Dear Juanjo,

As far as I know, metaGGAs are like GGAs for gaps: there are not accurate. For 
getting good gaps you have to  switch to hybrid functionals or GW formalism 
(not implemented in QE though). Depending on what you want to do, of course, 
and if you know the gap value you may try this: optimize with a standard GGA 
functional, run a nscf calculation and if the gap is not totally closed up then 
operate a rigid band shifting for further properties calculations. This is a 
bit brute force...

If you do not know the gap value: run a hybrid single point calculation on the 
GGA optimized structure.

As Yves said, there are not so many options...

Pascal

"Juanjo Meléndez" <[email protected]> wrote:Dear Yves Thanks a lot for your 
comments. Unfortunately, I need a good description ofgaps to calculate optical 
absorption, and hybrid functionals are prohibitive forthe supercells that I 
need to use. That is why I started to try withmetaGGA. I will have a look to 
the paper you mention (which I did not know, by theway, thanks!) for more 
ideas... Take care Juanjo From: Yves Ferro Sent: Friday, October 31, 2014 10:20 
AMTo: PWSCF Forum Subject: Re: [Pw_forum] TB09 metaGGA DearJuanjo,  From what I 
can remember:- the meta-GGA kinetic terms are notsaved in order to restart a 
nscf, at least up to the 5.0 version,- the tools for building meta-GGA PPs are 
not availablein QE.However, I'm not sure using meta-GGA pseudos will solveyour 
problem. Meta-GGA are known to have numerical instabilities such as theones you 
met, in particular when then electronic density drop to a very lowlevel as 
probably in your ionic crystal LiF, on the contrary with Si and C thatform 
covalent structures.
You can have a look to this paper you probablyknow:E.R. Johnson, JCP 131, 
0341112009
I don't believe a cure to you problem exists at themoment, except by changing 
the functional to a GGA one.
Best regards,
Yves. 

Le 31 oct. 2014 à 09:26, Juanjo Meléndez a écrit :
        Hi Pascal     Thanks for replying. I agree with you that building a PP 
consistent with  the metaGGA functional would solve most of the instability 
problems. But I do  not have *any* experience building PPs (which, by the way, 
seems to be not  trivial to me, even less trivial for metaGGA), so I followed 
http://dx.doi.org/10.1016/j.cpc.2013.02.020  and tried the trick. I was just 
wondering if any general strategy for  convergence exists.      Regarding point 
2, I asked one of the authors of the aforementioned paper  and he declared not 
the have seen such a problem before, so I guess that the  kinetic terms are not 
responsible. I have overcome the problem by using a  dense kpoints path already 
in scf calculations and calculating the bands   without the standard 
intermediate nscf run, but it would be nice if the  developers could have a 
look and check.      Again, thank you very much for your interest.     Juanjo   
  Juan J.  Meléndez 
Associate Professor
Department of Physics · University of  Extremadura
Avda. de Elvas, s/n 06006 Badajoz (Spain)
Phone: +34 924 28  96 55
Fax: +34 924 28 96 51
Email: [email protected]
Web: http://materiales.unex.es/miembros/personal/jj-melendez/Index.html         
  From: Pascal BOULET   Sent: Thursday, October 30, 2014 7:15 PM  To: PWSCF 
Forum   Subject: Re: [Pw_forum] TB09 metaGGA         hello,     I have never 
tried meta-GGA functionals with QE, so I am guessing.      For point 1, one 
possible reason is the inadequacy between the pseudo  potential and the 
functional. I guess you have build a special pseudopotential  for this 
functional.     Point 2: Could it be because the meta-GGA kinetic terms are not 
saved in  the checkpoint file and hence not readable when doing the  nscf?

Pascal          "Juanjo Meléndez" <[email protected]> wrote:              Hi all 
        I am starting to work with metaGGA functionals in QE (v.    5.1 + 
libXc), following Èric Germaneau and colleagues’ work 
(http://dx.doi.org/10.1016/j.cpc.2013.02.020).    I know that metaGGA is little 
tested, but I would be pleased if somebody    could answer a couple of 
questions:         1) Convergence is quite tricky. Up to know, I got some    
results in simple systems using a very small mixing_beta (within 0.01–0.05),    
not too many bands (just one or two conduction bands, never converged for    
more bands) and restarting from a previously fully converged calculation. I    
got results only for carbon, silicon and germanium, never got any    
convergence for any binary simple compound (like LiF). Does anyone have    
additional hints for metaGGA calculations to converge?         2) In addition, 
I get something wrong with nscf    calculations. After convergence of a scf 
run, I get a list of bands at each    k-point, as usual –nothing strange here. 
Then I made a path of k-points to    get the band structure and run a nscf 
calculation. This finishes fine as    well, but the bands are not only 
different from those from the scf    calculations, but also unrealistically 
high. I am attaching the input and    output files for both the scf and nscf 
runs, as well as a couple of    eigenval.xml files taken after nscf. Does 
anybody know how to manage this?    Or could this be a bug in the code?         
Thanks a lot in advance         Take care         Juanjo         Juan J.    
Meléndez 
Associate Professor
Department of Physics · University of    Extremadura
Avda. de Elvas, s/n 06006 Badajoz (Spain)
Phone: +34 924    28 96 55
Fax: +34 924 28 96    51
Email: [email protected]
Web: http://materiales.unex.es/miembros/personal/jj-melendez/Index.html         
****************************    “All    those who look stupid actually are, as 
also are half of those who do not    look like” (F. de Quevedo)         
****************************

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Aix-Marseille University 
MADIREL Laboratory
Avenue  Normandie-Niemen 
13397 Marseille Cedex 20 
Email: [email protected] 
Tel.  +33 413 55 18 10 
Fax +33 413 55 18  50

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Pascal Boulet
Aix-Marseille University 
MADIREL Laboratory
Avenue Normandie-Niemen
13397 Marseille Cedex 20
Email: [email protected]
Tel. +33 413 55 18 10
Fax  +33 413 55 18 50
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