Figure

Description
The time-bin qubit encodes quantum information in the temporal degree of freedom of a single photon: and , corresponding to two well-separated time slots (typically ) within a single optical pulse window. Superposition states are prepared by passing a single photon through an unbalanced Mach-Zehnder interferometer, where the path-length difference defines the time-bin separation.
Time-bin encoding is the natural choice for fiber-based quantum communication because it is inherently robust against polarization-mode dispersion and birefringence fluctuations in optical fibers — the dominant decoherence mechanisms that plague polarization-encoded photonic qubits over long distances. The two time bins experience identical polarization transformations in the fiber (assuming slow polarization drift compared to ), making the encoding self-compensating.
Measurement in the computational basis requires only time-resolved single-photon detection, while measurement in the superposition basis uses a second unbalanced interferometer matched to the preparation interferometer. This encoding was introduced by Brendel et al. (1999) and has become the standard for long-distance quantum key distribution and quantum teleportation experiments over deployed fiber networks.
Hamiltonian
The time-bin qubit is described by the single-photon state in a two-mode temporal basis:
where and create a photon in the early and late time bins, respectively.
The unbalanced Mach-Zehnder interferometer implements the beam-splitter transformation:
where is set by the beam-splitter ratio and is the relative phase between the two arms. A balanced beam splitter () with phase prepares:
Motivation
Polarization qubits suffer rapid decoherence in optical fibers due to birefringence, polarization-mode dispersion, and mechanical stress — effects that fluctuate unpredictably over km-scale links. Time-bin encoding eliminates these issues because both temporal modes traverse the same fiber path and experience identical polarization evolution. This makes time-bin qubits the preferred encoding for deployed fiber-based quantum networks, QKD systems, and long-distance quantum teleportation, where stability over hours to days is required without active polarization compensation.
Key Findings
- Franson interferometry using time-bin entangled photon pairs demonstrated violation of Bell inequalities over 50 km of fiber (Brendel et al. 1999).
- Quantum teleportation over 600 m of deployed fiber using time-bin qubits at telecom wavelengths (Marcikic et al. 2004).
- Time-bin encoding adopted in commercial QKD systems (ID Quantique, Toshiba) operating over 100+ km fiber links.
- Long-distance entanglement distribution with time-bin qubits over 300 km of fiber demonstrated using quantum repeater-like protocols (Takesue et al. 2015).
- Compatible with integrated photonic circuits: on-chip time-bin sources and interferometers demonstrated in silicon photonics.
Key Metrics
| Metric | Value | Notes | Fidelity reference |
|---|---|---|---|
| Time-bin separation | 1–5 ns | Set by interferometer path difference | Brendel et al. 1999 |
| Fiber transmission distance | >300 km | At telecom wavelengths (1550 nm) | Takesue et al. 2015 |
| State preparation fidelity | >99% | Interferometric visibility | Marcikic et al. 2004 |
| Bell-state visibility | >95% | Franson interferometry | Brendel et al. 1999 |
| Photon loss rate | ~0.2 dB/km | Standard telecom fiber at 1550 nm | — |
| Detector timing jitter | <100 ps | Superconducting nanowire SPDs | — |
| Operating temperature | 300 K (fiber) / 1 K (detectors) | SNSPDs require cryogenics | — |