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Narrow Linewidth Tunable Laser Source for Quantum Key Distribution (QKD)

Prepare and verify quantum key distribution states with a narrow linewidth tunable laser placed precisely on the ITU-T grid for shared-fibre links.
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Narrow Linewidth Tunable Laser Source for Quantum Key Distribution (QKD)

Industry:

Quantum Key Distribution
Products:
Optical Communication

Key Highlights

  • Clean QKD source or development reference for quantum key distribution, with sub-1 kHz linewidth
  • High side-mode suppression keeps encoded states spectrally indistinguishable
  • Long coherence time for phase-encoded, interferometric and continuous-variable protocols
  • Coarse and fine tuning to sit the quantum channel precisely on the ITU-T grid
  • Supplied and supported in India by USI, authorised distributor for ID Photonics

Why Quantum Key Distribution Depends on the Quality of Its Laser

In most photonic systems, a better laser simply improves performance, but in quantum key distribution the laser is also part of the security argument.

QKD protocols assume the transmitted states differ only in the property chosen to carry the key. If the source drifts in wavelength, or carries spectral impurity or residual side modes, the states can differ in ways the security proof never accounted for. That opens a possible side channel for an eavesdropper.

The same imperfections raise the error rate and lower the secret key rate. A QKD link is only as secure and as fast as the light it starts with.

Where the Narrow Linewidth Tunable Laser Fits in a QKD Link

This sub-1 kHz linewidth tunable laser can act as the QKD source laser that prepares the quantum states, or as the clean development reference that prototype transmitters are measured against. Both roles matter: a QKD transmitter cannot be properly validated against a source that is no cleaner than itself.

How Sub-1 kHz Linewidth Protects Security and Key Rate

A sub-1 kHz linewidth works on two fronts at once. In the frequency domain, the narrow emission and strong side-mode suppression keep states prepared at different settings indistinguishable. In the time domain, the long coherence keeps the phase between pulses well defined across the encoding delay.

  • Tighter security assumptions: fewer spectral signatures that could correlate with the encoded state.
  • More usable key in CV-QKD: excess laser phase noise looks exactly like eavesdropper noise in homodyne or heterodyne detection, so a quieter laser leaves more of the budget for key.
  • Longer reach in DV-QKD: stable interferometric visibility lowers the quantum bit error rate floor, and every fraction of a percent saved there extends usable distance.

Designed for QKD on Real, Shared Fibre

Deployed QKD rarely gets a dark fibre of its own. The quantum channel usually shares the fibre with classical data and the post-processing link, and noise photons from Raman scattering and crosstalk, rather than loss, become the main limit on key rate.

Grid placement

Coarse tuning moves the source quickly to the chosen ITU-T channel. Fine tuning then centres it in the filter passband, so the filters spend their rejection on real noise rather than on avoidable misalignment.

Drift-free key runs

Key accumulation can run for hours or days. Low residual drift stops a slow walk toward a filter edge, which would otherwise look like a falling key rate and be blamed on the fibre or the detectors.

Multiple sources, one platform

Multiplexed experiments often need a signal, a local oscillator and a reference together. CoBrite DX, DX2 and MX chassis host several laser modules in one benchtop, compact or 19-inch rack unit, on a shared thermal and mechanical base and one control interface.

Ready for field trials

Programmatic control logs wavelength and power alongside key-rate data, so a later dip can be checked against the source’s own record. A source that returns to the same operating point after transport and power cycling also saves scarce time on installed-fibre trials.

Assembling a QKD Development Bench

A QKD bench usually starts with the laser in a CoBrite DX, DX2 or MX chassis, with separate modules serving as signal, local oscillator and reference. Before key runs begin, the ID OSA Optical Spectrum Analyser confirms centre wavelength, linewidth and side-mode suppression, so spectral purity is documented rather than assumed. For the classical characterisation that runs alongside the quantum work, the CORX Coherent Optical IQ Receiver provides calibrated coherent detection, and the OMFT IQ Reference Transmitter generates precisely modulated signals from the same laser family.

With every source and instrument from one family, a change in key rate points to the link under test, not to the bench.

Who Uses It

  • QKD and quantum cryptography research groups
  • Quantum communication and secure networking laboratories
  • National quantum mission programmes
  • Telecom and research teams trialling QKD over installed fibre
  • Universities and institutes working on quantum-safe communication

Supply and Support in India

United Spectrum Instruments (USI), Chennai, is the authorised distributor for ID Photonics GmbH in India and supplies this narrow linewidth tunable laser with the CoBrite chassis options, ID OSA, CORX receiver and OMFT transmitter.

Buying the full QKD bench from one source keeps wavelength-band choice, module count, calibration and installation support under one roof. USI can also help match the configuration to the protocol, discrete-variable or continuous-variable, before the order is placed.

Request a Configuration

Download the brochure from this page, use the Enquire Now button, write to sales@unitedspectrum.in, or call +91 93631 83748 / +91 97899 04948. Please mention:

  • QKD protocol: discrete-variable or continuous-variable
  • Role of the source: QKD source, local oscillator or reference
  • ITU-T channels and wavelength band
  • Number of laser modules and preferred chassis
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FAQs

Yes, as the continuous-wave light source, but not on its own. In quantum key distribution research, the narrow linewidth tunable laser supplies the optical carrier for the transmitter and, in continuous-variable QKD, the local oscillator. The QKD system adds the modulation, attenuation and detection the protocol needs. Its sub-1 kHz linewidth and low drift give both discrete-variable and continuous-variable set-ups a stable, repeatable starting point.

CV-QKD measures signal quadratures against a local oscillator using homodyne or heterodyne detection, and shot-noise-limited performance requires signal and local oscillator to stay mutually coherent. Excess laser phase noise shows up as added quadrature noise, which cannot be distinguished from eavesdropper-induced excess noise and therefore reduces the secret key rate directly. A sub-1 kHz linewidth source keeps that contribution negligible.

In multiplexed deployments, the limiting factor is usually noise photons from Raman scattering and crosstalk rather than loss, so the quantum channel has to sit accurately on its ITU-T grid slot and stay inside the filter passband. Coarse tuning reaches the intended channel, fine tuning centres it in the passband and low drift keeps it there through key-accumulation runs lasting hours or days. The ID OSA Optical Spectrum Analyser confirms grid placement before a long run.

United Spectrum Instruments (USI), Chennai, is the distributor for ID Photonics in India and supplies the narrow linewidth tunable laser to quantum technology programmes, research institutes and universities working on quantum key distribution. USI can provide the complete test bench from one supplier, including the CoBrite chassis options, ID OSA, CORX receiver and OMFT, with pre-sales guidance on configuration and after-sales support.

Download the brochure from this page or click Enquire Now. You can also email sales@unitedspectrum.in or call +91 93631 83748 / +91 97899 04948. For an accurate quote for QKD work, mention the protocol (discrete- or continuous-variable), the number of channels, the wavelength range and the chassis option (DX, DX2 or MX) you are considering.

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