This is a 2D phasor-diagram counterpart to the 3D waveguide-chip modulator. Instead of watching light packets fly down two 3D tubes, each arm's optical field is drawn directly as a unit-length phasor rotating in the complex (Argand) plane — the plane itself is the physics, not a camera angle on it.
E_A = e^(iφ_A), E_B = e^(iφ_B) (unit-amplitude arm fields)
E_bar = (E_A + E_B) / 2 → P_bar = |E_bar|² = cos²(Δφ/2)
E_cross = (E_A − E_B) / 2 → P_cross = |E_cross|² = sin²(Δφ/2)
Δφ = φ_A − φ_B = π · V(t) / Vπ, P_bar + P_cross = 1
Vector-adding the two arm phasors and squaring the resultant's length reproduces the textbook cos² coupler transfer function exactly — the parallelogram construction shown live in the diagram is the interference, not an illustration of it.
- Bias sets the DC operating (quadrature) point on the transfer curve.
- Drive swing is the peak-to-peak RF voltage riding on top of the bias, in units of Vπ.
- Push-pull drives the two arms with equal and opposite voltage (±V/2), reaching the same Δφ as a single-arm drive of V but with half the voltage swing per arm — the standard silicon-photonics topology because it also cancels residual optical-frequency chirp. Watch the two arm phasors: push-pull rotates them symmetrically toward and away from each other, single-arm holds one still and rotates only the other — yet the sum/difference vectors, and therefore the output powers, land on identical values for the same drive.
- Extinction ratio is 10·log₁₀(P_max/P_min) of the bar port sampled over one drive cycle — how dark the "off" state gets relative to the "on" state.
Real-world relevance: this exact cos² transfer function governs the silicon-photonic and lithium-niobate MZMs used to encode data onto laser light in every fiber-optic transceiver and data-center interconnect.