If your basis set is not converged, it is clear that the eigenvalues will change (go down in energy) when the basis set is increased.

The cutoff is defined by RKMAX, i.e. we take all plane waves such that |(k+K)| < KMAX. In a bandstructure plot k varies slightly, but it can then happen that at a certain k, the maximal K is too large and gets reduced. Then a "jump" in the bandstructure will appear. In this description, "k" is the vector of the k-point, "K" is a full reciprocal lattice vector.

PS: Yes, RKMAX=7 is of course too small for a 3d (Cu) element, while RKMAX=7 is much too large for H. It is a compromise.

On our website www.wien2k.at at reg.user and faq there are some suggestions for a "minimal" RKMAX for each element. You look into your structure and identify the atom which has the smallest RMT. This atom determines RKMAX according to the list given on this site. However, these values are kind of "minimal" RKMAX values (quite good for eg. optimization of atomic positions (-min), but for highest precision they should be increased by 1-3.

Just a simple example:
You do Cu and need RKMAX=9 for full convergence.
You do CuOH with RMT=1.8; 1.2 and 0.6 for the 3 elements.
RKMAX=3  is counting for H; gives "effective RKMAX=6 for O and 9 for Cu.
Hence RKMAX=3 is fully converged for CuOH (when using RMTs according to the suggestion of setrmt).


Am 23.01.2021 um 04:49 schrieb 巴拉比:
Dear professor Jianxin Zhu,

Thank you so much for your quick reply.

Enlarging RKmax solves the problem! I found I have to set RKmax=9 which is pretty large compared to default 7 to completely eliminate all sawtooth artifacts in bands.

But I still want to know why a smaller RKmax would cause eigenvalues to be discontinuous (in essence hamiltonian is discontinuous) at several k points.

best regards



------------------ Original ------------------
*From:* "A Mailing list for WIEN2k users" <jx...@lanl.gov>;
*Date:* Fri, Jan 22, 2021 11:57 PM
*To:* "A Mailing list for WIEN2k users"<wien@zeus.theochem.tuwien.ac.at>;
*Subject:* Re: [Wien] [EXTERNAL] Bands are often not smooth when zoom in

What rkmax value are you using? Usually a larger rkmax helps make the bands smooth.

Jianxin


Sent with BlackBerry Work
(www.blackberry.com)


*From: *Wien <wien-boun...@zeus.theochem.tuwien.ac.at <mailto:wien-boun...@zeus.theochem.tuwien.ac.at>> on behalf of: 巴拉比 <bal...@qq.com <mailto:bal...@qq.com>>
*Date: *Friday, Jan 22, 2021, 8:15 AM
*To: *wien <wien@zeus.theochem.tuwien.ac.at <mailto:wien@zeus.theochem.tuwien.ac.at>>
*Subject: *[EXTERNAL] [Wien] Bands are often not smooth when zoom in

Dear wien2k developers,

I found bands obtained from wien2k are often not smooth and have many small sawtooth bumps especially when you zoom in. I can reproduce this kind of band artifacts in version 19.2 and 17.1, on differnet computers and link to different version of MKL. I'll take simple copper as an example to show how I obtain the bands:

the structure file I use is as:

blebleble
F   LATTICE,NONEQUIV.ATOMS:  1 225 Fm-3m
              RELA
   6.872726  6.872726  6.872726 90.000000 90.000000 90.000000
ATOM   1: X=0.00000000 Y=0.00000000 Z=0.00000000
           MULT= 1          ISPLIT= 2
Cu1        NPT=  781  R0=0.00005000 RMT=    2.0000   Z: 29.0
LOCAL ROT MATRIX:    1.0000000 0.0000000 0.0000000
                      0.0000000 1.0000000 0.0000000
                      0.0000000 0.0000000 1.0000000
   48      NUMBER OF SYMMETRY OPERATIONS
1 0 0 0.00000000
0 1 0 0.00000000
0 0 1 0.00000000
        1
-1 0 0 0.00000000
0-1 0 0.00000000
0 0 1 0.00000000
        2
-1 0 0 0.00000000
0 1 0 0.00000000
0 0-1 0.00000000
        3
1 0 0 0.00000000
0-1 0 0.00000000
0 0-1 0.00000000
        4
0 0 1 0.00000000
1 0 0 0.00000000
0 1 0 0.00000000
        5
0 0 1 0.00000000
-1 0 0 0.00000000
0-1 0 0.00000000
        6
0 0-1 0.00000000
-1 0 0 0.00000000
0 1 0 0.00000000
        7
0 0-1 0.00000000
1 0 0 0.00000000
0-1 0 0.00000000
        8
0 1 0 0.00000000
0 0 1 0.00000000
1 0 0 0.00000000
        9
0-1 0 0.00000000
0 0 1 0.00000000
-1 0 0 0.00000000
       10
0 1 0 0.00000000
0 0-1 0.00000000
-1 0 0 0.00000000
       11
0-1 0 0.00000000
0 0-1 0.00000000
1 0 0 0.00000000
       12
0 1 0 0.00000000
1 0 0 0.00000000
0 0-1 0.00000000
       13
0-1 0 0.00000000
-1 0 0 0.00000000
0 0-1 0.00000000
       14
0 1 0 0.00000000
-1 0 0 0.00000000
0 0 1 0.00000000
       15
0-1 0 0.00000000
1 0 0 0.00000000
0 0 1 0.00000000
       16
1 0 0 0.00000000
0 0 1 0.00000000
0-1 0 0.00000000
       17
-1 0 0 0.00000000
0 0 1 0.00000000
0 1 0 0.00000000
       18
-1 0 0 0.00000000
0 0-1 0.00000000
0-1 0 0.00000000
       19
1 0 0 0.00000000
0 0-1 0.00000000
0 1 0 0.00000000
       20
0 0 1 0.00000000
0 1 0 0.00000000
-1 0 0 0.00000000
       21
0 0 1 0.00000000
0-1 0 0.00000000
1 0 0 0.00000000
       22
0 0-1 0.00000000
0 1 0 0.00000000
1 0 0 0.00000000
       23
0 0-1 0.00000000
0-1 0 0.00000000
-1 0 0 0.00000000
       24
-1 0 0 0.00000000
0-1 0 0.00000000
0 0-1 0.00000000
       25
1 0 0 0.00000000
0 1 0 0.00000000
0 0-1 0.00000000
       26
1 0 0 0.00000000
0-1 0 0.00000000
0 0 1 0.00000000
       27
-1 0 0 0.00000000
0 1 0 0.00000000
0 0 1 0.00000000
       28
0 0-1 0.00000000
-1 0 0 0.00000000
0-1 0 0.00000000
       29
0 0-1 0.00000000
1 0 0 0.00000000
0 1 0 0.00000000
       30
0 0 1 0.00000000
1 0 0 0.00000000
0-1 0 0.00000000
       31
0 0 1 0.00000000
-1 0 0 0.00000000
0 1 0 0.00000000
       32
0-1 0 0.00000000
0 0-1 0.00000000
-1 0 0 0.00000000
       33
0 1 0 0.00000000
0 0-1 0.00000000
1 0 0 0.00000000
       34
0-1 0 0.00000000
0 0 1 0.00000000
1 0 0 0.00000000
       35
0 1 0 0.00000000
0 0 1 0.00000000
-1 0 0 0.00000000
       36
0-1 0 0.00000000
-1 0 0 0.00000000
0 0 1 0.00000000
       37
0 1 0 0.00000000
1 0 0 0.00000000
0 0 1 0.00000000
       38
0-1 0 0.00000000
1 0 0 0.00000000
0 0-1 0.00000000
       39
0 1 0 0.00000000
-1 0 0 0.00000000
0 0-1 0.00000000
       40
-1 0 0 0.00000000
0 0-1 0.00000000
0 1 0 0.00000000
       41
1 0 0 0.00000000
0 0-1 0.00000000
0-1 0 0.00000000
       42
1 0 0 0.00000000
0 0 1 0.00000000
0 1 0 0.00000000
       43
-1 0 0 0.00000000
0 0 1 0.00000000
0-1 0 0.00000000
       44
0 0-1 0.00000000
0-1 0 0.00000000
1 0 0 0.00000000
       45
0 0-1 0.00000000
0 1 0 0.00000000
-1 0 0 0.00000000
       46
0 0 1 0.00000000
0-1 0 0.00000000
-1 0 0 0.00000000
       47
0 0 1 0.00000000
0 1 0 0.00000000
1 0 0 0.00000000
       48

then I do step by step
1. init_lapw -b
2. run_lapw -in1new 3   # I use -in1new 3 to avoid the QTL-B value warning message in the last few cycles of case.scf file
3. using xcrysden to generate a k path along GAMMA-W-X-L with 400 k points.
    since the klist_band file is too long. I share it on https://pastebin.com/ZaYuFMZE
4. x lapw1 -band
5. x lapw2 -band -qtl

finally, I use the data in case.qtl to plot bands
in [-10eV,10eV] range, it looks pretty normal as shared in below link
https://pasteboard.co/JKPC1tB.png
in [-2eV,-1eV] zoom in range, the look of bands becomes abnormal with full of sawtooth bump as shared in link
https://pasteboard.co/JKPCB7Y.png

So I am wondering if this is a bug? Or what I have done wrong to have this kind of bands(it appears in all my other bands calculation)? I inspected the k path and found it is pretty fine. So I can not think of a reason why the eigenvalue solutions would be discontinous at two nearby k points.

best regards







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Phone: +43-1-58801-165300             FAX: +43-1-58801-165982
Email: bl...@theochem.tuwien.ac.at    WIEN2k: http://www.wien2k.at
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