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Anastasiia Kutakh committed 2021-08-24 01:26:11 -04:00
1 parent aadd720f1e
commit d0bca7633b
2 files changed
+177 -31

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+30 -25
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@@ -14,7 +14,7 @@ __all__ = ['apply_linear_polarizer',
'apply_circular_polarizer',
'apply_jones_matrix',
'generate_linear_polarizer',
'generate_phase_retarder']
'generate_birefringent_obj']
# Abe - split these into two functions
@@ -36,10 +36,10 @@ def generate_linear_polarizer(pol_angle):
cd = t.stack((c, d), dim=-1)
jones_matrices = t.stack((ab, cd), dim=-2)
if single_angle:
return jones_matrices[0].to(dtype=t.cfloat)
return jones_matrices[0].to(dtype=t.cfloat)
else:
return jones_matrices.to(dtype=t.cfloat)
def apply_linear_polarizer(probe, polarizer, multiple_modes=True, transpose=True):
"""
@@ -56,7 +56,7 @@ def apply_linear_polarizer(probe, polarizer, multiple_modes=True, transpose=True
Returns:
--------
linearly polarized probe: t.Tensor
(N)(P)x2x1xMxL
(N)(P)x2x1xMxL
"""
jones_matrices = generate_linear_polarizer(polarizer)
return apply_jones_matrix(probe, jones_matrices, transpose=transpose, multiple_modes=multiple_modes)
@@ -75,19 +75,19 @@ def apply_jones_matrix(probe, jones_matrix, transpose=True, multiple_modes=True)
probe: t.Tensor
A (N)(P)x2xMxL tensor representing the probe
jones_matrix: t.tensor
(N)x2x2x(M)x(L)
(N)x2x2x(M)x(L)
Returns:
--------
a probe with the jones matrix applied: t.Tensor
(N)(P)x2xMxL
(N)(P)x2xMxL
"""
if transpose:
if jones_matrix.dim() < 4:
jones_matrix = jones_matrix[..., None, None]
if multiple_modes:
jones_matrix = jones_matrix.unsqueeze(-5)
jones_matrix = jones_matrix.unsqueeze(-5)
probe = probe[..., None, :, :]
# if jones matrices do not differ from pattern to pattern
if probe.dim() > jones_matrix.dim():
@@ -96,19 +96,19 @@ def apply_jones_matrix(probe, jones_matrix, transpose=True, multiple_modes=True)
elif jones_matrix.dim() > probe.dim():
probe = probe.unsqueeze(0)
# print('apply jonesmatrix: probe', probe.shape, 'matrix:', jones_matrix)
jones_matrix = jones_matrix.transpose(-1, -3).transpose(-2, -4)
jones_matrix = jones_matrix.transpose(-1, -3).transpose(-2, -4)
probe = probe.transpose(-1, -3).transpose(-2, -4)
output = t.matmul(jones_matrix, probe).transpose(-2, -4).transpose(-1, -3).squeeze(-3)
else:
raise NotImplementedError
return output
def apply_phase_retardance(probe, phase_shift, multiple_modes=True):
"""
Shifts the y-component of the field wrt the x-component by a given phase shift
Shifts the y-component of the field wrt the x-component by a given phase shift
Parameters:
----------
@@ -120,7 +120,7 @@ def apply_phase_retardance(probe, phase_shift, multiple_modes=True):
Returns:
--------
probe: t.Tensor
(...)x2x1xMxL
(...)x2x1xMxL
"""
theta = t.as_tensor(phase_shift, dtype=t.float32)
theta = t.deg2rad(theta)
@@ -140,11 +140,11 @@ def apply_circular_polarizer(probe, left_polarized=True, multiple_modes=True):
A (...)x2xMxL tensor representing the probe
left_polarizd: bool
True for the left-polarization, False for the right
Returns:
--------
circularly polarized probe: t.Tensor
(...)x2xMxL
(...)x2xMxL
"""
probe = probe.to(dtype=t.cfloat)
if left_polarized:
@@ -166,7 +166,7 @@ def apply_quarter_wave_plate(probe, fast_axis_angle, multiple_modes=True):
Returns:
--------
polarized probe: t.Tensor
(...)x2x1xMxL
(...)x2x1xMxL
"""
probe = probe.to(dtype=t.cfloat)
theta = math.radians(fast_axis_angle)
@@ -174,7 +174,7 @@ def apply_quarter_wave_plate(probe, fast_axis_angle, multiple_modes=True):
jones_matrix = exponent* t.tensor([[(cos(theta))**2 + 1j * (sin(theta))**2, (1 - 1j) * sin(theta) * cos(theta)], [(1 - 1j) * sin(theta) * cos(theta), (sin(theta))**2 + 1j * (cos(theta))**2]]).to(dtype=t.cfloat)
out = apply_jones_matrix(probe, jones_matrix, multiple_modes=multiple_modes)
return out
return out
def apply_half_wave_plate(probe, fast_axis_angle, multiple_modes=True):
"""
@@ -188,7 +188,7 @@ def apply_half_wave_plate(probe, fast_axis_angle, multiple_modes=True):
Returns:
--------
polarized probe: t.Tensor
(...)x2x1xMxL
(...)x2x1xMxL
"""
probe = probe.to(dtype=t.cfloat)
theta = math.radians(fast_axis_angle)
@@ -196,19 +196,24 @@ def apply_half_wave_plate(probe, fast_axis_angle, multiple_modes=True):
jones_matrix = exponent * t.tensor([[(cos(theta))**2 - (sin(theta))**2, 2 * sin(theta) * cos(theta)], [2 * sin(theta) * cos(theta), (sin(theta))**2 - (cos(theta))**2]]).to(dtype=t.cfloat)
out = apply_jones_matrix(probe, jones_matrix, multiple_modes=multiple_modes)
return out
def generate_phase_retarder(fast_axis=0, phase=0):
phase = t.as_tensor(phase).to(dtype=t.float32)
phase = t.deg2rad(phase)
def coord_rot(angle):
return out
def generate_birefringent_obj(fast_axis=90, phase_ret=10, atten_fast=1, atten_ret=1, global_phase=0):
def to_rad(angle):
angle = t.as_tensor(angle, dtype=t.float32)
angle = t.deg2rad(angle)
return angle
fast_axis = to_rad(fast_axis)
phase_ret = to_rad(phase_ret)
global_phase = to_rad(global_phase)
def coord_rot(angle):
a = t.stack((t.cos(angle), t.sin(angle)), dim=-1)
b = t.stack((-t.sin(angle), t.cos(angle)), dim=-1)
return t.stack((a, b), dim=-2).to(dtype=t.cfloat)
r1 = coord_rot(-fast_axis)
r2 = coord_rot(fast_axis)
p = t.as_tensor([[1, 0], [0, t.exp(phase*1j)]], dtype=t.cfloat)
return t.matmul(r1, t.matmul(p, r2))
p = t.exp(global_phase * 1j) * t.as_tensor([[atten_fast, 0], [0, atten_ret * t.exp(phase_ret*1j)]], dtype=t.cfloat)
return t.matmul(r1, t.matmul(p, r2))