Dear Daria,
Thanks for your immediate reply!
We will try it.
Kemal
----- Original Message ----- From: "Lydia Nemec" <[EMAIL PROTECTED]>
To: <[email protected]>
Sent: Thursday, May 15, 2008 12:10 PM
Subject: Re: [SIESTA-L] MnO No bandgap with AFII magnetisation


Hello!

Thanks for your immediate reply!

Here is my Input File:

# MnO with corrections according to the PRL 96, 047209 (2006) by Goodwin,
#Tucker, Dove and Keen and relaxed
# FDF file for bulk MnO
# AFII magnatisation
# Geometrical Relaxation

# General system specifications

SystemName          MnO bulk #Descriptive name of the system
SystemLabel         MnO #Short Name for Naming files
NumberOfAtoms       24 #Numbers of atoms in the calculation
NumberOfSpecies     2 # Numbers of Species

%block ChemicalSpeciesLabel
1  25 Mn         # Species index, atomic number, species label
2   8 O          # Species index, atomic number, species label
%endblock ChemicalSpeciesLabel

# Basis set definition
PAO.Basis < basis.fdf

# Lattice, Coordinates, k-sampling
#expended Structure along the [111] layer

LatticeConstant 1.0 Ang
%block LatticeParameters
5.44582   3.1464713   15.1675818   90.0000   89.9617   90.0000
%endblock LatticeParameters

#Atomic coordinates

AtomicCoordinatesFormat ScaledByLatticeVectors

%block AtomicCoordinatesAndAtomicSpecies
0.1645946   0.51011   0.0860413 1 1 #Mn down
0.6645946   0.01011   0.0860413 1 2 #Mn down
0.8312613   0.51011   0.9193746 1 3 #Mn up
0.3312613   0.01011   0.9193746 1 4 #Mn up
-0.004144    0.02022   0.252708  1 5 #Mn up
0.495856    0.52022   0.252708 1 6 #Mn up
-0.004144    0.02022   0.752708 1 7 #Mn down
0.495856    0.52022   0.752708 1 8 #Mn down
0.3312613   0.01011   0.4193746 1 9 #Mn down
0.8312613   0.51011   0.4193746 1 10 #Mn down
0.6645946   0.01011   0.5860413 1 11 #Mn up
0.1645946   0.51011   0.5860413 1 12 #Mn up
0.0000000   0.00000   0.0000000 2 13
0.5000000   0.50000   0.000000  2 14
0.3333333   0.00000   0.167477  2 15
0.8333333   0.50000   0.167477  2 16
0.6666666   0.00000   0.833333  2 17
0.1666666   0.50000   0.833333  2 18
0.1666666   0.50000   0.334144  2 19
0.6666666   0.00000   0.334144  2 20
0.8333333   0.50000   0.666666  2 21
0.3333333   0.00000   0.666666  2 22
0.0000000   0.00000   0.500000  2 23
0.5000000   0.50000   0.500000  2 24
%endblock AtomicCoordinatesAndAtomicSpecies


# Spin Polarisation Antiferromagnetic AFII

SpinPolarized .true.

%block DM.InitSpin
 1   -
 2   -
 3   +
 4   +
 5   +
 6   +
 7   -
 8   -
 9   -
10   -
11   +
12   +
%endblock DM.InitSpin

# K-sampling (alternative specification using kgrid_cutoff)

%block kgrid_Monkhorst_Pack
        3  0  0  0.5
        0  6  0  0.5
4  0  2  0.5
%endblock kgrid_Monkhorst_Pack

#Projected Debsity of States

%block ProjectedDensityOfStates
-85.00   85.00   0.1   1500  eV
%endblock ProjectedDensityOfStates

# Band lines of an monoclinic MnO bulk

BandLinesScale ReciprocalLatticeVectors

%block BandLines
1  1.000  1.000  1.000  A      #Beginn at A
40  0.000  0.000  1.000  Z      #go to Z
40  0.000  0.000  0.000  \Gamma #along Lambda
40  0.000  1.000  0.000  Y      #alomg Delta
40  0.000  1.000  1.000  D      #along U
%endblock BandLines

#Geometrical Optimization

MD.TypeOfRun    CG
MD.VariableCell .true.
MD.MaxForceTol  0.01 eV/Ang
MD.MaxStressTol 0.1  GPa
MD.NumCGsteps   25

#Density functional (Notice that Xc.authors and XC.functional
#are both needed and must be consistent)

XC.Functional GGA #exchange correlation functional type
XC.Authors PBE #(Perdew-Burke-Ernzerhof). Generalized gradients approximation.
#Ref: Perdew, Burke and Ernzerhof, PRL 77, 3865 (1996)

#Real space grid
MeshCutoff 400 Ry #equivalent planewave cutoff for the grid

# Convergence of SCF

DM.MixingWeight 0.04
DM.NumberPulay  4
DM.Tolerance 1.d-4
MaxSCFIterations 100

# Type of solution (diagon is the  default for less than 100 atoms)

SolutionMethod diagon
ElectronicTemperature 5 K

#Use files from previous run
#DM.UseSaveDM   .true.
#MD.UseSaveCG   .true.
#MD.UseSaveXV   .true.

# Output options

AtomCoorFormatOut Ang

#WriteCoorInitial .true.
#WriteCoorStep    .true.
WriteCoorXmol    .true.
WriteMDhistory   .true.
WriteMDXmol      .true.
Am Donnerstag 15 Mai 2008 01:27:37 schrieb Marcos Verissimo Alves:
Lydia,

This is too little information... Send us your input file, so we can take
a better look and find possible errors.

Marcos.



Vous avez écrit / You have written / Lei ha scritto / Você escreveu...
Lydia Nemec

> Dear All!
>
> I'm just started with my Diplomathesis and connected with my Thesis I

started

> to run SIESTA. I tried to run some Calculations on MnO, but it doesn't

worked

> well.
> For example I haven't found a bandgap yet. There are just very few

states

> in
> the DOS and few bands crossing the Fermi level.
> But for AFII magnetisation I should find a bandgap.
> I run the calculation with to different structurs one in the classical

rocksalt structure and one in a Monoclinic structure according to the
paper

> by
>
> Goodwin, Andrew L.; Tucker, Matthew G.; Dove, Martin T.; Keen and David

A.

> Magnetic Structure of MnO at 10 K from Total Neutron Scattering Data

http://link.aps.org/abstract/PRL/v96/e047209

> I have choosen LDA and GGA Pseudos and the Basis Set available on > Siesta

Hompage (already tested with LaMnO3 and LSMO) for three different
Magnetisations (ferromagnetic, Antiferromagnetic [100] known as AFI, and
Antiferromagnetic [111] known as AFII)

> The Total Energy and the DOS are for both structures almost the same.

I've

> get
> reasonable small changes in the Totalenergy for different

magnetisations.

> But I don't find the bandgap for AFII Magnetisation. I found papers in

which

> they performed dft calculations on MnO and found the bandgap.
>
> I let the structure relax with :
> #Geometrical optimization
>
> MD.TypeOfRun    CG
> MD.VariableCell .true.
> MD.MaxStressTol  0.1 GPa
> MD.MaxForceTol   0.01 eV/Ang
> MD.NumCGsteps    25
>
> But there are still bands crossing the Fermilevel.
>
> Has anybody experiences with MnO and SIESTA?
>
> Thanks a lot for your help.
>
> Best Regards,
> Lydia Nemec
>
> --
> Lydia Nemec
> =======================================================
> Department of Earth Sciences, University of Cambridge
> Downing Street, Cambridge CB2 3EQ, UK
> Tel. 0044(01223)3-33411
> Email: [EMAIL PROTECTED]
> -------------------------------------------------------
> Institute for Theoretical Physics
> University Regensburg
> 93040 Regensburg, Germany
> =======================================================



--
Lydia Nemec
=======================================================
Department of Earth Sciences, University of Cambridge
Downing Street, Cambridge CB2 3EQ, UK
Tel. 0044(01223)3-33411
Email: [EMAIL PROTECTED]
-------------------------------------------------------
Institute for Theoretical Physics
University Regensburg
93040 Regensburg, Germany
=======================================================

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