root / ase / dft / dos.py @ 7
Historique | Voir | Annoter | Télécharger (2,11 ko)
| 1 | 1 | tkerber | from math import pi, sqrt |
|---|---|---|---|
| 2 | 1 | tkerber | |
| 3 | 1 | tkerber | import numpy as np |
| 4 | 1 | tkerber | |
| 5 | 1 | tkerber | |
| 6 | 1 | tkerber | class DOS: |
| 7 | 1 | tkerber | def __init__(self, calc, width=0.1, window=None, npts=201): |
| 8 | 1 | tkerber | """Electronic Density Of States object.
|
| 9 | 1 | tkerber |
|
| 10 | 1 | tkerber | calc: calculator object
|
| 11 | 1 | tkerber | Any ASE compliant calculator object.
|
| 12 | 1 | tkerber | width: float
|
| 13 | 1 | tkerber | Width of guassian smearing.
|
| 14 | 1 | tkerber | window: tuple of two float
|
| 15 | 1 | tkerber | Use ``window=(emin, emax)``. If not specified, a window
|
| 16 | 1 | tkerber | big enough to hold all the eigenvalues will be used.
|
| 17 | 1 | tkerber | npts: int
|
| 18 | 1 | tkerber | Number of points.
|
| 19 | 1 | tkerber |
|
| 20 | 1 | tkerber | """
|
| 21 | 1 | tkerber | |
| 22 | 1 | tkerber | self.npts = npts
|
| 23 | 1 | tkerber | self.width = width
|
| 24 | 1 | tkerber | self.w_k = calc.get_k_point_weights()
|
| 25 | 1 | tkerber | self.nspins = calc.get_number_of_spins()
|
| 26 | 1 | tkerber | self.e_skn = np.array([[calc.get_eigenvalues(kpt=k, spin=s)
|
| 27 | 1 | tkerber | for k in range(len(self.w_k))] |
| 28 | 1 | tkerber | for s in range(self.nspins)]) |
| 29 | 1 | tkerber | self.e_skn -= calc.get_fermi_level()
|
| 30 | 1 | tkerber | |
| 31 | 1 | tkerber | if window is None: |
| 32 | 1 | tkerber | emin = self.e_skn.min() - 5 * self.width |
| 33 | 1 | tkerber | emax = self.e_skn.max() + 5 * self.width |
| 34 | 1 | tkerber | else:
|
| 35 | 1 | tkerber | emin, emax = window |
| 36 | 1 | tkerber | |
| 37 | 1 | tkerber | self.energies = np.linspace(emin, emax, npts)
|
| 38 | 1 | tkerber | |
| 39 | 1 | tkerber | def get_energies(self): |
| 40 | 1 | tkerber | """Return the array of energies used to sample the DOS."""
|
| 41 | 1 | tkerber | return self.energies |
| 42 | 1 | tkerber | |
| 43 | 1 | tkerber | def delta(self, energy): |
| 44 | 1 | tkerber | """Return a delta-function centered at 'energy'."""
|
| 45 | 1 | tkerber | x = -((self.energies - energy) / self.width)**2 |
| 46 | 1 | tkerber | return np.exp(x) / (sqrt(pi) * self.width) |
| 47 | 1 | tkerber | |
| 48 | 1 | tkerber | def get_dos(self, spin=None): |
| 49 | 1 | tkerber | """Get array of DOS values.
|
| 50 | 1 | tkerber |
|
| 51 | 1 | tkerber | The *spin* argument can be 0 or 1 (spin up or down) - if not
|
| 52 | 1 | tkerber | specified, the total DOS is returned.
|
| 53 | 1 | tkerber | """
|
| 54 | 1 | tkerber | |
| 55 | 1 | tkerber | if spin is None: |
| 56 | 1 | tkerber | if self.nspins == 2: |
| 57 | 1 | tkerber | # Spin-polarized calculation, but no spin specified -
|
| 58 | 1 | tkerber | # return the total DOS:
|
| 59 | 1 | tkerber | return self.get_dos(spin=0) + self.get_dos(spin=1) |
| 60 | 1 | tkerber | else:
|
| 61 | 1 | tkerber | spin = 0
|
| 62 | 1 | tkerber | |
| 63 | 1 | tkerber | dos = np.zeros(self.npts)
|
| 64 | 1 | tkerber | for w, e_n in zip(self.w_k, self.e_skn[spin]): |
| 65 | 1 | tkerber | for e in e_n: |
| 66 | 1 | tkerber | dos += w * self.delta(e)
|
| 67 | 1 | tkerber | return dos |