You might try to use the latest development version of plotband.x available
through the SVN server:
http://qe-forge.org/gf/project/q-e/scmsvn/?action=AccessInfo
Now it can combine the data from bands.x and projwfc.x to assign a
projection-dependent weight to each epsilon_k,v in the band
Well, this is not enough to prove that this was the real problem.
If you look into your pseudopotential file (with a simple text editor), you
should search for something like ?number_of_wfc? in the header. If the number
is 0, surely you cannot use that PP in LDA+U calculations (but it should be
Dear Jiajie,
on top of all these problems mentioned by Matteo and Andrei, there can be
issues when the pseudopotential is not in a ?standard? format. For instance, if
it was converted from another format, the atomic wave functions might be
missing from the file (as, for instance, in the
In general, you cannot, because in presence of spin-orbit coupling the
spherical harmonics are not eigenstates of the atomic Hamiltonian. Therefore
the code projects onto spin-angle functions (see PRB 71, 115106), which are
eigenstates of total angular momentum J=L+S, and of its projections
Hello,
I do not know who (if anyone) is currently developing such feature, but for
sure it is not yet in the SVN repository. The header of pw2wannier90.f90
presently reads:
! pw2wannier was written by Stefano de Gironcoli
! with later additions by
! Jonathan Yates - spinors
! Arash
Dear Dmitry,
I am sure there is nothing puzzling in there. When lda_plus_u is true, but
all Hubbard_U?s are zero, the Hubbard component of the forces are still
computed and added to the total force, but such component will be zero (try
verbosity=?high? to get them printed on output). In
vext.f90 ?
> Dear users,
>
> I'm learning to generate UPFs using ld1.x code. We knew that the exchange
> and correlation potential can be GGA or LDA, etc. My problem is: how could
> I modify the potential expression? For example, I want to use a new
> potential
> based on GGA:
Dear Vladislav,
I mostly agree with what Nicki said here below. I also believe that in your
case the problem is the ewind value, which is too small and can lead to some
weirdnesses in the 2D-basis set reduction. You should try at least 4.0 and
check convergence as suggested by Nicki.
In my
You can "add" vacuum by increasing the cell size along z. In the ibrav=4 case
this can be accomplished by increasing the celldm(3) parameter by a suitable
amount. See also here:
http://www.quantum-espresso.org/wp-content/uploads/Doc/INPUT_PW.html#idp82000
HTH
GS
Sir, I am unable to
Dear Siddheshwar Chopra,
Do you want to study a graphene flake or an infinite graphene layer. In the
first case you need to saturate edges with H, and add enough vacuum both within
the plane of the flake and out of the plane (remember that the code uses
periodic boundary conditions in all
Dear Manoj,
The code should give on output exactly what you are searching for. The
total magnetization is the integral of (charge_density_up -
charge_density_down) in the unit cell. The absolute magnetization is obtained
by integrating the absolute value of that difference.
GS
Dear QE
Dear Vladislav,
I think there was an erroneous extra factor 2 in some PWcond versions
between 5.0 and 5.0.2. I would stick to the latest stable version 5.1, recently
released.
Best regards,
GS
> I calculate the spin-polarized transmission for a tunnel junction
> using the PWCOND code.
band lineups
at heterointerfaces.
I agree with Nicola that the problem is subtle, given that a pure bulk
calculation for an infinite solid cannot provide absolute energy levels.
Hopefully someone with clearer ideas than me will be able to suggest
alternative solutions.
Best,
GS
Dear Sclau
Dear Rajdeep Banerjee,
the following paper
http://journals.aps.org/prl/pdf/10.1103/PhysRevLett.101.046405
and related work in the Pasquarello group (EPFL) could also be of help to solve
your problem.
Best,
GS
Dear all,
I want to look at the movement of valence band maxima
Dear Rajdeep Banerjee,
the amount of information you posted is not sufficient to understand what
kind of problem there is.
The error message you report comes from the parallel environment and does not
tell anything about the nature of the crash.
It could be due to a segmentation fault
Dear Rajdeep Banerjee,
I would suggest to use the latest stable version (5.0.3) of the code
instead.
Still, stress and tefield cannot be used together, even if you have
norm-conserving pseudopotentials . However, forces are available, so you can
still do a set of relax calculations for
I
guess that, as for wannier90, you need to provide Bloch states and eigenvalues
on a regular grid covering the full Brillouin Zone, not only the irreducible
wedge.
Practically speaking, try to perform a nscf calculation using nosym=.TRUE.
before using wannier_ham.
You might need to specify
Dear Dr. Sclauzero
Thanks a lot for your help and suggestion. I studied mentioned examples and
changed my input files. I separated electrodes in another file with
prefix='au', molecule with prefix='adn' and pwcond.x with prefixl='au',
prefixs='adn'
So fast! Please have a look at
Dear Lijuan,
Please try to explain better your problem. What does it happen when you run
that command within Matlab? Do you get an error message? Nothing happens? ...?
I don't think the problem is mpi, the code should work anyway on one processor.
It works on my Ubuntu desktop with QE 5.0.3
Dear Paresh,
in my understanding you should start with a very small lambda value (e.g.
0.1), make sure the calculation has converged (not always trivial), then
restart with a larger value.
It is important to tune the steps by which you increase lambda. Increasing it
by steps of 5 seems
Thank you very much for your reply, it is really appreciated. I will changed
all parameters of my input file. I have a planer molecule in X-Y plane and I
want to use a planar lead in Y-Z. I realized I have to change the transmission
direction to Z.
Good!
Could I have a lead in X-Y plane
21 matches
Mail list logo