2019-08-04 13:48:41 -07:00
|
|
|
"""
|
|
|
|
PML implementations
|
|
|
|
|
2020-01-08 00:51:56 -08:00
|
|
|
#TODO discussion of PMLs
|
|
|
|
#TODO cpml documentation
|
|
|
|
|
2019-08-04 13:48:41 -07:00
|
|
|
"""
|
|
|
|
# TODO retest pmls!
|
|
|
|
|
|
|
|
from typing import List, Callable, Tuple, Dict
|
|
|
|
import numpy
|
|
|
|
|
2019-11-27 22:59:52 -08:00
|
|
|
from ..fdmath import dx_lists_t, fdfield_t, fdfield_updater_t
|
2019-08-04 13:48:41 -07:00
|
|
|
|
|
|
|
|
|
|
|
__author__ = 'Jan Petykiewicz'
|
|
|
|
|
|
|
|
|
2019-10-27 16:12:48 -07:00
|
|
|
def cpml(direction: int,
|
2019-08-04 13:48:41 -07:00
|
|
|
polarity: int,
|
|
|
|
dt: float,
|
2019-11-27 22:59:52 -08:00
|
|
|
epsilon: fdfield_t,
|
2019-08-04 13:48:41 -07:00
|
|
|
thickness: int = 8,
|
|
|
|
ln_R_per_layer: float = -1.6,
|
|
|
|
epsilon_eff: float = 1,
|
|
|
|
mu_eff: float = 1,
|
|
|
|
m: float = 3.5,
|
|
|
|
ma: float = 1,
|
|
|
|
cfs_alpha: float = 0,
|
|
|
|
dtype: numpy.dtype = numpy.float32,
|
2019-11-27 22:59:52 -08:00
|
|
|
) -> Tuple[Callable, Callable, Dict[str, fdfield_t]]:
|
2019-08-04 13:48:41 -07:00
|
|
|
|
|
|
|
if direction not in range(3):
|
|
|
|
raise Exception('Invalid direction: {}'.format(direction))
|
|
|
|
|
|
|
|
if polarity not in (-1, 1):
|
|
|
|
raise Exception('Invalid polarity: {}'.format(polarity))
|
|
|
|
|
|
|
|
if thickness <= 2:
|
|
|
|
raise Exception('It would be wise to have a pml with 4+ cells of thickness')
|
|
|
|
|
|
|
|
if epsilon_eff <= 0:
|
|
|
|
raise Exception('epsilon_eff must be positive')
|
|
|
|
|
|
|
|
sigma_max = -ln_R_per_layer / 2 * (m + 1)
|
|
|
|
kappa_max = numpy.sqrt(epsilon_eff * mu_eff)
|
|
|
|
alpha_max = cfs_alpha
|
|
|
|
transverse = numpy.delete(range(3), direction)
|
|
|
|
u, v = transverse
|
|
|
|
|
|
|
|
xe = numpy.arange(1, thickness+1, dtype=float)
|
|
|
|
xh = numpy.arange(1, thickness+1, dtype=float)
|
|
|
|
if polarity > 0:
|
|
|
|
xe -= 0.5
|
|
|
|
elif polarity < 0:
|
|
|
|
xh -= 0.5
|
|
|
|
xe = xe[::-1]
|
|
|
|
xh = xh[::-1]
|
|
|
|
else:
|
|
|
|
raise Exception('Bad polarity!')
|
|
|
|
|
|
|
|
expand_slice = [None] * 3
|
|
|
|
expand_slice[direction] = slice(None)
|
2019-11-27 22:59:52 -08:00
|
|
|
expand_slice = tuple(expand_slice)
|
2019-08-04 13:48:41 -07:00
|
|
|
|
|
|
|
def par(x):
|
|
|
|
scaling = (x / thickness) ** m
|
|
|
|
sigma = scaling * sigma_max
|
|
|
|
kappa = 1 + scaling * (kappa_max - 1)
|
|
|
|
alpha = ((1 - x / thickness) ** ma) * alpha_max
|
|
|
|
p0 = numpy.exp(-(sigma / kappa + alpha) * dt)
|
|
|
|
p1 = sigma / (sigma + kappa * alpha) * (p0 - 1)
|
|
|
|
p2 = 1 / kappa
|
|
|
|
return p0[expand_slice], p1[expand_slice], p2[expand_slice]
|
|
|
|
|
|
|
|
p0e, p1e, p2e = par(xe)
|
|
|
|
p0h, p1h, p2h = par(xh)
|
|
|
|
|
|
|
|
region = [slice(None)] * 3
|
|
|
|
if polarity < 0:
|
|
|
|
region[direction] = slice(None, thickness)
|
|
|
|
elif polarity > 0:
|
|
|
|
region[direction] = slice(-thickness, None)
|
|
|
|
else:
|
|
|
|
raise Exception('Bad polarity!')
|
2019-11-27 22:59:52 -08:00
|
|
|
region = tuple(region)
|
2019-08-04 13:48:41 -07:00
|
|
|
|
|
|
|
se = 1 if direction == 1 else -1
|
|
|
|
|
|
|
|
# TODO check if epsilon is uniform in pml region?
|
|
|
|
shape = list(epsilon[0].shape)
|
|
|
|
shape[direction] = thickness
|
|
|
|
psi_e = [numpy.zeros(shape, dtype=dtype), numpy.zeros(shape, dtype=dtype)]
|
|
|
|
psi_h = [numpy.zeros(shape, dtype=dtype), numpy.zeros(shape, dtype=dtype)]
|
|
|
|
|
|
|
|
fields = {
|
|
|
|
'psi_e_u': psi_e[0],
|
|
|
|
'psi_e_v': psi_e[1],
|
|
|
|
'psi_h_u': psi_h[0],
|
|
|
|
'psi_h_v': psi_h[1],
|
|
|
|
}
|
|
|
|
|
|
|
|
# Note that this is kinda slow -- would be faster to reuse dHv*p2h for the original
|
|
|
|
# H update, but then you have multiple arrays and a monolithic (field + pml) update operation
|
2019-11-27 22:59:52 -08:00
|
|
|
def pml_e(e: fdfield_t, h: fdfield_t, epsilon: fdfield_t) -> Tuple[fdfield_t, fdfield_t]:
|
2019-08-04 13:48:41 -07:00
|
|
|
dHv = h[v][region] - numpy.roll(h[v], 1, axis=direction)[region]
|
|
|
|
dHu = h[u][region] - numpy.roll(h[u], 1, axis=direction)[region]
|
|
|
|
psi_e[0] *= p0e
|
|
|
|
psi_e[0] += p1e * dHv * p2e
|
|
|
|
psi_e[1] *= p0e
|
|
|
|
psi_e[1] += p1e * dHu * p2e
|
|
|
|
e[u][region] += se * dt / epsilon[u][region] * (psi_e[0] + (p2e - 1) * dHv)
|
|
|
|
e[v][region] -= se * dt / epsilon[v][region] * (psi_e[1] + (p2e - 1) * dHu)
|
|
|
|
return e, h
|
|
|
|
|
2019-11-27 22:59:52 -08:00
|
|
|
def pml_h(e: fdfield_t, h: fdfield_t) -> Tuple[fdfield_t, fdfield_t]:
|
2019-08-04 13:48:41 -07:00
|
|
|
dEv = (numpy.roll(e[v], -1, axis=direction)[region] - e[v][region])
|
|
|
|
dEu = (numpy.roll(e[u], -1, axis=direction)[region] - e[u][region])
|
|
|
|
psi_h[0] *= p0h
|
|
|
|
psi_h[0] += p1h * dEv * p2h
|
|
|
|
psi_h[1] *= p0h
|
|
|
|
psi_h[1] += p1h * dEu * p2h
|
|
|
|
h[u][region] -= se * dt * (psi_h[0] + (p2h - 1) * dEv)
|
|
|
|
h[v][region] += se * dt * (psi_h[1] + (p2h - 1) * dEu)
|
|
|
|
return e, h
|
|
|
|
|
|
|
|
return pml_e, pml_h, fields
|