Transfer functions¶
Overview¶
A transfer function (TransferBase)
describes how an optical system modifies the
spectral content of an envelope
(typically a BaseEnvelope).
It acts multiplicatively in the frequency domain:
Examples¶
Typical transfer functions include:
spectral filters
phase shifts
dispersion
time delays
Normalization and loss¶
Applying a transfer produces an unnormalized result
The modes subsystem enforces:
Here:
\(\zeta_{\mathrm{out}}\) remains normalized
\(\eta\) represents transmitted power
This separation allows loss to be handled at the quantum-state level.
Execution strategies¶
Gaussian-closed (analytic)¶
If both the envelope and transfer support analytic Gaussian representations:
transformation is evaluated in closed form
no sampling is required
output is typically a Gaussian mixture
Numerical filtering¶
For general cases:
spectrum is evaluated on a grid
multiplication is performed pointwise
result is reconstructed via FFT
This path is more general but computationally heavier.
Gaussian transfer formalism¶
Gaussian-compatible transfers can be expressed as
where each \(G_k\) is a Gaussian atom.
Applying such a transfer to a Gaussian envelope yields a finite Gaussian mixture in closed form.
Structure-preserving operations¶
Some operations act directly on envelope parameters:
time delay (shift in \(\tau\))
phase shift
frequency offset
These transformations preserve normalization and typically satisfy
Common transfer implementations include:
Transfers are typically applied using
apply_transfer().
Examples¶
Gaussian band-pass filter (analytic)¶
import numpy as np
from symop.modes.envelopes import GaussianEnvelope
from symop.modes.transfer import GaussianBandpass
from symop.modes.transfer.apply import apply_transfer
import symop.viz as viz
env = GaussianEnvelope(
omega0=10.0,
sigma=2.0,
tau=0.0,
phi0=0.0,
)
filt = GaussianBandpass(
w0=10.0,
sigma_w=0.1,
)
out, eta = apply_transfer(filt, env)
t = np.linspace(-30.0, 30.0, 2000)
w = np.linspace(8.0, 12.0, 2000)
viz.plot(
env,
t=t,
w=w,
title="Input envelope",
normalize_spectrum=False,
freq_relative=True,
show=False,
)
viz.plot(
out,
t=t,
w=w,
title=f"Filtered envelope, eta={eta:.6f}",
normalize_spectrum=False,
freq_relative=True,
show=False,
)
Expected behavior:
output remains in the Gaussian-closed family
\(\eta < 1\) due to filtering loss
Time delay (structure-preserving)¶
import numpy as np
from symop.modes.envelopes import GaussianEnvelope
from symop.modes.transfer import TimeDelay
import symop.viz as viz
env = GaussianEnvelope(
omega0=10.0,
sigma=1.0,
tau=0.0,
phi0=0.0,
)
delay = TimeDelay(tau=2.0)
out, eta = delay.apply_to_gaussian(env)
print(out.tau, eta)
t = np.linspace(-6.0, 10.0, 2000)
w = np.linspace(8.0, 12.0, 2000)
viz.plot(
env,
t=t,
w=w,
title="Before delay",
freq_relative=True,
show=False,
)
viz.plot(
out,
t=t,
w=w,
title="After delay",
freq_relative=True,
show=False,
)
A time delay shifts the envelope in time without introducing loss:
Numerical filtering fallback¶
import numpy as np
from symop.modes.envelopes import GaussianEnvelope
from symop.modes.transfer import RectBandpass
from symop.modes.transfer.apply import apply_transfer
import symop.viz as viz
env = GaussianEnvelope(
omega0=10.0,
sigma=1.0,
tau=0.0,
phi0=0.0,
)
filt = RectBandpass(
w0=10.0,
width=1.0,
)
out, eta = apply_transfer(filt, env)
print(type(out).__name__)
print(f"eta = {eta:.6f}")
t = np.linspace(-10.0, 10.0, 2000)
w = np.linspace(8.0, 12.0, 2000)
viz.plot(
out,
t=t,
w=w,
title=f"Numerically filtered envelope, eta={eta:.6f}",
freq_relative=True,
show=False,
)
(Source code, png, hires.png, pdf)
Expected behavior:
output is a
FilteredEnvelopeevaluation is performed numerically rather than analytically
Design notes¶
Transfers act in the frequency domain.
They may introduce loss, captured by \(\eta\).
Analytic and numerical paths share a common interface.
Transfers compose algebraically.