.000000000
> L= 6 M= 4 PLANE WAVE MULTIPOLMOMENT = -0.071322169 0.000000000
> L= -3 M= 2 PLANE WAVE MULTIPOLMOMENT = 0.000000000 -0.279651825
>
> ATOM= 1 Si1 Z=14.00 LM= 6 POSITION= 0.875 0.375 0.375
>
> L= 0 M= 0 PSEUDO MULTIPOLMOMENT = 1.182098040 0.000000000
> L= 4 M= 0 PSEUDO MULTIPOLMOMENT = 0.000970878 0.000000000
> L= 4 M= 4 PSEUDO MULTIPOLMOMENT = 0.000580211 0.000000000
> L= 6 M= 0 PSEUDO MULTIPOLMOMENT = -0.000327742 0.000000000
> L= 6 M= 4 PSEUDO MULTIPOLMOMENT = 0.000613150 0.000000000
> L= -3 M= 2 PSEUDO MULTIPOLMOMENT = 0.000000000 0.001583058
> L= 4 M=-4 PSEUDO MULTIPOLMOMENT = 0.000580211 0.000000000
> L= 6 M=-4 PSEUDO MULTIPOLMOMENT = 0.000613150 0.000000000
> L= -3 M=-2 PSEUDO MULTIPOLMOMENT = 0.000000000 -0.001583058
>
> Best wish to you!
> Yonghua
>
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>
P.Blaha
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Peter BLAHA, Inst.f. Materials Chemistry, TU Vienna, A-1060 Vienna
Phone: +43-1-58801-15671 FAX: +43-1-58801-15698
Email: blaha at theochem.tuwien.ac.at WWW: http://info.tuwien.ac.at/theochem/
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