-
Notifications
You must be signed in to change notification settings - Fork 0
Expand file tree
/
Copy pathThesisProblem.py
More file actions
215 lines (169 loc) · 8.32 KB
/
ThesisProblem.py
File metadata and controls
215 lines (169 loc) · 8.32 KB
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
51
52
53
54
55
56
57
58
59
60
61
62
63
64
65
66
67
68
69
70
71
72
73
74
75
76
77
78
79
80
81
82
83
84
85
86
87
88
89
90
91
92
93
94
95
96
97
98
99
100
101
102
103
104
105
106
107
108
109
110
111
112
113
114
115
116
117
118
119
120
121
122
123
124
125
126
127
128
129
130
131
132
133
134
135
136
137
138
139
140
141
142
143
144
145
146
147
148
149
150
151
152
153
154
155
156
157
158
159
160
161
162
163
164
165
166
167
168
169
170
171
172
173
174
175
176
177
178
179
180
181
182
183
184
185
186
187
188
189
190
191
192
193
194
195
196
197
198
199
200
201
202
203
204
205
206
207
208
209
210
211
212
213
214
215
from baseCompounds import *
from PotentialWell import PotentialWell
from PotWellSolver import *
import numpy as np
from MGCMTStencilMaker import MGCMTStencilMaker
from MGCMTSolver import MGCMTSolver
from MGCMTProcessor import MGCMTProcessor
import scipy.sparse.linalg as sparsela
import scipy.sparse as sparse
import matplotlib.pyplot as plt
from operator import itemgetter
max_iters = 10 # Maximaal aantal V-cycles
iter_x = np.arange(0, max_iters + 1)
solver = MGCMTSolver()
stencil_maker = MGCMTStencilMaker()
processor = MGCMTProcessor()
gridsize = 2**8
machine_eps = np.finfo(float).eps
tolerance = machine_eps
num_eigenvalues = 6
k = 0 # Zoek de oplossingen in het gamma punt
potwell = PotentialWell("z") # Opsluiting in de z-richting
GaAs = Compound(GaAsValues) # Oplossen voor GaAs. Si is ook mogelijk.
potwellsolver_eigs = PotWellSolver(GaAs, potwell, 4)
potwellsolver_eigs.setGridPoints(gridsize)
potwellsolver_eigs.setXRange(-1, 1)
x_axis = potwellsolver_eigs.getXAxisVector()
hamiltonian_dense = potwellsolver_eigs.makeMatrix(k)
potwellsolver_eigs.setDense(0)
hamiltonian_sparse = potwellsolver_eigs.makeMatrix(k)
print "Direct method"
eigenvalues_eigs, eigenvectors_eigs = np.linalg.eigh(hamiltonian_dense)
del hamiltonian_dense
print "Direct method end"
eigenvalues_eigs *= unitE
eigenvalues_eigs = sorted(eigenvalues_eigs)
eigenvectors_eigs = np.array(eigenvectors_eigs)
print "Eigenvalues direct method: ", eigenvalues_eigs
# Multigrid method
########################################################
print "Iterative method"
# Generate guesses for fine grid
#2**5 is minimum voor correcte resultaten. 2**4 geeft foute convergentie
bad_gridsize = 2**5
potwellsolver_eigs.setGridPoints(bad_gridsize)
bad_hamiltonian = potwellsolver_eigs.makeMatrix(k)
eigenvalues_shift = np.zeros((1, num_eigenvalues))
eigenvectors_shift = np.zeros((gridsize * potwellsolver_eigs.matrixDim, num_eigenvalues), dtype=complex)
bad_eigenvalues, bad_eigenvectors = sparsela.eigsh(bad_hamiltonian, k=num_eigenvalues, which='SM', tol=tolerance)
# Sorteren van de eigenwaarden en eigenvectoren
bad_eigenvectors = np.array([np.array(bad_eigenvectors[:, i]) for i in xrange(num_eigenvalues)])
bad_eigenvalues, bad_eigenvectors = zip(*sorted(zip(bad_eigenvalues, bad_eigenvectors), key=itemgetter(0)))
bad_eigenvalues = np.array(bad_eigenvalues)
print "Initial guess eigenvalues: %s" % (bad_eigenvalues * unitE)
w0 = np.zeros((gridsize * potwellsolver_eigs.matrixDim, 1))
interpolated_vectors = np.zeros((gridsize * potwellsolver_eigs.matrixDim, num_eigenvalues), dtype=complex)
interpolation_matrix = stencil_maker.interpolation(bad_gridsize * potwellsolver_eigs.matrixDim, gridsize * potwellsolver_eigs.matrixDim)
for i in xrange(num_eigenvalues):
interpolated_vectors[:, i] = interpolation_matrix * bad_eigenvectors[i]
interpolated_vectors[:, i] /= np.linalg.norm(interpolated_vectors[:, i])
residuals = np.zeros((len(iter_x), num_eigenvalues))
for i in xrange(num_eigenvalues):
eigenvectors_shift[:, i] = interpolation_matrix * bad_eigenvectors[i]
eigenvectors_shift[:, i] /= np.linalg.norm(eigenvectors_shift[:, i])
shifted_matrix = hamiltonian_sparse - sparse.eye(gridsize * potwellsolver_eigs.matrixDim) * bad_eigenvalues[i] # Create shifted matrix
iters = 0
residuals[0, i] = np.linalg.norm(eigenvectors_shift[:, i] - shifted_matrix * w0)
while iters < max_iters:
w = w0
#Lowest good level is 2**5
w = solver.vcycle(w, eigenvectors_shift[:, i], hamiltonian_sparse, stencil_maker, shift=bad_eigenvalues[i], lowest_level=2**5, smoother=solver.gseidel)
eigenvectors_shift[:, i] = w / np.linalg.norm(w)
iters += 1
residuals[iters, i] = np.linalg.norm(eigenvectors_shift[:, i] - shifted_matrix * w)
print iters, residuals[iters, i]
eigenvalues_shift[0, i] = np.dot(eigenvectors_shift[:, i].conj().T, hamiltonian_sparse.dot(eigenvectors_shift[:, i]))
eigenvalues_shift[0, i] = eigenvalues_shift[0, i].real * unitE # Real call because eigenvalues have a very very small imaginary part, compuational artifact ?
print "Iterative method end"
print "Eigenvalues shift method: ", eigenvalues_shift
#######################################################################################
fig_eigs, axarray = plt.subplots(num_eigenvalues / 2, 2, sharex='col', sharey='row')
row_index = 0
column_index = 0
for i in xrange(num_eigenvalues):
if i != 0:
if i % 2 == 0:
row_index += 1
if column_index > 0:
column_index -= 1
else:
column_index += 1
HH1 = eigenvectors_eigs[0:gridsize, i]
LH1 = eigenvectors_eigs[gridsize:2*gridsize, i]
LH2 = eigenvectors_eigs[2*gridsize:3*gridsize, i]
HH2 = eigenvectors_eigs[3*gridsize:4*gridsize, i]
HH_sq = np.ma.conjugate(HH1) * HH1 + np.ma.conjugate(HH2) * HH2
LH_sq = np.ma.conjugate(LH1) * LH1 + np.ma.conjugate(LH2) * LH2
axarray[row_index, column_index].plot(x_axis, HH_sq, c='b', label="Heavy Hole")
axarray[row_index, column_index].plot(x_axis, LH_sq, c='g', label="Light Hole")
axarray[row_index, column_index].set_title("n = " + str(i+1))
axarray[row_index, column_index].legend()
plt.suptitle("Eigh Method (DIRECT)")
fig_eigs.text(0.5, 0.04, 'x', ha='center', va='center')
fig_eigs.text(0.06, 0.5, '|Psi(x)|^2', ha='center', va='center', rotation='vertical')
fig_shift, axarray = plt.subplots(num_eigenvalues / 2, 2, sharex='col', sharey='row')
row_index = 0
column_index = 0
for i in xrange(num_eigenvalues):
if i != 0:
if i % 2 == 0:
row_index += 1
if column_index > 0:
column_index -= 1
else:
column_index += 1
HH1_shift = eigenvectors_shift[0:gridsize, i]
LH1_shift = eigenvectors_shift[gridsize:2*gridsize, i]
LH2_shift = eigenvectors_shift[2*gridsize:3*gridsize, i]
HH2_shift = eigenvectors_shift[3*gridsize:4*gridsize, i]
HH_sq = np.ma.conjugate(HH1_shift) * HH1_shift + np.ma.conjugate(HH2_shift) * HH2_shift
LH_sq = np.ma.conjugate(LH1_shift) * LH1_shift + np.ma.conjugate(LH2_shift) * LH2_shift
axarray[row_index, column_index].plot(x_axis, HH_sq, c='b', label="Heavy Hole")
axarray[row_index, column_index].plot(x_axis, LH_sq, c='g', label="Light Hole")
axarray[row_index, column_index].set_title("n = " + str(i+1))
axarray[row_index, column_index].legend()
plt.suptitle("Multigrid method")
fig_shift.text(0.5, 0.04, 'x', ha='center', va='center')
fig_shift.text(0.06, 0.5, '|Psi(x)|^2', ha='center', va='center', rotation='vertical')
fig_guess, axarray = plt.subplots(num_eigenvalues / 2, 2, sharex='col', sharey='row')
row_index = 0
column_index = 0
for i in xrange(num_eigenvalues):
if i != 0:
if i % 2 == 0:
row_index += 1
if column_index > 0:
column_index -= 1
else:
column_index += 1
HH1_int = interpolated_vectors[0:gridsize, i]
LH1_int = interpolated_vectors[gridsize:2*gridsize, i]
LH2_int = interpolated_vectors[2*gridsize:3*gridsize, i]
HH2_int = interpolated_vectors[3*gridsize:4*gridsize, i]
HH_sq = np.ma.conjugate(HH1_int) * HH1_int + np.ma.conjugate(HH2_int) * HH2_int
LH_sq = np.ma.conjugate(LH1_int) * LH1_int + np.ma.conjugate(LH2_int) * LH2_int
axarray[row_index, column_index].plot(x_axis, HH_sq, c='b', label="Heavy Hole")
axarray[row_index, column_index].plot(x_axis, LH_sq, c='g', label="Light Hole")
axarray[row_index, column_index].set_title("n = " + str(i+1))
axarray[row_index, column_index].legend()
plt.suptitle("Begingok voor Multigrid methode")
fig_guess.text(0.5, 0.04, 'x', ha='center', va='center')
fig_guess.text(0.06, 0.5, '|Psi(x)|^2', ha='center', va='center', rotation='vertical')
fig_residuals, axarray = plt.subplots(num_eigenvalues / 2, 2, sharex='col', sharey='row')
row_index = 0
column_index = 0
for i in xrange(num_eigenvalues):
if i != 0:
if i % 2 == 0:
row_index += 1
if column_index > 0:
column_index -= 1
else:
column_index += 1
axarray[row_index, column_index].plot(iter_x, residuals[:, i], c='b', label="Heavy Hole")
axarray[row_index, column_index].set_title("n = " + str(i+1))
plt.suptitle("2-norm van residu")
fig_residuals.text(0.5, 0.04, 'x', ha='center', va='center')
fig_residuals.text(0.06, 0.5, 'Residu', ha='center', va='center', rotation='vertical')
plt.show()