The only thing that is evident to me at this moment is that you are avoiding 
the K-points in your k-point sampling; as indicated by Marco Verisimo a number 
of years ago your number of k-points must be a multiple of three, which it is, 
but the shift by 0.5, 0.5 is driving the sampling away from the K-points and 
avoiding them... Hopefully bringing the shifts to 0.0 0.0 0.0 solves the 
"differential," or the missing of the K-point on the conduction band.


I would work on the Mo pseudo a little more; and have you checked the effect of 
the basis size as well? Do your pseudos give you a reasonable bulk band 
structure?


Best regards,

-Salvador


________________________________
From: [email protected] <[email protected]> on behalf of Xiaoming 
Wang <[email protected]>
Sent: Thursday, April 30, 2015 7:23 PM
To: [email protected]
Subject: [SIESTA-L] Band structure of MoSe2

Dear Siesta users,

Recently, I’m trying to  calculate the band structure of monolayer MoSe2.  
However, when I plotting the bands, the band curves at K point are not at 
maximum or minimum, which should be. And there seems a non-differential point 
at K along the bands. The band structure of MoSe2 is attached, the 
non-differential point is more obvious at the lowest two bands shown in the 
Fig. Both LDA and PBE functionals give this strange phenomenon. I have tried to 
tune many parameters, but failed to get good result. Can anyone help me with 
the problem?
By the way, I have tried pseudopotentials from Siesta website and from 
http://charter.cnf.cornell.edu/<https://urldefense.proofpoint.com/v2/url?u=http-3A__charter.cnf.cornell.edu_&d=AwMFAg&c=JL-fUnQvtjNLb7dA39cQUcqmjBVITE8MbOdX7Lx6ge8&r=n_Y76F1vumEs9EYNHN2gzA5FD9jzyPhrzl3eOzxCHIQ&m=NaDRSvcZImjiuqSJSGFoSEOGLfumFBd6_fRZa0Hs0Bs&s=UQq2ZNZfUJL5kmP2F3B0GlcPmhnT4dJuFcGi_NHsl2Q&e=>,
 and also used the recently published pps of Comput. Mater. Sci. , 98 (2015) 
372-389. I also changed the energshift, meshcutoff, and k point mesh. But none 
of them can resolve the problem. Below are the input files for relaxation and 
band structure calculations. Any comment or advice are highly appreciated.


fdf for relaxation:

# General System Descriptors

SystemName              mose2
SystemLabel             mose2

NumberOfAtoms           3
NumberOfSpecies         2

%block ChemicalSpeciesLabel
1  42  Mo
2  34  Se
%endblock ChemicalSpeciesLabel

PAO.EnergyShift         50 meV
PAO.BasisSize           DZP

# Structure and K-sampling

LatticeConstant         1.00 Ang
%block LatticeParameters
3.25 3.25 20.00 90. 90. 120.
%endblock LatticeParameters

AtomicCoordinatesFormat Fractional
AtomicCoorFormatOut     Ang
%block AtomicCoordinatesAndAtomicSpecies
       0.333333333   0.666666670   0.505669950  1
       0.666666667   0.333333330   0.625537344  2
       0.666666667   0.333333330   0.385811946  2
%endblock AtomicCoordinatesAndAtomicSpecies

%block kgrid_Monkhorst_Pack
  12  0  0  0.5
   0 12  0  0.5
   0  0  1  0.0
%endblock kgrid_Monkhorst_Pack

# DFT

XC.functional           LDA
XC.authors              CA
SpinPolarized           false
MaxSCFIterations        200
DM.MixingWeight         0.25
DM.NumberPulay          3
DM.Tolerance            1.d-5
MeshCutoff              300 Ry
SolutionMethod          diagon
ElectronicTemperature   300.0 K

# MD and Relaxations

MD.TypeOfRun            CG
MD.VariableCell         T
MD.MaxForceTol          0.01 eV/Ang
MD.MaxStressTol         0.1 GPa
MD.NumCGsteps           200
MD.MaxCGDispl           0.1 Ang
MD.RelaxCellOnly        F

%block GeometryConstraints
   stress 3 4 5 6
%endblock GeometryConstraints

# Output options

WriteCoorInitial        true
WriteCoorStep           true
WriteForces             true
WriteKpoints            false
WriteEigenvalues        false
WriteKbands             false
WriteBands              false
WriteMullikenPop        0
WriteWaveFunction       false
WriteCoorXmol           true
WriteCoorCerius         false
WriteMDCoorXmol         true
WriteMDhistory          true
WriteMDXmol             true
WriteDM                 true

fdf for band structure:
# General System Descriptors

SystemName             mose2
SystemLabel             mose2

NumberOfAtoms           3
NumberOfSpecies         2
%block ChemicalSpeciesLabel
1  42  Mo
2  34  Se
%endblock ChemicalSpeciesLabel

PAO.BasisSize           DZP
PAO.EnergyShift         50 meV

# Structure and K-sampling

LatticeConstant         1.00 Ang
%block LatticeParameters
3.16 3.16 13.00 90. 90. 120.
%endblock LatticeParameters

AtomicCoordinatesFormat Fractional
AtomicCoorFormatOut     Ang
%block AtomicCoordinatesAndAtomicSpecies
       0.333333333   0.666666670   0.505669950  1
       0.666666667   0.333333330   0.625537344  2
       0.666666667   0.333333330   0.385811946  2
%endblock AtomicCoordinatesAndAtomicSpecies

%block kgrid_Monkhorst_Pack
  24  0  0  0.5
   0 24  0  0.5
   0  0  1  0.0
%endblock kgrid_Monkhorst_Pack

# DFT

XC.functional           LDA
XC.authors              CA
SpinPolarized           false
MaxSCFIterations        200
DM.MixingWeight         0.25
DM.NumberPulay          3
DM.Tolerance            1.d-5
MeshCutoff              300 Ry
SolutionMethod          diagon
ElectronicTemperature   300.0 K

# Output options

WriteCoorInitial        true
WriteCoorStep           true
WriteForces             true
WriteKpoints            false
WriteEigenvalues        false
WriteKbands             false
WriteBands              false
WriteMullikenPop        0
WriteWaveFunction       false
WriteCoorXmol           true
WriteCoorCerius         false
WriteMDCoorXmol         true
WriteMDhistory          true
WriteMDXmol             true
WriteDM                 true
UseStructFile           T

BandLinesScale ReciprocalLatticeVectors

%block BandLines
1   0.0000  0.0000 0.0000  \Gamma
70  0.0000  0.5000 0.0000  M
40  0.3333  0.3333 0.0000  K
80  0.0000  0.0000 0.0000  \Gamma
%endblock BandLines




Best regards,

Xiaoming Wang
IAMDN, Rutgers

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