def B(x):
"""
Bernoulli function B(x)=x/(exp(x)-1), implemented for double precision
calculation
"""
# For small x, Taylor expansion should be used instead of direct
# formula which will is not even defined for x=0.
BP = 0.0031769106669272879
# Taylor series
x2 = x**2.
taylor = 1. - x / 2. + x2 / 12. - x2**2 / 720.
# Direct calculation
# 1e-20 is added to avoid NaN for small x. It only modifies
# the result if abs(x)<BP. In such a case, the direct formula
# is not used anyway.
# In order to avoid overflow errors, maximum x is limited to 700
# to ensure that exp(xn) is always representable in double precision.
# Anyway xn/(exp(xn)-1.) is almost 0. for large x
xn = ad.where(x < 700., x, 700.)
direct = xn / ((ad.exp(xn) - 1.) + 1e-20)
# Breakpoint BP is chosen so that Taylor series and direct
# calculation coincide in double precision.
return ad.where(abs(x) < BP, taylor, direct)
def c(self, ctx, eq, Ef, numeric_parameters=False):
Ef_raw = Ef
if self.Ef_max is not None:
Ef = where(Ef < self.Ef_max, Ef, self.Ef_max)
if self.logger.isEnabledFor(logging.INFO):
if np.any(nvalue(Ef) != nvalue(Ef_raw)):
self.logger.info(
'c(%r): clipping Ef>%r, max(Ef)=%r' %
(eq.prefix, self.Ef_max, np.amax(
nvalue(Ef_raw))))
N0 = self.N0(ctx, eq)
if numeric_parameters:
N0 = nvalue(N0)
Vt = ctx.varsOf(eq.thermal)['Vt']
if numeric_parameters:
Vt = nvalue(Vt)
v = Ef / Vt
if self.c_limit:
v_raw = v
v = where(v <= 0., v, 0.)
if self.logger.isEnabledFor(logging.INFO):
if np.any(nvalue(v_raw) != nvalue(v)):
self.logger.info(
'c(%r): clipping Ef/kT>0, max(Ef/kT)=%r' %
(eq.prefix, np.amax(
nvalue(v_raw))))
c = exp(v) * N0
return c
def mobility(self, parent, ctx, eq):
mu0 = ctx.param(eq, 'mu0')
gamma = ctx.param(eq, 'gamma')
v = gamma * sqrt(ctx.varsOf(eq.poisson)['Ecellm'] + 1e-10)
v_max = log(1e10)
v_min = -v_max
v = where(v < v_max, v, v_max)
v = where(v > v_min, v, v_min)
mu = mu0 * exp(v)
mu_face = eq.mesh.faceaverage(mu)
ctx.varsOf(eq)['mu_face'] = mu_face
ctx.varsOf(eq)['mu_cell'] = mu
def species_v_D_limited(ctx, eq):
"Species with concentration limitation"
v, D = species_v_D_charged_from_params(ctx, eq)
c = ctx.varsOf(eq)['c']
c = where(v > 0, c[eq.mesh.faces['+']], c[eq.mesh.faces['-']])
v = v * (1. - c / ctx.param(eq, 'N0'))
return v, D
def Aux2(x):
"""
Auxiliary function Aux2(x) = 1./(exp(x)+1)
Properties: Aux2(x)+Aux2(-x)=1
"""
xn = ad.where(x < 700., x, 700.)
return 1. / (ad.exp(xn) + 1.)
def image_correction(self, ctx, eq, ixto):
if not self.image_force:
return 0.
n = eq.mesh.boundaries[self.name]['normal']
F = eq.z * eq.mesh.dotv(ctx.varsOf(eq.poisson)['Ecellv'][ixto], n)
F = where(F > self.F_eps, F, self.F_eps)
return -eq.z * \
functions.EmtageODwyerBarrierLowering(
F, getitem(ctx.varsOf(eq.poisson)['epsilon'], ixto))
def Ef(self, ctx, eq):
c = ctx.varsOf(eq)['c']
c_raw = c
c = where(c > self.c_eps, c, self.c_eps) # avoid NaN
if self.logger.isEnabledFor(logging.INFO):
if np.any(nvalue(c_raw) != nvalue(c)):
self.logger.info(
'Ef(%r): clipping c<%r, min(c)=%r' %
(eq.prefix, self.c_eps, np.amin(nvalue(c_raw))))
N0 = self.N0(ctx, eq)
return ctx.varsOf(eq.thermal)['Vt'] * np.log(c / N0)
def _load(self, ctx, eq):
variables = ctx.varsOf(eq)
if 'gdos_data' in variables:
return variables['gdos_data']
info = self.disorder.disorder_parameters(self, ctx, eq)
nsigma = info['nsigma']
nsigma = where(nsigma > self.nsigma_min, nsigma, self.nsigma_min)
nsigma = where(nsigma < self.nsigma_max, nsigma, self.nsigma_max)
if np.any(nsigma != info['nsigma']):
self.logger.info(
'nsigma clipped to ensure numerical stability: probably not calculating what you want. This is OK in initial Newton iterations, but not in the final one')
N0 = info['N0']
c = ctx.varsOf(eq)['c'] / N0
assert self.c_eps >= self.impl.I_min
assert self.c_max <= self.impl.I_max
c = where(c > self.c_eps, c, self.c_eps)
c = where(c < self.c_max, c, self.c_max)
b = self.impl.b(np.sqrt(2.) * nsigma, c)
info.update(b=b, c=c, nsigma=nsigma)
variables['gdos_data'] = info
return info
def mobility(self, parent, ctx, eq):
info = self._load(ctx, eq)
a = _egdm.N0toa(info['N0'])
nsigma = info['nsigma']
sigma = info['sigma']
mu_cell = _egdm.mu0t(nsigma, info['mu0'])
c = info['c']
if self.use_g1:
mu_cell = mu_cell * \
_egdm.g1(nsigma, where(c < self.g1_max_c, c, self.g1_max_c))
mu_face = eq.mesh.faceaverage(mu_cell)
E = ctx.varsOf(eq.poisson)['E']
if self.use_g2:
En = (E * a) / sigma
En2 = En**2
En2_max = self.g2_max_En**2
mu_face = mu_face * \
_egdm.g2_En2(nsigma, where(En2 < En2_max, En2, En2_max))
ctx.varsOf(eq).update(
mu_face=mu_face,
mu_cell=eq.mesh.cellaveragev(mu_face))
def D_mu(self, parent, ctx, eq):
info = self._load(ctx, eq)
assert self.g3_max_c <= self.gdosImpl.I_max
assert self.c_eps >= self.gdosImpl.I_min
assert self.nsigma_max * np.sqrt(2.) <= self.gdosImpl.a_max
c = info['c']
nsigma = info['nsigma']
inlimit_g3 = c < self.g3_max_c
def branch_if_inlimit(ix):
return getitem(info['b'], ix)
def branch_cut_limit(ix):
return self.impl.b(
np.sqrt(2.) * getitem(nsigma, ix), self.g3_max_c)
b_g3 = branch(inlimit_g3, branch_if_inlimit, branch_cut_limit)
c_g3 = where(inlimit_g3, c, self.g3_max_c)
g3 = _egdm.g3(nsigma, c_g3, impl=self.impl, b=b_g3)
return eq.mesh.faceaverage(g3*info['Vt'])
def evaluate(self, ctx, eq):
if ctx.solver.poissonOnly:
return
assert eq.electron_eq.poisson is eq.hole_eq.poisson
assert eq.electron_eq.thermal is eq.hole_eq.thermal
poissonvars = ctx.varsOf(eq.electron_eq.poisson)
epsilon = poissonvars['epsilon']
Vt = ctx.varsOf(eq.electron_eq.thermal)['Vt']
nvars = ctx.varsOf(eq.electron_eq)
pvars = ctx.varsOf(eq.hole_eq)
evars = ctx.varsOf(eq.eq)
if self.binding_energy_param:
Eb = ctx.param(eq.eq, 'binding_energy')
a = scipy.constants.elementary_charge / \
(Eb * 4 * np.pi * epsilon)
else:
a = ctx.param(eq.eq, 'distance')
Eb = scipy.constants.elementary_charge / \
(4 * np.pi * epsilon * a)
u = 3. / (4. * np.pi * a**3) # m^-3
v = exp(-Eb / Vt) # 1
b = (scipy.constants.elementary_charge / (8 * np.pi)) * \
poissonvars['Ecellm'] / (epsilon * Vt**2) # 1
# b=0.
t = functions.OnsagerFunction(
where(b < self.b_max, b, self.b_max) + self.b_eps) # 1
gamma = scipy.constants.elementary_charge * \
(nvars['mu_cell'] + pvars['mu_cell']) / \
epsilon # m^3 /s
r = gamma * (nvars['c'] * pvars['c'] - ctx.common_param(
[eq.electron_eq, eq.hole_eq], 'npi')) # 1/(m^3 s) # TODO
d = gamma * evars['c'] * u * v * t
ctx.outputCell([eq.eq, self.name, 'recombination'],
r,
unit=ctx.units.dconcentration_dt)
ctx.output([eq.eq, self.name, 'dissociation'],
d,
unit=ctx.units.dconcentration_dt)
f = r - d
self.add(ctx, f, plus=[eq.eq], minus=[eq.hole_eq, eq.electron_eq])
def value(self, ctx, eq):
if isinstance(ctx.solver, solver.RamoShockleyCalculation):
return where(self.name == ctx.solver.boundary_name, 1, 0)
return self.potential(ctx, eq)
def I(self, a, b):
v = self._value(a, b)
l_max = np.log(self.I_max)
v = ad.where(v <= l_max, v, l_max)
return ad.exp(v)
