sorry, it is​
'change the kpoint until the energy/atom (eV) change is less than 0.01eV ?​'

-- 
Best Regards

邱芳瑜  Chiu Fang Yu
國立成功大學 材料科學與工程學系碩二
MOBILE:0930287221(中華)
GMAIL:[email protected] <[email protected]>



2014-12-17 14:55 GMT+08:00 joyce79928cc . <[email protected]>:
>
> I was wondering how to decide whether it is converge?
> change the kpoint until the energy(eV) change is less than 0.01eV or...?
> Thanks!
>
> --
> Best Regards
>
> 邱芳瑜  Chiu Fang Yu
> 國立成功大學 材料科學與工程學系碩二
> MOBILE:0930287221(中華)
> GMAIL:[email protected] <[email protected]>
>
>
>
> 2014-12-17 14:51 GMT+08:00 joyce79928cc . <[email protected]>:
>>
>> Thanks for reply. I will try to fix it!
>>
>> --
>> Best Regards
>>
>> 邱芳瑜  Chiu Fang Yu
>> 國立成功大學 材料科學與工程學系碩二
>> MOBILE:0930287221(中華)
>> GMAIL:[email protected] <[email protected]>
>>
>>
>>
>> 2014-12-17 14:38 GMT+08:00 <[email protected]>:
>>>
>>> Dear joyce79928:
>>>
>>> just some ideas.
>>> Your results may be noise due to insufficient basis and/or
>>> insufficient k-mesh ans/or insufficient MeshCutoff
>>> (probably all three).
>>> Does your DOS have any resemblance with what is expected for a 1-dim.
>>> chain?
>>> Does your stress definition in the GeometryConstrains block
>>> serve any purpose?
>>> There is a number of works with Siesta on Au chains around,
>>> maybe scroll through them first.
>>> Anyway, you can systematically proceed in the following way:
>>>
>>> Take just one atom along the chain step, not three
>>> (make the third lattice vector shorter :-).
>>> Fix it.
>>> For the k-mesh, you need just 1 point in the plane but more than 4
>>> along Z.
>>> Run a sequence of calculations just varying the 3d lattice vector
>>> (chain step) - single point, no relaxation.
>>> Trace the total energy curve as function of chain step.
>>> This will give you an approximation to "true Siesta" result.
>>> Study how it depends on basis, k-mesh and MeshCutoff.
>>> Find "good" values for all three.
>>> Make the usual "egg box" test.
>>> Then hopefully your forces will be OK so that
>>> you can add more atoms to your unit, release them, let them relax etc.
>>>
>>> Good luck
>>>
>>> Andrei
>>>
>>> [email protected]
>>>
>>>
>>> > Dear:
>>> >
>>> > I want to relax the chain with Siesta.
>>> > but different atom position with same parameter will get different
>>> > structure.
>>> > for example, I set the distance between chain to 2.93 A and get a final
>>> > structure of 2.569 A between chain.
>>> > Then I change initial chain distance to 2.88 A and get a final
>>> structure
>>> > of
>>> > 2.758 A between chain.
>>> >
>>> > why this happened?
>>> >
>>> > Thanks for reading my mail and it is welcome to discuss with me.
>>> >
>>> > below's are my fdf input file.
>>> >
>>> > SystemName  bulk_au
>>> > SystemLabel bulk_au
>>> >
>>> > ==================================================
>>> > ==================================================
>>> > # SPECIES AND BASIS
>>> >
>>> > # Number of species
>>> > NumberOfSpecies 1
>>> > %block ChemicalSpeciesLabel
>>> >   1  79 Au
>>> > %endblock ChemicalSpeciesLabel
>>> >
>>> > PAO.BasisSize    SZP
>>> > PAO.EnergyShift  0.04 Ry
>>> >
>>> >
>>> > # K-points
>>> >
>>> > %block kgrid_Monkhorst_Pack
>>> > 4   0   0   0.0
>>> > 0   4   0   0.0
>>> > 0   0   4   0.5
>>> > %endblock kgrid_Monkhorst_Pack
>>> >
>>> >
>>> > # UNIT CELL AND ATOMIC POSITIONS
>>> >
>>> > # UNIT CELL
>>> > LatticeConstant       1.0 Ang
>>> > %block LatticeVectors
>>> > 8.81553253 0.00000000 0.00000000
>>> > 4.40776625 7.63447409 0.00000000
>>> > 0.00000000 0.00000000 8.79434817
>>> > %endblock LatticeVectors
>>> >
>>> > # Atomic coordinates
>>> > NumberOfAtoms 3
>>> > AtomicCoordinatesFormat ScaledCartesian
>>> > %block AtomicCoordinatesAndAtomicSpecies
>>> > 4.407766232 4.241374236 0.00000000 1
>>> > 4.407766232 4.241374236 2.93144939 1
>>> > 4.407766232 4.241374236 5.86289878 1
>>> > %endblock AtomicCoordinatesAndAtomicSpecies
>>> >
>>> > ==================================================
>>> > ==================================================
>>> > # General variables
>>> >
>>> > ElectronicTemperature  300 K
>>> > MeshCutoff           200. Ry
>>> > xc.functional         LDA           # Exchange-correlation functional
>>> > xc.authors            CA
>>> > SpinPolarized .false.
>>> > SolutionMethod Diagon
>>> >
>>> >
>>> > # SCF variables
>>> >
>>> > DM.MixSCF1   T
>>> > MaxSCFIterations      300           # Maximum number of SCF iter
>>> > DM.MixingWeight       0.03          # New DM amount for next SCF cycle
>>> > DM.Tolerance          1.d-4         # Tolerance in maximum difference
>>> > DM.UseSaveDM          true          # to use continuation files
>>> > DM.NumberPulay         5
>>> > #Diag.ParallelOverK    yes
>>> >
>>> > # MD variables
>>> >
>>> > MD.FinalTimeStep 1
>>> > MD.TypeOfRun CG
>>> > MD.NumCGsteps     50
>>> > MD.VariableCell      T
>>> > UseSaveData  T
>>> >
>>> > # Output variables
>>> >
>>> > WriteMullikenPop                1
>>> > WriteBands                      .false.
>>> > SaveRho                         .false.
>>> > SaveDeltaRho                    .false.
>>> > SaveHS                          .false.
>>> > SaveElectrostaticPotential      True
>>> > SaveTotalPotential              no
>>> > WriteCoorXmol                   .true.
>>> > WriteMDXmol                     .true.
>>> > WriteMDhistory                  .false.
>>> > WriteEigenvalues                yes
>>> >
>>> > %block GeometryConstraints
>>> > stress 4 5 6
>>> > position 1
>>> > %endblock GeometryConstraints
>>> >
>>> >
>>> >
>>> > --
>>> > Best Regards
>>> >
>>> > 邱芳瑜  Chiu Fang Yu
>>> > 國立成功大學 材料科學與工程學系碩二
>>> > MOBILE:0930287221(中華)
>>> > GMAIL:[email protected] <[email protected]>
>>> >
>>>
>>>
>>>
>>>
>>>

Responder a