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cleanup

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jan 2018-01-08 23:28:57 -08:00
parent 4067766478
commit c4cbdff751
1 changed files with 63 additions and 62 deletions
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81
fdfd_tools/bloch.py
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@ -447,15 +447,10 @@ def eigsolve(num_modes: int,
continue
break
def rtrace_AtB(A, B):
return real(numpy.sum(A.conj() * B))
def symmetrize(A):
return (A + A.conj().T) * 0.5
max_iters = 10000
for iter in range(max_iters):
U = numpy.linalg.inv(Z.conj().T @ Z)
ZtZ = Z.conj().T @ Z
U = numpy.linalg.inv(ZtZ)
AZ = scipy_op @ Z
AZU = AZ @ U
ZtAZU = Z.conj().T @ AZU
@ -469,47 +464,44 @@ def eigsolve(num_modes: int,
break
KG = scipy_iop @ G
traceGtKG = rtrace_AtB(G, KG)
gamma_numerator = traceGtKG
traceGtKG = _rtrace_AtB(G, KG)
reset_iters = 100
reset_iters = 100 # TODO
if prev_traceGtKG == 0 or iter % reset_iters == 0:
print('RESET!')
logger.inf('CG reset')
gamma = 0
else:
gamma = gamma_numerator / prev_traceGtKG
gamma = traceGtKG / prev_traceGtKG
D = gamma * d_scale * D + KG
d_scale = numpy.sqrt(rtrace_AtB(D, D)) / num_modes
d_scale = numpy.sqrt(_rtrace_AtB(D, D)) / num_modes
D /= d_scale
ZtAZ = Z.conj().T @ AZ
AD = scipy_op @ D
DtD = D.conj().T @ D
DtAD = D.conj().T @ AD
ZtD = Z.conj().T @ D
ZtAD = Z.conj().T @ AD
symZtD = symmetrize(ZtD)
symZtAD = symmetrize(ZtAD)
symZtD = _symmetrize(Z.conj().T @ D)
symZtAD = _symmetrize(Z.conj().T @ AD)
'''
U_sZtD = U @ symZtD
dE = 2.0 * (rtrace_AtB(U, symZtAD) - rtrace_AtB(ZtAZU, U_sZtD))
dE = 2.0 * (_rtrace_AtB(U, symZtAD) -
_rtrace_AtB(ZtAZU, U_sZtD))
S2 = DtD - 4 * symZtD @ U_sZtD
d2E = 2 * (rtrace_AtB(U, DtAD) -
rtrace_AtB(ZtAZU, U @ S2) -
4 * rtrace_AtB(U, symZtAD @ U_sZtD))
d2E = 2 * (_rtrace_AtB(U, DtAD) -
_rtrace_AtB(ZtAZU, U @ (DtD - 4 * symZtD @ U_sZtD)) -
4 * _rtrace_AtB(U, symZtAD @ U_sZtD))
# Newton-Raphson to find a root of the first derivative:
theta = -dE/d2E
if d2E < 0 or abs(theta) >= pi:
theta = -abs(prev_theta) * numpy.sign(dE)
# ZtAZU * ZtZ = ZtAZ for use in line search
ZtZ = Z.conj().T @ Z
ZtAZ = ZtAZU @ ZtZ.conj().T
'''
def Qi_func(theta, memo=[None, None]):
if memo[0] == theta:
@ -525,10 +517,10 @@ def eigsolve(num_modes: int,
# if c or s small, taylor expand
if c < 1e-4 * s and c != 0:
Qi = numpy.linalg.inv(DtD)
Qi = Qi / (s*s) - 2*c/(s*s*s) * (Qi @ symZtD.conj().T @ Qi.conj().T)
Qi = Qi / (s*s) - 2*c/(s*s*s) * (Qi @ (Qi @ symZtD).conj().T)
elif s < 1e-4 * c and s != 0:
Qi = numpy.linalg.inv(ZtZ)
Qi = Qi / (c*c) - 2*s/(c*c*c) * (Qi @ symZtD.conj().T @ Qi.conj().T)
Qi = Qi / (c*c) - 2*s/(c*c*c) * (Qi @ (Qi @ symZtD).conj().T)
else:
raise Exception('Inexplicable singularity in trace_func')
memo[0] = theta
@ -540,22 +532,24 @@ def eigsolve(num_modes: int,
s = numpy.sin(theta)
Qi = Qi_func(theta)
R = c*c * ZtAZ + s*s * DtAD + 2*s*c * symZtAD
trace = rtrace_AtB(R, Qi)
trace = _rtrace_AtB(R, Qi)
return numpy.abs(trace)
#def trace_deriv(theta):
# Qi = Qi_func(theta)
# c2 = numpy.cos(2 * theta)
# s2 = numpy.sin(2 * theta)
# F = -0.5*s2 * (ZtAZ - DtAD) + c2 * symZtAD
# trace_deriv = rtrace_AtB(Qi, F)
'''
def trace_deriv(theta):
Qi = Qi_func(theta)
c2 = numpy.cos(2 * theta)
s2 = numpy.sin(2 * theta)
F = -0.5*s2 * (ZtAZ - DtAD) + c2 * symZtAD
trace_deriv = _rtrace_AtB(Qi, F)
# G = Qi @ F.conj().T @ Qi.conj().T
# H = -0.5*s2 * (ZtZ - DtD) + c2 * symZtD
# trace_deriv -= rtrace_AtB(G, H)
G = Qi @ F.conj().T @ Qi.conj().T
H = -0.5*s2 * (ZtZ - DtD) + c2 * symZtD
trace_deriv -= _rtrace_AtB(G, H)
# trace_deriv *= 2
# return trace_deriv * sgn
trace_deriv *= 2
return trace_deriv * sgn
'''
'''
theta, new_E, new_dE = linmin(theta, E, dE, 0.1, min(tolerance, 1e-6), 1e-14, 0, -numpy.sign(dE) * K_PI, trace_func)
@ -623,3 +617,10 @@ def eigsolve(num_modes: int,
# return x, fx, dfx
def _rtrace_AtB(A, B):
return real(numpy.sum(A.conj() * B))
def _symmetrize(A):
return (A + A.conj().T) * 0.5