Niobium

Datasets:

name

valence electrons

frozen core electrons

default

13

28

'5'

5

36

13 valence electrons

Radial cutoffs and eigenvalues:

id

occ

eig [eV]

cutoff [Bohr]

1s

2

-18795.035

2s

2

-2629.534

2p

6

-2349.185

3s

2

-438.736

3p

6

-346.867

3d

10

-196.299

4s

2

-58.361

2.50

5s

1

-3.980

2.50

4p

6

-34.526

2.50

5p

0

-1.111

2.50

4d

4

-3.041

2.35

d

0

24.171

2.35

The figure shows convergence of the absolute energy (blue line) and atomization energy (orange line) of a Nb dimer relative to completely converged numbers (plane-wave calculation at 1500 eV). Also shown are finite-difference and LCAO (dzp) calculations at gridspacings 0.143 Å, 0.167 Å and 0.200 Å.

../_images/Nb.default.png

Egg-box errors in finite-difference mode:

grid-spacing [Å]

energy error [eV]

0.16

0.0003

0.18

0.0016

0.20

0.0006

5 valence electrons

Radial cutoffs and eigenvalues:

id

occ

eig [eV]

cutoff [Bohr]

1s

2

-18795.035

2s

2

-2629.535

2p

6

-2349.185

3s

2

-438.736

3p

6

-346.867

3d

10

-196.299

4s

2

-58.361

4p

6

-34.526

5s

1

-3.980

2.90

5p

0

-1.111

2.90

4d

4

-3.041

2.60

s

0

23.232

2.90

p

0

26.100

2.90

d

0

24.171

2.60

The figure shows convergence of the absolute energy (blue line) and atomization energy (orange line) of a Nb dimer relative to completely converged numbers (plane-wave calculation at 1500 eV). Also shown are finite-difference and LCAO (dzp) calculations at gridspacings 0.143 Å, 0.167 Å and 0.200 Å.

../_images/Nb.5.png

Egg-box errors in finite-difference mode:

grid-spacing [Å]

energy error [eV]

0.16

0.0008

0.18

0.0013

0.20

0.0019