Hello dear Siesta users,

I am calculating Pd bulk (magnetic moment, DoS, ...) and now got some
strange results. I checked the convergence in k-points:

kgrid_Monkhorst_Pack        Total energy (eV)
magnetic moment (uB)
20X20X20                                -968.637543                          
0.174395
21X21X21                                -968.642055                          
0.040505
22X22X22                                -968.638237                         
-0.000013
23X23X23                                -968.639318                          
0.163287
26X26X26                                -968.640164                           
0.118672
27X27X27                                -968.640788                         
-0.000280
28X28X28                         -968.638520                            0.214440
29X29X29                                -968.640467                           
0.001473
33X33X33                                -968.639769                           
0.034345
35X35X35                                -968.640274                           
0.015791
46X46X46                                -968.639395                           
0.004353

The calculated lattice constant of Pd is 3.90Ang (experimental
3.89Ang). And around this value the Pd bulk should be paramagnetic.
Why do the mag. moments here always change? Can I choose a "good" one,
eg. 22X22X22, to continue my work?

------ pd.fdf-------

SystemName       fcc Pd LDA   # Descriptive name of the system
SystemLabel            Pd         # Short name for naming files

# Output options

WriteCoorStep
WriteMullikenPop       1
WriteBands              .true.
WriteKbands             .true.
WriteKpoints            .true.

# Species and atoms

NumberOfSpecies        1
NumberOfAtoms          1
%block ChemicalSpeciesLabel
  1  46  Pd
%endblock ChemicalSpeciesLabel

# Basis

PAO.EnergyShift       50 meV
PAO.BasisSize         DZP

LatticeConstant       3.90 Ang

%block LatticeVectors
  0.000  0.500  0.500
  0.500  0.000  0.500
  0.500  0.500  0.000
%endblock LatticeVectors

%block kgrid_Monkhorst_Pack
       27  0  0   0.0
       0  27  0   0.0
       0  0  27   0.0
%endblock kgrid_Monkhorst_Pack

%block BandLines
1   1.000  1.000  1.000     L     # Begin at L
40  0.000  0.000  0.000  \Gamma   # 40 points from L to Gamma
30  2.000  0.000  0.000     X     # 50 points from Gamma to X
20  1.500  1.500  0.000     K     # 20 points from X to K
30  0.000  0.000  0.000  \Gamma   # 50 points from K to Gamma
%endblock BandLines

%block ProjectedDensityOfStates
-20.00 5.00 0.200 500 eV
%endblock ProjectedDensityOfStates

xc.functional         LDA           # Exchange-correlation functional
xc.authors            CA           # Exchange-correlation version

SpinPolarized         true          # Logical parameters are: yes or no

MeshCutoff           350. Ry        # Mesh cutoff. real space mesh

# SCF options
MaxSCFIterations       150           # Maximum number of SCF iter
DM.Tolerance          1.d-4         # Tolerance in maximum difference
                                              # between input and output DM
DM.UseSaveDM          true          # to use continuation files
DM.NumberPulay         5
DM.MixingWeigh        0.1

SolutionMethod        diagon        # OrderN or Diagon
ElectronicTemperature   300 K       # Temp. for Fermi smearing

# Atomic coordinates
AtomicCoordinatesFormat     ScaledCartesian
%block AtomicCoordinatesAndAtomicSpecies
  0.000000000000    0.000000000000    0.000000000000  1
%endblock AtomicCoordinatesAndAtomicSpecies

---------------------------------------------------


Another question:

in the paper by G. Kresse and J. Furthmiiller (Computational Materials
Science  6 (1996)  15-50 ) they calcuted some "convenient  settings"
for  the  Methfessel&Paxton smearing  parameter  sigma  for  different
metals. For Aluminium it's 1.0 eV, for transition metals like Vanadium
and Rhodium it's 0.3eV, and so on...

For Pd is an ElectronicTemperature of 0.3eV rational?


best rerards,
Lun

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