def Cyz(self):
sum=np.sum(( iv(self.n,self.l) - ivp(self.n,self.l) )*( self.zeta(self.n)*self.Z(self.n) + self.zeta(-self.n)*self.Z(-self.n) ))
firstTerm = ( iv(0,self.l) - ivp(0,self.l) )*( self.zeta(0)*self.Z(0) + self.zeta(0)*self.Z(0) )
return -self.Byz()*(sum + 0.5*firstTerm )
def dKyy_du(self, u):
sum = np.sum(
self.dlam_du(u) *
(self.n**2 * ivp(self.n, self.l) + 4 * self.l *
(iv(self.n, self.l) - ivp(self.n, self.l)) + 2 * self.l**2 *
(ivp(self.n, self.l) - ivp(self.n, self.l, 2))) *
(self.Z(self.n) + self.Z(-self.n)) +
(self.dzetan_du(u, self.n) * self.Zp(self.n) +
self.dzetan_du(u, -self.n) * self.Zp(-self.n)) *
(self.n**2 * iv(self.n, self.l) + 2 * self.l**2 *
(iv(self.n, self.l) - ivp(self.n, self.l))))
nn = 0
firstTerm = self.dlam_du(u) * (
nn**2 * ivp(nn, self.l) + 4 * self.l *
(iv(nn, self.l) - ivp(nn, self.l)) + 2 * self.l**2 *
(ivp(nn, self.l) - ivp(nn, self.l, 2))) * (
self.Z(nn) + self.Z(-nn)
) + (self.dzetan_du(u, nn) * self.Zp(nn) + self.dzetan_du(u, -nn) *
self.Zp(-nn)) * (nn**2 * iv(nn, self.l) + 2 * self.l**2 *
(iv(nn, self.l) - ivp(nn, self.l)))
return self.pdByy_du(u) * (self.Kyy() -
1) + self.Byy() * (sum + 0.5 * firstTerm)
def det_M1(η, m):
c = η + 1 / η
return lambda z: (
sp.ivp(m, η * z, 2) * sp.hankel1(m, z)
+ c * sp.ivp(m, η * z) * sp.h1vp(m, z)
+ sp.iv(m, η * z) * sp.h1vp(m, z, 2)
)
def rootsAnnSec(m, rMin, rMax, aMin, aMax):
f0 = lambda k: ivp(m, η * k) * hankel1(m, k) / η + iv(m, η * k) * h1vp(
m, k)
f1 = (lambda k: ivp(m, η * k, 2) * hankel1(m, k) + c * ivp(m, η * k) *
h1vp(m, k) + iv(m, η * k) * h1vp(m, k, 2))
A = AnnulusSector(center=0.0, radii=(rMin, rMax), phiRange=(aMin, aMax))
z = A.roots(f0, df=f1)
return z.roots
def dCxy_du(self, u):
sum = np.sum(self.n *
(self.dlam_du(u) *
(ivp(self.n, self.l, 1) - ivp(self.n, self.l, 2)) *
(self.Z(self.n) - self.Z(-self.n)) +
(self.dzetan_du(u, self.n) * self.Zp(self.n) -
self.dzetan_du(u, -self.n) * self.Zp(-self.n)) *
(iv(self.n, self.l) - ivp(self.n, self.l))))
return self.pdBxy_du(u) * self.Cxy() - self.Bxy() * sum
def dKzz_du(self, u):
sum= np.sum(self.dlam_du(u) * ivp(self.n,self.l)*( self.zeta(self.n)*self.Zp(self.n)+self.zeta(-self.n)*self.Zp(-self.n))\
+ iv(self.n,self.l)*( self.dzetan_du(u,self.n)*(self.Zp(self.n)+self.zeta(self.n)*self.Zpp(self.n)) + self.dzetan_du(u,-self.n)*( self.Zp(-self.n)+self.zeta(-self.n)*self.Zpp(-self.n) ) ))
nn = 0
firstTerm = self.dlam_du(u) * ivp(nn,self.l)*( self.zeta(nn)*self.Zp(nn)+self.zeta(-nn)*self.Zp(-nn))\
+ iv(nn,self.l)*( self.dzetan_du(u,nn)*(self.Zp(nn)+self.zeta(nn)*self.Zpp(nn)) + self.dzetan_du(u,-nn)*( self.Zp(-nn)+self.zeta(-nn)*self.Zpp(-nn) ) )
return self.pdBzz_du(u) * (self.Kzz() -
1) - self.Bzz() * (sum + 0.5 * firstTerm)
def test_cylindrical_bessel_i_prime():
order = np.random.randint(0, 10)
value = np.random.rand(1).item()
assert (roundScaler(NumCpp.bessel_in_prime_Scaler(order, value), NUM_DECIMALS_ROUND) ==
roundScaler(sp.ivp(order, value).item(), NUM_DECIMALS_ROUND))
shapeInput = np.random.randint(20, 100, [2, ])
shape = NumCpp.Shape(shapeInput[0].item(), shapeInput[1].item())
cArray = NumCpp.NdArray(shape)
order = np.random.randint(0, 10)
data = np.random.rand(shape.rows, shape.cols)
cArray.setArray(data)
assert np.array_equal(roundArray(NumCpp.bessel_in_prime_Array(order, cArray), NUM_DECIMALS_ROUND),
roundArray(sp.ivp(order, data), NUM_DECIMALS_ROUND))
def Psi(self, r, neff, wl, nu, C):
u = self.u(r, neff, wl)
if neff < self.maxIndex(wl):
psi = (C[0] * jn(nu, u) + C[1] * yn(nu, u) if C[1] else
C[0] * jn(nu, u))
psip = u * (C[0] * jvp(nu, u) + C[1] * yvp(nu, u) if C[1] else
C[0] * jvp(nu, u))
else:
psi = (C[0] * iv(nu, u) + C[1] * kn(nu, u) if C[1] else
C[0] * iv(nu, u))
psip = u * (C[0] * ivp(nu, u) + C[1] * kvp(nu, u) if C[1] else
C[0] * ivp(nu, u))
# if numpy.isnan(psi):
# print(neff, self.maxIndex(wl), C, r)
return psi, psip
def Psi(self, r, neff, wl, nu, C):
u = self.u(r, neff, wl)
if neff < self.maxIndex(wl):
psi = (C[0] * jn(nu, u) + C[1] * yn(nu, u) if C[1] else C[0] *
jn(nu, u))
psip = u * (C[0] * jvp(nu, u) +
C[1] * yvp(nu, u) if C[1] else C[0] * jvp(nu, u))
else:
psi = (C[0] * iv(nu, u) + C[1] * kn(nu, u) if C[1] else C[0] *
iv(nu, u))
psip = u * (C[0] * ivp(nu, u) +
C[1] * kvp(nu, u) if C[1] else C[0] * ivp(nu, u))
# if numpy.isnan(psi):
# print(neff, self.maxIndex(wl), C, r)
return psi, psip
def prime(self, r):
w = self.w(r)
return (self.V_WCA_prime(r) - 2 * self.l0 *
spec.ivp(0, self.l0 * w * r) / spec.i0(self.l0 * w * r) *
(w + r * self.w_prime(r)))
def mag_field_function2(a, b, z, cart=False):
'''give r,phi,z, (or x,y,z) and return br,bphi,bz (or bx,by,bz)'''
if cart:
r = np.sqrt(a**2 + b**2)
phi = np.arctan2(b, a)
else:
r = a
phi = b
iv = np.empty((ns, ms))
ivp = np.empty((ns, ms))
for n in range(ns):
iv[n, :] = special.iv(n, kms[n, :] * np.abs(r))
ivp[n, :] = special.ivp(n, kms[n, :] * np.abs(r))
br = 0.0
bphi = 0.0
bz = 0.0
for n in range(ns):
for m in range(ms):
br += np.cos(n*phi-Ds[n])*ivp[n][m]*kms[n][m]*\
(As[n][m]*np.cos(kms[n][m]*z) + Bs[n][m]*np.sin(kms[n][m]*z))
bz += np.cos(n*phi-Ds[n])*iv[n][m]*kms[n][m]*\
(-As[n][m]*np.sin(kms[n][m]*z) + Bs[n][m]*np.cos(kms[n][m]*z))
if abs(r) > 1e-10:
bphi += n*(-np.sin(n*phi-Ds[n]))*\
(1/abs(r))*iv[n][m]*(As[n][m]*np.cos(kms[n][m]*z) + Bs[n][m]*np.sin(kms[n][m]*z))
if cart:
bx = br * np.cos(phi) - bphi * np.sin(phi)
by = br * np.sin(phi) + bphi * np.cos(phi)
return (bx, by, bz)
else:
return (br, bphi, bz)
def k_2(self, dumk1):
temp = -1 / (3 * np.sqrt(self.Pi))
temp -= dumk1 * special.ivp(1, np.sqrt(self.Pi) * self.r0, 1)
return temp / special.kvp(1, np.sqrt(self.Pi) * self.r0, 1)
def coeff_w_m(η, m, k):
M = np.array(
[[sp.iv(m, η * k), -sp.hankel1(m, k)], [sp.ivp(m, η * k) / η, sp.h1vp(m, k)]]
)
V = np.array([[sp.jv(m, k)], [-sp.jvp(m, k)]])
S = np.linalg.solve(M, V)
return (S[0, 0], S[1, 0])
def __delta(self, nu, u1r1, u2r1, s1, s2, s3, n1sq, n2sq, n3sq):
"""s3 is sign of Delta"""
if s1 < 0:
f = ivp(nu, u1r1) / (iv(nu, u1r1) * u1r1) # c
else:
jnnuu1r1 = jn(nu, u1r1)
if jnnuu1r1 == 0: # Avoid zero division error
return float("inf")
f = jvp(nu, u1r1) / (jnnuu1r1 * u1r1) # a b d
if s1 == s2:
# b d
kappa1 = -(n1sq + n2sq) * f / n2sq
kappa2 = (n1sq * f * f / n2sq -
nu**2 * n3sq / n2sq * (1 / u1r1**2 - 1 / u2r1**2)**2)
else:
# a c
kappa1 = (n1sq + n2sq) * f / n2sq
kappa2 = (n1sq * f * f / n2sq -
nu**2 * n3sq / n2sq * (1 / u1r1**2 + 1 / u2r1**2)**2)
d = kappa1**2 - 4 * kappa2
if d < 0:
return numpy.nan
return u2r1 * (nu / u2r1**2 + (kappa1 + s3 * sqrt(d)) * 0.5)
def mag_field_function(a, b, z, cart=False):
'''give r,phi,z, (or x,y,z) and return br,bphi,bz (or bx,by,bz)'''
if cart:
r = np.sqrt(a**2 + b**2)
phi = np.arctan2(b, a)
else:
r = a
phi = b
# print(r,phi,z)
cms1 = np.zeros(ms)
iv = np.zeros((ms, ns))
ivp = np.zeros((ms, ns))
for m in range(ms):
cms1[m] = ((m + 1) * np.pi / L1)
for n in range(ns):
iv[m][n] = special.iv(n, cms1[m] * r)
ivp[m][n] = special.ivp(n, cms1[m] * r)
# print(iv)
# print(ivp)
# iv = np.empty((ns,ms))
# ivp = np.empty((ns,ms))
# for n in range(ns):
# iv[n,:] = special.iv(n,kms[n,:]*np.abs(r))
# ivp[n,:] = special.ivp(n,kms[n,:]*np.abs(r))
br = 0.0
bphi = 0.0
bz = 0.0
for n in range(ns):
for m in range(ms):
# km = (m+1)*np.pi / L1
br += (Ds[n]*np.sin(n*phi) + (1-Ds[n])*np.cos(n*phi)) * \
ivp[m][n]*cms1[m]*(As[m][n]*np.cos(cms1[m]*z) + Bs[m][n]*np.sin(cms1[m]*z))
if abs(r) > 1e-10:
bphi += n*(Ds[n]*np.cos(n*phi) - (1-Ds[n])*np.sin(n*phi)) * \
(1/r)*iv[m][n]*(As[m][n]*np.cos(cms1[m]*z) + Bs[m][n]*np.sin(cms1[m]*z))
bz += (Ds[n]*np.sin(n*phi) + (1-Ds[n])*np.cos(n*phi)) * \
iv[m][n]*cms1[m]*(-As[m][n]*np.sin(cms1[m]*z) + Bs[m][n]*np.cos(cms1[m]*z))
bz += k3
# for n in range(ns):
# for m in range(ms):
# br += (Cs[n]*np.cos(n*phi)+Ds[n]*np.sin(n*phi))*ivp[n][m]*kms[n][m]*(As[n][m]*np.cos(kms[n][m]*z) + Bs[n][m]*np.sin(-kms[n][m]*z))
# if abs(r)>1e-10:
# bphi += n*(-Cs[n]*np.sin(n*phi)+Ds[n]*np.cos(n*phi))*(1/abs(r))*iv[n][m]*(As[n][m]*np.cos(kms[n][m]*z) + Bs[n][m]*np.sin(-kms[n][m]*z))
# bz += -(Cs[n]*np.cos(n*phi)+Ds[n]*np.sin(n*phi))*iv[n][m]*kms[n][m]*(As[n][m]*np.sin(kms[n][m]*z) + Bs[n][m]*np.cos(-kms[n][m]*z))
if cart:
bx = br * np.cos(phi) - bphi * np.sin(phi)
by = br * np.sin(phi) + bphi * np.cos(phi)
return (bx, by, bz)
else:
return (br, bphi, bz)
def mag_field_function(a,b,z,cart=False):
'''give r,phi,z, (or x,y,z) and return br,bphi,bz (or bx,by,bz)'''
if cart:
r = np.sqrt(a**2+b**2)
phi = np.arctan2(b,a)
else:
r = a
phi = b
iv = np.empty((ns,ms))
ivp = np.empty((ns,ms))
for n in range(ns):
iv[n,:] = special.iv(n,kms[n,:]*np.abs(r))
ivp[n,:] = special.ivp(n,kms[n,:]*np.abs(r))
br = 0.0
bphi = 0.0
bz = 0.0
for n in range(ns):
for m in range(ms):
br += (Cs[n]*np.cos(n*phi)+Ds[n]*np.sin(n*phi))*ivp[n][m]*kms[n][m]*(As[n][m]*np.cos(kms[n][m]*z) + Bs[n][m]*np.sin(-kms[n][m]*z))
if abs(r)>1e-10:
bphi += n*(-Cs[n]*np.sin(n*phi)+Ds[n]*np.cos(n*phi))*(1/abs(r))*iv[n][m]*(As[n][m]*np.cos(kms[n][m]*z) + Bs[n][m]*np.sin(-kms[n][m]*z))
bz += -(Cs[n]*np.cos(n*phi)+Ds[n]*np.sin(n*phi))*iv[n][m]*kms[n][m]*(As[n][m]*np.sin(kms[n][m]*z) + Bs[n][m]*np.cos(-kms[n][m]*z))
if cart:
bx = br*np.cos(phi)-bphi*np.sin(phi)
by = br*np.sin(phi)+bphi*np.cos(phi)
return (bx,by,bz)
else:
return (br,bphi,bz)
def fullDet(b, nu):
a = rho * b
i = ivp(nu, u1*a) / (u1*a * iv(nu, u1*a))
if nu == 1:
k2 = -2
k = 0
else:
k2 = 2 * nu / (u2 * b)**2 - 1 / (nu - 1)
k = -1
X = (1 / (u1*a)**2 + 1 / (u2*a)**2)
P1 = jn(nu, u2*a) * yn(nu, u2*b) - yn(nu, u2*a) * jn(nu, u2*b)
P2 = (jvp(nu, u2*a) * yn(nu, u2*b) - yvp(nu, u2*a) * jn(nu, u2*b)) / (u2 * a)
P3 = (jn(nu, u2*a) * yvp(nu, u2*b) - yn(nu, u2*a) * jvp(nu, u2*b)) / (u2 * b)
P4 = (jvp(nu, u2*a) * yvp(nu, u2*b) - yvp(nu, u2*a) * jvp(nu, u2*b)) / (u2 * a * u2 * b)
A = (n12 * i**2 - n32 * nu**2 * X**2)
if nu == 1:
B = 0
else:
B = 2 * n22 * n32 * nu * X * (P1 * P4 - P2 * P3)
return (n32 * k2 * A * P1**2 +
(n12 + n22) * n32 * i * k2 * P1 * P2 -
(n22 + n32) * k * A * P1 * P3 -
(n12*n32 + n22*n22) * i * k * P1 * P4 +
n22 * n32 * k2 * P2**2 -
n22 * (n12 + n32) * i * k * P2 * P3 -
n22 * (n22 + n32) * k * P2 * P4 -
B)
def fullDet(b, nu):
a = rho * b
i = ivp(nu, u1 * a) / (u1 * a * iv(nu, u1 * a))
if nu == 1:
k2 = -2
k = 0
else:
k2 = 2 * nu / (u2 * b)**2 - 1 / (nu - 1)
k = -1
X = (1 / (u1 * a)**2 + 1 / (u2 * a)**2)
P1 = jn(nu, u2 * a) * yn(nu, u2 * b) - yn(nu, u2 * a) * jn(nu, u2 * b)
P2 = (jvp(nu, u2 * a) * yn(nu, u2 * b) -
yvp(nu, u2 * a) * jn(nu, u2 * b)) / (u2 * a)
P3 = (jn(nu, u2 * a) * yvp(nu, u2 * b) -
yn(nu, u2 * a) * jvp(nu, u2 * b)) / (u2 * b)
P4 = (jvp(nu, u2 * a) * yvp(nu, u2 * b) -
yvp(nu, u2 * a) * jvp(nu, u2 * b)) / (u2 * a * u2 * b)
A = (n12 * i**2 - n32 * nu**2 * X**2)
if nu == 1:
B = 0
else:
B = 2 * n22 * n32 * nu * X * (P1 * P4 - P2 * P3)
return (n32 * k2 * A * P1**2 + (n12 + n22) * n32 * i * k2 * P1 * P2 -
(n22 + n32) * k * A * P1 * P3 -
(n12 * n32 + n22 * n22) * i * k * P1 * P4 +
n22 * n32 * k2 * P2**2 - n22 * (n12 + n32) * i * k * P2 * P3 -
n22 * (n22 + n32) * k * P2 * P4 - B)
def _hefield(self, wl, nu, neff, r):
self._heceq(neff, wl, nu)
for i, rho in enumerate(self.fiber._r):
if r < rho:
break
else:
i += 1
layer = self.fiber.layers[i]
n = layer.maxIndex(wl)
u = layer.u(rho, neff, wl)
urp = u * r / rho
c1 = rho / u
c2 = wl.k0 * c1
c3 = nu * c1 / r if r else 0 # To avoid div by 0
c6 = constants.Y0 * n * n
if neff < n:
B1 = jn(nu, u)
B2 = yn(nu, u)
F1 = jn(nu, urp) / B1
F2 = yn(nu, urp) / B2 if i > 0 else 0
F3 = jvp(nu, urp) / B1
F4 = yvp(nu, urp) / B2 if i > 0 else 0
else:
c2 = -c2
B1 = iv(nu, u)
B2 = kn(nu, u)
F1 = iv(nu, urp) / B1
F2 = kn(nu, urp) / B2 if i > 0 else 0
F3 = ivp(nu, urp) / B1
F4 = kvp(nu, urp) / B2 if i > 0 else 0
A, B, Ap, Bp = layer.C[:, 0] + layer.C[:, 1] * self.alpha
Ez = A * F1 + B * F2
Ezp = A * F3 + B * F4
Hz = Ap * F1 + Bp * F2
Hzp = Ap * F3 + Bp * F4
if r == 0 and nu == 1:
# Asymptotic expansion of Ez (or Hz):
# J1(ur/p)/r (r->0) = u/(2p)
if neff < n:
f = 1 / (2 * jn(nu, u))
else:
f = 1 / (2 * iv(nu, u))
c3ez = A * f
c3hz = Ap * f
else:
c3ez = c3 * Ez
c3hz = c3 * Hz
Er = c2 * (neff * Ezp - constants.eta0 * c3hz)
Ep = c2 * (neff * c3ez - constants.eta0 * Hzp)
Hr = c2 * (neff * Hzp - c6 * c3ez)
Hp = c2 * (-neff * c3hz + c6 * Ezp)
return numpy.array((Er, Ep, Ez)), numpy.array((Hr, Hp, Hz))
def dKxx_du(self, u):
sum = np.sum(self.n**2 *
(self.dlam_du(u) * ivp(self.n, self.l) *
(self.Z(self.n) + self.Z(-self.n)) + iv(self.n, self.l) *
(self.dzetan_du(u, self.n) * self.Zp(self.n) +
self.dzetan_du(u, -self.n) * self.Zp(-self.n))))
return self.pdBxx_du(u) * (self.Kxx() - 1) + self.Bxx() * sum
def lpConstants(self, r, neff, wl, nu, A):
u = self.u(r, neff, wl)
if neff < self.maxIndex(wl):
W = constants.pi / 2
return (W * (u * yvp(nu, u) * A[0] - yn(nu, u) * A[1]),
W * (jn(nu, u) * A[1] - u * jvp(nu, u) * A[0]))
else:
return ((u * kvp(nu, u) * A[0] - kn(nu, u) * A[1]),
(iv(nu, u) * A[1] - u * ivp(nu, u) * A[0]))
def main():
l=np.arange(0.0, 4.0, 0.1)
for m in range(5):
plt.plot(l, ivp(m, l), label = 'm={}'.format(m))
plt.title('Derivative of modified Bessel function of order $m$ (even w. $m$)')
plt.xlabel('$\lambda$')
plt.ylabel('$I_m^{\prime}(\lambda$)')
plt.legend(loc = 'upper left')
plt.savefig('Imprime.pdf')
def lpConstants(self, r, neff, wl, nu, A):
u = self.u(r, neff, wl)
if neff < self.maxIndex(wl):
W = constants.pi / 2
return (W * (u * yvp(nu, u) * A[0] - yn(nu, u) * A[1]),
W * (jn(nu, u) * A[1] - u * jvp(nu, u) * A[0]))
else:
return ((u * kvp(nu, u) * A[0] - kn(nu, u) * A[1]),
(iv(nu, u) * A[1] - u * ivp(nu, u) * A[0]))
def dCxz_du(self, u):
sum = np.sum(
self.n *
(self.dlam_du(u) * ivp(self.n, self.l, 1) *
(-self.Zp(self.n) + self.Zp(-self.n)) + iv(self.n, self.l) *
(-self.dzetan_du(u, self.n) * self.Zpp(self.n) +
self.dzetan_du(u, -self.n) * self.Zpp(-self.n))) / 2)
return self.pdBxz_du(u) * self.Cxz() - self.Bxz() * sum
def calcInt():
plaTrue = ε > -1.0
if plaTrue:
Int = open(f"eps_{ε}_int", "w")
Pla = open(f"eps_{ε}_pla", "w")
else:
Int = open(f"eps_{ε}_int", "w")
for m in range(65):
print(f"m = {m}")
f0 = lambda k: ivp(m, η * k) * hankel1(m, k) / η + iv(m, η * k) * h1vp(
m, k)
f1 = (lambda k: ivp(m, η * k, 2) * hankel1(m, k) + c * ivp(m, η * k) *
h1vp(m, k) + iv(m, η * k) * h1vp(m, k, 2))
t = np.linspace(0.2, 65.0, num=1024)
k = 1j * t
rf = np.real(f0(k))
ind = np.where(rf[1:] * rf[:-1] < 0.0)[0]
roots = np.zeros(np.shape(ind), dtype=complex)
for a, i in enumerate(ind):
C = Circle(center=1j * (t[i] + t[i + 1]) / 2.0,
radius=(t[i + 1] - t[i]))
z = C.roots(f0, df=f1)
roots[a] = z.roots[0]
if plaTrue:
if m:
writeFile(Int, m, roots[1:])
writeFile(Pla, m, roots[[0]])
else:
writeFile(Int, m, roots)
else:
writeFile(Int, m, roots)
if plaTrue:
Int.close()
Pla.close()
else:
Int.close()
def cutoffHE1(b):
a = rho * b
i = ivp(1, u1*a) / (u1*a * i1(u1*a))
X = (1 / (u1*a)**2 + 1 / (u2*a)**2)
P = j1(u2*a) * y1(u2*b) - y1(u2*a) * j1(u2*b)
Ps = (jvp(1, u2*a) * y1(u2*b) - yvp(1, u2*a) * j1(u2*b)) / (u2 * a)
return (i * P + Ps) * (n12 * i * P + n22 * Ps) - n32 * X * X * P * P
def cutoffHE1(b):
a = rho * b
i = ivp(1, u1 * a) / (u1 * a * i1(u1 * a))
X = (1 / (u1 * a)**2 + 1 / (u2 * a)**2)
P = j1(u2 * a) * y1(u2 * b) - y1(u2 * a) * j1(u2 * b)
Ps = (jvp(1, u2 * a) * y1(u2 * b) - yvp(1, u2 * a) * j1(u2 * b)) / (u2 * a)
return (i * P + Ps) * (n12 * i * P + n22 * Ps) - n32 * X * X * P * P
def EH_fields(self, ri, ro, nu, neff, wl, EH, tm=True):
"""
modify EH in-place (for speed)
"""
n = self.maxIndex(wl)
u = self.u(ro, neff, wl)
if ri == 0:
if nu == 0:
if tm:
self.C = numpy.array([1., 0., 0., 0.])
else:
self.C = numpy.array([0., 0., 1., 0.])
else:
self.C = numpy.zeros((4, 2))
self.C[0, 0] = 1 # Ez = 1
self.C[2, 1] = 1 # Hz = alpha
elif nu == 0:
self.C = numpy.zeros(4)
if tm:
c = constants.Y0 * n * n
idx = (0, 3)
self.C[:2] = self.tetmConstants(ri, ro, neff, wl, EH, c, idx)
else:
c = -constants.eta0
idx = (1, 2)
self.C[2:] = self.tetmConstants(ri, ro, neff, wl, EH, c, idx)
else:
self.C = self.vConstants(ri, ro, neff, wl, nu, EH)
# Compute EH fields
if neff < n:
c1 = wl.k0 * ro / u
F3 = jvp(nu, u) / jn(nu, u)
F4 = yvp(nu, u) / yn(nu, u)
else:
c1 = -wl.k0 * ro / u
F3 = ivp(nu, u) / iv(nu, u)
F4 = kvp(nu, u) / kn(nu, u)
c2 = neff * nu / u * c1
c3 = constants.eta0 * c1
c4 = constants.Y0 * n * n * c1
EH[0] = self.C[0] + self.C[1]
EH[1] = self.C[2] + self.C[3]
EH[2] = (c2 * (self.C[0] + self.C[1]) -
c3 * (F3 * self.C[2] + F4 * self.C[3]))
EH[3] = (c4 * (F3 * self.C[0] + F4 * self.C[1]) -
c2 * (self.C[2] + self.C[3]))
return EH
def EH_fields(self, ri, ro, nu, neff, wl, EH, tm=True):
"""
modify EH in-place (for speed)
"""
n = self.maxIndex(wl)
u = self.u(ro, neff, wl)
if ri == 0:
if nu == 0:
if tm:
self.C = numpy.array([1., 0., 0., 0.])
else:
self.C = numpy.array([0., 0., 1., 0.])
else:
self.C = numpy.zeros((4, 2))
self.C[0, 0] = 1 # Ez = 1
self.C[2, 1] = 1 # Hz = alpha
elif nu == 0:
self.C = numpy.zeros(4)
if tm:
c = constants.Y0 * n * n
idx = (0, 3)
self.C[:2] = self.tetmConstants(ri, ro, neff, wl, EH, c, idx)
else:
c = -constants.eta0
idx = (1, 2)
self.C[2:] = self.tetmConstants(ri, ro, neff, wl, EH, c, idx)
else:
self.C = self.vConstants(ri, ro, neff, wl, nu, EH)
# Compute EH fields
if neff < n:
c1 = wl.k0 * ro / u
F3 = jvp(nu, u) / jn(nu, u)
F4 = yvp(nu, u) / yn(nu, u)
else:
c1 = -wl.k0 * ro / u
F3 = ivp(nu, u) / iv(nu, u)
F4 = kvp(nu, u) / kn(nu, u)
c2 = neff * nu / u * c1
c3 = constants.eta0 * c1
c4 = constants.Y0 * n * n * c1
EH[0] = self.C[0] + self.C[1]
EH[1] = self.C[2] + self.C[3]
EH[2] = (c2 * (self.C[0] + self.C[1]) - c3 *
(F3 * self.C[2] + F4 * self.C[3]))
EH[3] = (c4 * (F3 * self.C[0] + F4 * self.C[1]) - c2 *
(self.C[2] + self.C[3]))
return EH
def w_minus_prime(self, r):
if self.r0 == 1:
return r * 0
sPi = np.sqrt(self.Pi)
return (sPi * special.ivp(1, sPi * r, 1) * self.nu_1(r) / r +
special.i1(sPi * r) * self.nu_1_prime(r) / r +
sPi * special.kvp(1, sPi * r, 1) * self.nu_2(r) / r +
special.k1(sPi * r) * self.nu_2_prime(r) / r -
self.w_minus(r) / r)
def dCyz_du(self, u):
sum=np.sum(self.dlam_du(u)*(ivp(self.n,self.l)-ivp(self.n,self.l,2))*(self.zeta(self.n)*self.Z(self.n)+self.zeta(-self.n)*self.Z(-self.n))\
+(iv(self.n,self.l)-ivp(self.n,self.l))*(self.dzetan_du(u,self.n)*(self.Z(self.n)+self.zeta(self.n)*self.Zp(self.n)) + self.dzetan_du(u,-self.n)*(self.Z(-self.n)+self.zeta(-self.n)*self.Zp(-self.n))))
nn = 0
firstTerm = self.dlam_du(u)*(ivp(nn,self.l)-ivp(nn,self.l,2))*(self.zeta(nn)*self.Z(nn)+self.zeta(-nn)*self.Z(-nn))\
+(iv(nn,self.l)-ivp(nn,self.l,1))*(self.dzetan_du(u,nn)*(self.Z(nn)+self.zeta(nn)*self.Zp(nn)) + self.dzetan_du(u,-nn)*(self.Z(-nn)+self.zeta(-nn)*self.Zp(-nn)))
return self.pdByz_du(u) * self.Cyz() - self.Byz() * (sum +
0.5 * firstTerm)
def cutoffHE2(b):
nu = 2
a = rho * b
i = ivp(2, u1*a) / (u1*a * iv(2, u1*a))
X = (1 / (u1*a)**2 + 1 / (u2*a)**2)
P1 = jn(nu, u2*a) * yn(nu, u2*b) - yn(nu, u2*a) * jn(nu, u2*b)
P2 = (jvp(nu, u2*a) * yn(nu, u2*b) - yvp(nu, u2*a) * jn(nu, u2*b)) / (u2 * a)
P3 = (jn(nu, u2*a) * yvp(nu, u2*b) - yn(nu, u2*a) * jvp(nu, u2*b)) / (u2 * b)
P4 = (jvp(nu, u2*a) * yvp(nu, u2*b) - yvp(nu, u2*a) * jvp(nu, u2*b)) / (u2 * a * u2 * b)
A = 2 * nu / (u2 * b)**2 - 1 / (nu - 1)
return (n22 / n32 * (i*P1 + P2) * (n12*i*P3 + n22 * P4) +
(A * i * P1 + A * P2 + i*P3 + P4) * (n12*i*P1 + n22*P2) -
n32 * nu**2 * X**2 * P1 * (A * P1 + P3) -
n22 * nu * X * (nu * X * P1 * P3 + 2 * P1 * P4 - 2 * P2 * P3))
def cutoffHE2(b):
nu = 2
a = rho * b
i = ivp(2, u1 * a) / (u1 * a * iv(2, u1 * a))
X = (1 / (u1 * a)**2 + 1 / (u2 * a)**2)
P1 = jn(nu, u2 * a) * yn(nu, u2 * b) - yn(nu, u2 * a) * jn(nu, u2 * b)
P2 = (jvp(nu, u2 * a) * yn(nu, u2 * b) -
yvp(nu, u2 * a) * jn(nu, u2 * b)) / (u2 * a)
P3 = (jn(nu, u2 * a) * yvp(nu, u2 * b) -
yn(nu, u2 * a) * jvp(nu, u2 * b)) / (u2 * b)
P4 = (jvp(nu, u2 * a) * yvp(nu, u2 * b) -
yvp(nu, u2 * a) * jvp(nu, u2 * b)) / (u2 * a * u2 * b)
A = 2 * nu / (u2 * b)**2 - 1 / (nu - 1)
return (n22 / n32 * (i * P1 + P2) * (n12 * i * P3 + n22 * P4) +
(A * i * P1 + A * P2 + i * P3 + P4) * (n12 * i * P1 + n22 * P2) -
n32 * nu**2 * X**2 * P1 * (A * P1 + P3) - n22 * nu * X *
(nu * X * P1 * P3 + 2 * P1 * P4 - 2 * P2 * P3))
def det_M_real_modes(Kz, Ω, modo, alfa): #xz es en fracción de k0
Kz_real = Kz[0]
Kz_imag = Kz[1]
if Kz_imag == 0:
Kz = Kz_real
else:
Kz = Kz_real + 1j * Kz_imag
V1_star = alfa * (-Ω**2 + Kz**2 + 1)**(1 / 2)
V2_star = alfa * (-Ω**2 + Kz**2)**(1 / 2)
X = V1_star * special.ivp(modo, V1_star) / special.iv(modo, V1_star)
Y = V2_star * special.kvp(modo, V2_star) / special.kv(modo, V2_star)
rta1 = (Ω**2 - 1) * (Ω**2 - Kz**2)**2 * X**2 + Ω**2 * (Ω**2 - Kz**2 -
1)**2 * Y**2
rta2 = (2 * Ω**2 - 1) * (Ω**2 - Kz**2) * (Ω**2 - Kz**2 -
1) * X * Y + modo**2 * Kz**2
return rta1 - rta2
def vConstants(self, ri, ro, neff, wl, nu, EH):
a = numpy.zeros((4, 4))
n = self.maxIndex(wl)
u = self.u(ro, neff, wl)
urp = self.u(ri, neff, wl)
if neff < n:
B1 = jn(nu, u)
B2 = yn(nu, u)
F1 = jn(nu, urp) / B1
F2 = yn(nu, urp) / B2
F3 = jvp(nu, urp) / B1
F4 = yvp(nu, urp) / B2
c1 = wl.k0 * ro / u
else:
B1 = iv(nu, u)
B2 = kn(nu, u)
F1 = iv(nu, urp) / B1 if u else 1
F2 = kn(nu, urp) / B2
F3 = ivp(nu, urp) / B1 if u else 1
F4 = kvp(nu, urp) / B2
c1 = -wl.k0 * ro / u
c2 = neff * nu / urp * c1
c3 = constants.eta0 * c1
c4 = constants.Y0 * n * n * c1
a[0, 0] = F1
a[0, 1] = F2
a[1, 2] = F1
a[1, 3] = F2
a[2, 0] = F1 * c2
a[2, 1] = F2 * c2
a[2, 2] = -F3 * c3
a[2, 3] = -F4 * c3
a[3, 0] = F3 * c4
a[3, 1] = F4 * c4
a[3, 2] = -F1 * c2
a[3, 3] = -F2 * c2
return numpy.linalg.solve(a, EH)
def vConstants(self, ri, ro, neff, wl, nu, EH):
a = numpy.zeros((4, 4))
n = self.maxIndex(wl)
u = self.u(ro, neff, wl)
urp = self.u(ri, neff, wl)
if neff < n:
B1 = jn(nu, u)
B2 = yn(nu, u)
F1 = jn(nu, urp) / B1
F2 = yn(nu, urp) / B2
F3 = jvp(nu, urp) / B1
F4 = yvp(nu, urp) / B2
c1 = wl.k0 * ro / u
else:
B1 = iv(nu, u)
B2 = kn(nu, u)
F1 = iv(nu, urp) / B1 if u else 1
F2 = kn(nu, urp) / B2
F3 = ivp(nu, urp) / B1 if u else 1
F4 = kvp(nu, urp) / B2
c1 = -wl.k0 * ro / u
c2 = neff * nu / urp * c1
c3 = constants.eta0 * c1
c4 = constants.Y0 * n * n * c1
a[0, 0] = F1
a[0, 1] = F2
a[1, 2] = F1
a[1, 3] = F2
a[2, 0] = F1 * c2
a[2, 1] = F2 * c2
a[2, 2] = -F3 * c3
a[2, 3] = -F4 * c3
a[3, 0] = F3 * c4
a[3, 1] = F4 * c4
a[3, 2] = -F1 * c2
a[3, 3] = -F2 * c2
return numpy.linalg.solve(a, EH)
def _tmfield(self, wl, nu, neff, r):
N = len(self.fiber)
C = numpy.array((1, 0))
EH = numpy.zeros(4)
ri = 0
for i in range(N-1):
ro = self.fiber.outerRadius(i)
layer = self.fiber.layers[i]
n = layer.maxIndex(wl)
u = layer.u(ro, neff, wl)
if i > 0:
C = layer.tetmConstants(ri, ro, neff, wl, EH,
constants.Y0 * n * n, (0, 3))
if r < ro:
break
if neff < n:
c1 = wl.k0 * ro / u
F3 = jvp(nu, u) / jn(nu, u)
F4 = yvp(nu, u) / yn(nu, u)
else:
c1 = -wl.k0 * ro / u
F3 = ivp(nu, u) / iv(nu, u)
F4 = kvp(nu, u) / kn(nu, u)
c4 = constants.Y0 * n * n * c1
EH[0] = C[0] + C[1]
EH[3] = c4 * (F3 * C[0] + F4 * C[1])
ri = ro
else:
layer = self.fiber.layers[-1]
u = layer.u(ro, neff, wl)
# C =
return numpy.array((0, ephi, 0)), numpy.array((hr, 0, hz))
def derI(n):
return special.ivp(modo, xt(n) * ρ_barra)
def EH_fields(self, ri, ro, nu, neff, wl, EH, tm=False):
dr = 1e-10
if ri == 0:
# set initial condition
ri = dr
n = self.index(ri, wl)
u = self.u(ri, neff, wl)
if neff < n:
ez = jn(nu, u)
ezp = jvp(nu, u) * u / ri
else:
ez = iv(nu, u)
ezp = ivp(nu, u) * u / ri
hz = 0
hzp = 0
eza = 0
ezap = 0
hza = ez
hzap = ezp
elif nu == 0:
ez, hz = EH
else:
ez, eza = EH[0]
hz, hza = EH[1]
# find derivatives...
nu2 = nu * nu
beta = wl.k0 * neff
beta2 = beta * beta
def f(r, y):
"""
Bures (3.139)
"""
assert r != 0
r2 = r * r
p = (wl.k0 * self.index(r, wl))**2 - beta2
np = self.indexp(r, wl)
n = self.index(r, wl)
yp = numpy.empty(4)
yp[0] = y[2]
yp[1] = y[3]
yp[2] = (y[0] * (nu2 / r2 - p) +
y[2] * (2 * beta2 / p * np / n - 1 / r) -
y[1] * constants.eta0 * (2 * nu * beta * wl.k0 * np /
(r * p * n)))
yp[3] = (y[1] * (nu2 / r2 - p) +
y[3] * (2 * wl.k0**2 * n * np / p - 1 / r) -
y[0] * constants.Y0 * (2 * nu * beta * wl.k0 * n * np /
(r * p)))
return yp
def jac(r, y):
r2 = r * r
p = (wl.k0 * self.index(r, wl))**2 - beta2
np = self.indexp(r, wl)
n = self.index(r, wl)
m = numpy.empty((4, 4))
m[0, :] = (0, 0, 1, 0)
m[1, :] = (0, 0, 0, 1)
m[2, :] = ((nu2 / r2 - p),
-(constants.eta0 * (2 * nu * beta * wl.k0 * np /
(r * p * n))),
(2 * wl.k0**2 * n * np / p - 1 / r),
0)
m[3, :] = (-constants.Y0 * (2 * nu * beta * wl.k0 * n * np /
(r * p)),
0,
(nu2 / r2 - p),
(2 * wl.k0**2 * n * np / p - 1 / r))
return m
s = ode(f, jac).set_integrator("dopri5")
if nu == 0:
s.set_initial_value([ez, hz, ezp, hzp], ri)
ez, hz, ezp, hzp = s.integrate(ro)
EH = ez, hz
Ezp = numpy.array([ezp])
Hzp = numpy.array([hzp])
else:
s.set_initial_value([ez, hz, ezp, hzp], ri)
ez, hz, ezp, hzp = s.integrate(ro)
s.set_initial_value([eza, hza, ezap, hzap], ri)
eza, hza, ezap, hzap = s.integrate(ro)
EH[0] = ez, eza
EH[1] = hz, hza
Ezp = numpy.array([ezp, ezap])
Hzp = numpy.array([hzp, hzap])
# calc ephi and hphi
u = self.u(ro, neff, wl)
n = self.index(ro, wl)
beta = wl.k0 * neff
c = 1 / (wl.k0**2 * (n*n - neff*neff))
EH[2] = c * (beta * EH[0] * nu / ro -
constants.eta0 * wl.k0 * Hzp)
EH[3] = c * (-beta * EH[1] * nu / ro +
constants.Y0 * wl.k0 * n * n * Ezp)
return EH
def coeq(v0, nu, fiber):
r1, r2 = fiber.rho
n1, n2, n3 = fiber.n
na = sqrt(max(fiber.n)**2 - n3**2)
K0 = v0 / (na * r2)
beta = K0 * n3
if n1 > n3:
u1 = K0**2 * (n1**2 - n3**2)
s1 = 1
else:
u1 = K0**2 * (n3**2 - n1**2)
s1 = -1
if n2 > n3:
u2 = K0**2 * (n2**2 - n3**2)
s2 = 1
else:
u2 = K0**2 * (n3**2 - n2**2)
s2 = -1
s = -s1 * s2
u1r1 = u1 * r1
u2r1 = u2 * r1
u2r2 = u2 * r2
X = (u2r1**2 + s * u1r1**2) * nu * beta
if s1 == 1:
Y = jvp(nu, u1r1) / jn(nu, u1r1)
else:
Y = ivp(nu, u1r1) / iv(nu, u1r1)
ju2r1 = jn(nu, u2r1) if s2 == 1 else iv(nu, u2r1)
nu2r1 = yn(nu, u2r1) if s2 == 1 else kn(nu, u2r1)
jpu2r1 = jvp(nu, u2r1) if s2 == 1 else ivp(nu, u2r1)
npu2r1 = yvp(nu, u2r1) if s2 == 1 else kvp(nu, u2r1)
ju2r2 = jn(nu, u2r2) if s2 == 1 else iv(nu, u2r2)
nu2r2 = yn(nu, u2r2) if s2 == 1 else kn(nu, u2r2)
j1u2r2 = jn(nu+1, u2r2)
n1u2r2 = yn(nu+1, u2r2)
M = numpy.empty((4, 4))
M[0, 0] = X * ju2r1
M[0, 1] = X * nu2r1
M[0, 2] = -K0 * (jpu2r1 * u1r1 + s * Y * ju2r1 * u2r1) * u1r1 * u2r1
M[0, 3] = -K0 * (npu2r1 * u1r1 + s * Y * nu2r1 * u2r1) * u1r1 * u2r1
M[1, 0] = -K0 * (n2**2 * jpu2r1 * u1r1 +
s * n1**2 * Y * ju2r1 * u2r1) * u1r1 * u2r1
M[1, 1] = -K0 * (n2**2 * npu2r1 * u1r1 +
s * n1**2 * Y * nu2r1 * u2r1) * u1r1 * u2r1
M[1, 2] = X * ju2r1
M[1, 3] = X * nu2r1
D201 = nu * n3 / u2r2 * (j1u2r2 * nu2r2 - ju2r2 * yn(nu+1, u2r2))
D202 = -((n2**2 + n3**2) * nu * n1u2r2 * nu2r2 / u2r2 +
n3**2 * nu * nu2r2**2 / (nu - 1))
D203 = -(n2**2 * nu * ju2r2 * n1u2r2 / u2r2 +
n3**2 * nu * nu2r2 * j1u2r2 / u2r2 +
n3**2 * nu * (j1u2r2 * nu2r2 +
n1u2r2 * ju2r2) / (2 * (nu - 1)))
D212 = -(n2**2 * nu * nu2r2 * j1u2r2 / u2r2 +
n3**2 * nu * ju2r2 * n1u2r2 / u2r2 +
n3**2 * nu * (n1u2r2 * ju2r2 +
j1u2r2 * nu2r2) / (2 * (nu - 1)))
D213 = -((n2**2 + n3**2) * nu * j1u2r2 * ju2r2 / u2r2 +
n3**2 * nu * ju2r2**2 / (nu - 1))
D223 = nu * n2**2 * n3 / u2r2 * (j1u2r2 * nu2r2 - ju2r2 * n1u2r2)
D30 = M[1, 1] * D201 - M[1, 2] * D202 + M[1, 3] * D203
D31 = M[1, 0] * D201 - M[1, 2] * D212 + M[1, 3] * D213
D32 = M[1, 0] * D202 - M[1, 1] * D212 + M[1, 3] * D223
D33 = M[1, 0] * D203 - M[1, 1] * D213 + M[1, 2] * D223
return M[0, 0] * D30 - M[0, 1] * D31 + M[0, 2] * D32 - M[0, 3] * D33
