It seems to me that in the output we print the the square of the
projections, symmetrized, while the xml file contains the projections, not
squared and not symmetrized
Paolo
On Wed, Apr 6, 2022 at 4:38 PM Léo Gaspard wrote:
> Sorry I forgot to add the files, they are attached in this mail
Dear QE-Users,
I am planning to do some CPMD simulation about iron oxides (Fe2O3, Fe3O4 and
FeO) and their reactions with hydrogen at high temperature using cp.x of QE
7.0. My goal is only to try to simulate the reduction process in atomistic
scale, and the CPMD trajectory results should
Dear Kejiang
Only EXX functionals such as PBE0 or HSE significantly increase the
computation time. DFT+U has been primarily developed as a
cost-effective method to correct delocalization errors in the case of
localized shells such as those present in transition metal oxides.
There are
Dear Giuseppe,
Thanks for your kind explanation.
As per your suggestion, it might be better to do 'vc-relax'/'relax' only
with pw.x, while do CPMD only with cp.x. But we should try to keep the
parameters (such as, nspin, tot_magnetization, lda_plus_u, Hubbard_U(i),
degauss, smearing, ...) being
Thanks a lot for sharing this good paper, Nicola.
I will read this paper and use dft+hubbard in the future calculation for iron
and its oxide.
All the best,
Kejiang
-邮件原件-
发件人: users-boun...@lists.quantum-espresso.org
代表 Nicola Marzari via users
发送时间: 2022年4月7日 18:58
收件人:
Dear Giuseppe,
Thanks a lot for your prompt response and sharing your experience.
Yes, I found that there are parameters (nspin, tot_magnetization,
lda_plus_u, Hubbard_U(i)) that can be used to set spin, magnetism and U in
cp.x. But after I set these parameters (nspin = 2 , tot_magnetization=0,
Dear Kejiang
As a very general rule, partially depending on the history of the
codes included in the QE distribution, pw.x is the "engine" for
electronic structure calculations (including geometry and cell
optimizations, but also Born-Oppenheimer MD simulations), and cp.x the
"engine"
Thanks Giuseppe,
couldn't agree more! Never being one to miss an opportunity to promote
dft+hubbard, I would also add that these functional can be also more
accurate, because they screen a fock-like term with awareness of the
local bonding - see Iurii's just-out work on batteries:
Hello,
I would like to perform geometry optimizations constraining the spin density on
certain atoms in a system.
>From what I have read in some published works, there is an available
>implementation of constrained DFT in Quantum Espresso. However, I am not able
>to find in the
Hello Franklin,
IMO, the cutoff of 41 Ry is too short for a proper and stable structure
convergence. How does the stress tensor compare at the last step of vc-relax,
and at the verification step (latest stress tensor written in the output file)?
I'm more familiar with organic systems. But I
On Thu, Apr 7, 2022 at 3:21 PM Bidault, Xavier wrote:
Just my 2 cents.
>
I appreciate your 2-cent contribution, but none of your observations is
relevant to this case.
About the original post: while I think that options "noinv" and "nosym" are
a disgrace, I agree that one should obtain the
Dear QE-Users,
I am planning to do some CPMD simulation about iron oxides (Fe2O3, Fe3O4 and
FeO) and their reactions with hydrogen at high temperature using cp.x of QE
7.0.
As it is well known that spin and magnetism are the most fundamental
characteristics for iron and its oxides, we should
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