to the valence-band
maximum
(of a undoped case).
Am 13.04.2015 um 18:04 schrieb David Olmsted:
Dear Peter and all list members,
[Peter, thanks again for the response below.]
I am modeling XPS binding energy using a one-half core-hole, offset
by background charge.
I am looking at the Al
in the right units.
On Mon, Apr 13, 2015 at 1:37 PM, David Olmsted olms...@berkeley.edu wrote:
Laurence,
Thank you for the suggestion. It makes sense, but it may not work here.
For the 48 atom supercell of AlPO4, excluding the two P atoms that are
second neighbors of the Al with the half core
to correct for
it?
Apparently I cannot compare the Fermi energy of different runs, each
with one-half of a core-hole but different numbers of atoms, because
of the issue of the zero of energy that Peter Blaha points out below.
Thanks,
David
David Olmsted
Assistant Research Engineer
be a reasonable number. Your k-mesh sounds ok.
PPS: without core hole: the small and large cell should give identical
results when the k-mesh is equivalent (and all other computational
parameters, in particular RMT values, too).
Am 11.04.2015 um 00:45 schrieb David Olmsted:
Ouch! That is too bad
energy of different runs, each with
one-half of a core-hole but different numbers of atoms, because of the issue
of the zero of energy that Peter Blaha points out below.
Thanks,
David
David Olmsted
Assistant Research Engineer
Materials Science and Engineering
210 Hearst Memorial Mining Building
used comparable k-meshes. This means the mesh for the
2x2x1 supercell should be by by a factor of two smaller in x,y than for the
primitive cell
(eg. 2x2x2 vs 4x4x2)
Am 10.04.2015 um 19:33 schrieb David Olmsted:
I am modeling XPS binding energy using a half core-hole, offset by
background
situation.
Am 06.04.2015 um 21:37 schrieb David Olmsted:
Laurence,
Thank you for the response. As I mentioned in my first try at this issue
last week, I have put the sleep $delay back in, and it does seem to have
helped. I think I have less failures when the lapw1 processes are being
, sorry.
On Mon, Apr 6, 2015 at 11:32 AM, David Olmsted olms...@berkeley.edu wrote:
Hi,
There has been no response to my suggestion that in lapw1para_lapw, the
line “#sleep $delay” be changed to “sleep $delay”. Perhaps I have not
given enough information. In the userguide
with TORQUE. I was using
a revised version of a parallel_options file from a post by Lawrence Marks
which included set delay = 0.25, and was surprised to discover this did
not actually take effect in lapw1para_lapw.
Thanks,
David
David Olmsted
Assistant Research Engineer
Materials Science
be
set by the user in parallel_options.
Best,
David
David Olmsted
Assistant Research Engineer
Materials Science and Engineering
210 Hearst Memorial Mining Building
University of California
Berkeley, CA 94720-1760
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am not saying this is the right one.
Best,
David
David Olmsted
Assistant Research Engineer
Materials Science and Engineering
210 Hearst Memorial Mining Building
University of California
Berkeley, CA 94720-1760
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Wien
in the calculation, or just
something in the reporting? (I was unable to find anything on this in the
mail archive.)
case.stuct, case.inc and case.inm follow.
Thanks,
David
David Olmsted
Assistant Research Engineer
Materials Science and Engineering
210 Hearst Memorial Mining Building
University
.
-Original Message-
From: David Olmsted [mailto:olms...@berkeley.edu]
Sent: Thursday, March 19, 2015 9:04 AM
To: 'wien@zeus.theochem.tuwien.ac.at'
Subject: Determine primitive cell and positions, CXZ LATTICE 15_B2/b
Dear reader,
I am trying to determine the primitive cell and positions
thanks for any help.
David
David Olmsted
Assistant Research Engineer
Materials Science and Engineering
210 Hearst Memorial Mining Building
University of California
Berkeley, CA 94720-1760
--- case.struct
troll_icsd
CXZ LATTICE,NONEQUIV.ATOMS: 14 15_B2/b
MODE OF CALC=RELA unit=bohr
Peter,
Thank you very much for your help.
Together with the large P-s charge in :EPL it tells you, that you should
lower the P-s parameter in case.in1 to -1.34
Whether one sets in addition a second l=0 Eparameter in case.in1 depends
on
the E-separation between these EPL and EPH values,
.
In addition, final state screening effects are better accounted for.
Am 06.03.2015 um 00:44 schrieb David Olmsted:
Ghostbands: pushed energy range in case.in1 to 6.3, does this mean there is
a problem?
WIEN2k_14.2 (Release 15/10/2014)
Quad-Core AMD Opteron(tm) Processor 2378
Linux cluster
group of Mark Asta
David Olmsted
Assistant Research Engineer
Materials Science and Engineering
210 Hearst Memorial Mining Building
University of California
Berkeley, CA 94720-1760
== case.struct ===
metavar_v
P 12 14_P21/n
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