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computing betas and qs for NCPP/USPP/PAW PseudoPotentials

computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

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Page 1: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

computing

betas and qs

for

NCPP/USPP/PAWPseudoPotentials

Page 2: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

Periodic potential

Page 3: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

Periodic potential

Page 4: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

Periodic potential

Page 5: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

Periodic potential

Page 6: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

Periodic potential

atomic form factor crystal structure factor

Page 7: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

ab initio Norm Conserving PseudoPotentials

semilocal form

where projects over L = l(l+1)2

Page 8: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

ab initio Norm Conserving PseudoPotentials

semilocal form

is local with a Coulomb tail

is local in the radial coordinate, short ranged and l-dependent

where projects over L = l(l+1)2

Page 9: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

An example: Mo

l-dependent potential

Hamann, schlueter & Chiang, PRL 43, 1494 (1979)

Page 10: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

An example: Mo

Hamann, schlueter & Chiang, PRL 43, 1494 (1979)

Page 11: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

ab initio Norm Conserving PseudoPotentials

- Kleinman-Bylander fully non-local form

- semilocal form

Page 12: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

ab initio Norm Conserving PseudoPotentials

- Kleinman-Bylander fully non-local form

is local with a Coulomb tail

are localized radial functions such that the transformed pseudo acts in the same way as the original form on the reference config.

- semilocal form ...

One has

Page 13: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

ab initio Norm Conserving PseudoPotentials

Kleinman-Bylander fully non-local form

Page 14: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

ab initio Norm Conserving PseudoPotentials

Kleinman-Bylander fully non-local form

Page 15: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

ab initio Norm Conserving PseudoPotentials

Kleinman-Bylander fully non-local form

Page 16: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space
Page 17: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space
Page 18: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space
Page 19: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space
Page 20: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

with

Page 21: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

Ultra Soft PseudoPotentials

where the “augmentation charges” are

are projectors

are atomic states (not necessarily bound)

are pseudo-waves (coinciding with beyond some core radius)

Page 22: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

Ultra Soft PseudoPotentials

where

leading to a generalized eigenvalue problem

Orthogonality with USPP:

Page 23: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

Ultra Soft PseudoPotentials

where

There are additional terms in the density, in the energy, in the hamiltonianin the forces, ...

Page 24: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space
Page 25: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space
Page 26: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space
Page 27: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space
Page 28: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

with

Page 29: computing betas and qs for NCPP/USPP/PAW PseudoPotentialspeople.sissa.it/~degironc/FIST/Slides/13 betas and qs.pdf · The betas and qs functions can be computed in reciprocal space

The betas and qs functions can be computed in reciprocal space as described above.

Alternatively they can be computed directly in real-space interpolating from the radial grid to the fft grid.

If the kinetic energy cutoff used is not converged enough the two procedure ARE NOT the same.

In our experience the G-space treatment is more relieable.