Sophie,

>>
>> My calculation for 64-atoms:

Why do you have to go to 64 atoms to get this kind of quantities? The unit
cell should suffice. Nevertheless:

>> 1) Lattice Constant: I changed the lattice parameter and find the energy
>> and plotting that I find 5.45 Ang, instead of 5.40 as reported in the
>> paper. Why this so different?
>>
>> 2) Bulk modulus: With B = V*Curvature = V*2c3 = 15 MPa, which is far
>> less
>> than 98.6 MPa? Why? Here, c3 is defined as E =C1 + c2*V + c3*V^2, curve
>> fit to the E vs V curve.

This is my opinion based from previous personal experience, and doesn't
mean that the explanation is completely correct. The more experienced
users can correct me if I'm wrong. One of the possible reasons is that you
have a combination of two factors that are leading you to some error
there: using a 64 atom cell and using a quadratic equation as an equation
of state. If you are using a quadratic equation, you have to be very sure
that your total energy really behaves so, because your DFT calculations
will show terms in the total energy that would be of a higher order - by
choosing a quadratic dispersion, you are choosing to ignore these terms.
Anyway, using a quadratic dispersion is never a very good procedure. In my
experience, a cubic would be better because of the reasons stated above.

For the supercell you are using, any small change in the lattice parameter
will lead to rather large energy differences. So you might be missing a
good description in the minimum of the curve, which is one factor that
could be affecting your results - after all, the bulk modulus is
calculated at the point of minimum energy. If you are not describing it
well through your fit, then you will have poor results. A much better
procedure would be to use the unit cell, and a Murnaghan fit to determine
directly B, B' and V_0, the equilibrium volume. Using a small cell, the
energy changes will be smaller with changes in the lattice parameters, in
comparison to the 64-atom supercell. Moreover, the Murnaghan (or
Birch-Murnaghan) equation of state can handle larger changes while giving
you rather accurate results.

As to the cohesive energy, I can't think of anything right now, that could
be a source to the brutal discrepancies you are seeing. Maybe the k-point
sampling is not so good but, being Si and a 64-atom supercell, I would not
really guess that would be the problem.

Best regards,

Marcos

>>
>> 3) Cohesive Energy: I find energy per atom 107.759eV in the bulk. Now to
>> calculate energy per atom I tried to use the suggestions given at
>> http://www.mail-archive.com/[email protected]/msg03118.html
>> I get -7.49eV/atom as pseudopotential calculation, and -576.38eV/atom as
>> ae. So, which one is the energy of the free atom. None is a good one for
>> comparing with the energy I got from bulk to find the cohesive energy.
>>
>> I really tried to search the archive and find solutions to these. I
>> could
>> not find any explicit answers. I am not sure what I am missing. *Some
>> expert's simple directions can solve the problem right away*. I really
>> need this help.
>>
>>
>> Thanks in advance,
>> Sophia
>> Univ. of California - Berkeley
>>
>> Attached fdf file
>>
>> ------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------
>>
>> #
>> -----------------------------------------------------------------------------
>> # FDF for a cubic c-Si supercell with 64 atoms
>> #
>> # E. Artacho, April 1999
>> #
>> -----------------------------------------------------------------------------
>>
>> SystemName          64-atom Si
>> SystemLabel         Si
>>
>> NumberOfAtoms       64
>> NumberOfSpecies     1
>>
>> %block ChemicalSpeciesLabel
>>  1  14  Si
>> %endblock ChemicalSpeciesLabel
>>
>> PAO.BasisSize       DZP
>> PAO.EnergyShift     20 meV
>>
>> %Block PAO.Basis
>> Si   3     -0.46385
>>  n=3   0   2   E    15.42551     4.96988
>>      7.00000     4.37722
>>      1.00000     1.00000
>>  n=3   1   2   E     4.69636     3.83128
>>      7.00000     4.09123
>>      1.00000     1.00000
>>  n=3   2   1   E    11.96912     0.03131
>>      4.55426
>>      1.00000
>> %EndBlock PAO.Basis
>>
>>
>> LatticeConstant     5.430 Ang
>> %block LatticeVectors
>>   2.000  0.000  0.000
>>   0.000  2.000  0.000
>>   0.000  0.000  2.000
>> %endblock LatticeVectors
>>
>> %block kgrid_Monkhorst_Pack
>>         2  0  0     0.0
>>         0  2  0     0.0
>>         0  0  2     0.0
>> %endblock kgrid_Monkhorst_Pack
>>
>>
>> MeshCutoff          40.0 Ry
>>
>> MaxSCFIterations     100
>> DM.MixingWeight      0.3
>> DM.NumberPulay       3
>> DM.Tolerance         1.d-3
>> DM.UseSaveDM
>> XC.functional       LDA
>> XC.authors          CA
>>
>>
>> SolutionMethod       diagon
>> ElectronicTemperature  25 meV
>>
>> WriteForces       true
>> WriteCoorStep     true
>>
>> MD.TypeOfRun         cg
>> MD.NumCGsteps         0
>> MD.MaxCGDispl         0.1  Ang
>> MD.MaxForceTol        0.01 eV/Ang  # earler 0.04
>> SaveRho           true
>>
>> AtomicCoordinatesFormat  ScaledCartesian
>> %block AtomicCoordinatesAndAtomicSpecies
>>    0.00000   0.00000   0.00000         1
>>    0.00000   0.50000   0.50000         1
>>    0.25000   0.25000   0.75000         1
>>    0.25000   0.75000   0.25000         1
>>    0.50000   0.00000   0.50000         1
>>    0.50000   0.50000   0.00000         1
>>    0.75000   0.25000   0.25000         1
>>    0.75000   0.75000   0.75000         1
>>    0.00000   0.00000   1.00000         1
>>    0.00000   0.50000   1.50000         1
>>    0.25000   0.25000   1.75000         1
>>    0.25000   0.75000   1.25000         1
>>    0.50000   0.00000   1.50000         1
>>    0.50000   0.50000   1.00000         1
>>    0.75000   0.25000   1.25000         1
>>    0.75000   0.75000   1.75000         1
>>    0.00000   1.00000   0.00000         1
>>    0.00000   1.50000   0.50000         1
>>    0.25000   1.25000   0.75000         1
>>    0.25000   1.75000   0.25000         1
>>    0.50000   1.00000   0.50000         1
>>    0.50000   1.50000   0.00000         1
>>    0.75000   1.25000   0.25000         1
>>    0.75000   1.75000   0.75000         1
>>    0.00000   1.00000   1.00000         1
>>    0.00000   1.50000   1.50000         1
>>    0.25000   1.25000   1.75000         1
>>    0.25000   1.75000   1.25000         1
>>    0.50000   1.00000   1.50000         1
>>    0.50000   1.50000   1.00000         1
>>    0.75000   1.25000   1.25000         1
>>    0.75000   1.75000   1.75000         1
>>    1.00000   0.00000   0.00000         1
>>    1.00000   0.50000   0.50000         1
>>    1.25000   0.25000   0.75000         1
>>    1.25000   0.75000   0.25000         1
>>    1.50000   0.00000   0.50000         1
>>    1.50000   0.50000   0.00000         1
>>    1.75000   0.25000   0.25000         1
>>    1.75000   0.75000   0.75000         1
>>    1.00000   0.00000   1.00000         1
>>    1.00000   0.50000   1.50000         1
>>    1.25000   0.25000   1.75000         1
>>    1.25000   0.75000   1.25000         1
>>    1.50000   0.00000   1.50000         1
>>    1.50000   0.50000   1.00000         1
>>    1.75000   0.25000   1.25000         1
>>    1.75000   0.75000   1.75000         1
>>    1.00000   1.00000   0.00000         1
>>    1.00000   1.50000   0.50000         1
>>    1.25000   1.25000   0.75000         1
>>    1.25000   1.75000   0.25000         1
>>    1.50000   1.00000   0.50000         1
>>    1.50000   1.50000   0.00000         1
>>    1.75000   1.25000   0.25000         1
>>    1.75000   1.75000   0.75000         1
>>    1.00000   1.00000   1.00000         1
>>    1.00000   1.50000   1.50000         1
>>    1.25000   1.25000   1.75000         1
>>    1.25000   1.75000   1.25000         1
>>    1.50000   1.00000   1.50000         1
>>    1.50000   1.50000   1.00000         1
>>    1.75000   1.25000   1.25000         1
>>    1.75000   1.75000   1.75000         1
>> %endblock AtomicCoordinatesAndAtomicSpecies
>>
>


-- 
Dr. Marcos Verissimo Alves
Post-Doctoral Fellow
Unité de Physico-Chimie et de Physique des Matériaux (PCPM)
Université Catholique de Louvain
1 Place Croix du Sud, B-1348
Louvain-la-Neuve
Belgique

------

Gort, Klaatu barada nikto. Klaatu barada nikto. Klaatu barada nikto.

Reply via email to