Description

Broadband Polarization‑Entangled Photon Source – Fiber‑Based Telecom Band EPS-1000

The EPS-1000 broadband polarization-entangled photon source is a compact, fiber‑integrated platform designed for demanding quantum optics and quantum information experiments. Built on periodically‑poled silica fiber (PPSF) technology, this source delivers high‑quality polarization and frequency entanglement at telecom wavelengths, with a broad biphoton bandwidth that comfortably covers both the C‑ and L‑bands. In contrast to bulk‑crystal entanglement sources that require continuous alignment and environmental isolation, the EPS‑1000 uses an all‑fiber, alignment‑free architecture that is optimized for long‑term stability and practical deployment outside of the traditional optics lab.

Operating at a degeneracy wavelength around 1566 nm (tunable within the typical 1530–1580 nm range), the source produces broadband entangled photon pairs with a 3 dB biphoton bandwidth of approximately 80 nm and more than 120 nm possible under certain configurations. This broad spectral coverage enables simultaneous access to multiple wavelength channels, making the source particularly suitable for wavelength‑division‑multiplexed quantum key distribution (QKD) and multi‑channel quantum networking. The sum‑frequency bandwidth of the signal and idler photons is engineered to be very narrow (on the order of 0.1–0.4 nm), providing strong energy‑time correlations while preserving high‑quality polarization entanglement.

The EPS‑1000 is engineered for high pair‑generation efficiency and excellent signal‑to‑noise performance. Under continuous‑wave pump conditions, the typical pair generation rate is on the order of 2 × 106 pairs per second, with specified operation in the 1 × 106 to 4 × 106 pairs‑per‑second range depending on pump parameters and collection conditions. Coincidence‑to‑accidental ratios around 1000 (with a minimum of 100 in less‑ideal conditions) ensure that the produced entangled pairs are clean and well separated from noise, which is crucial for high‑fidelity quantum communication and precision metrology experiments. The entangled state fidelity to the Bell state |Ψ⟩ = (|HV⟩ + |VH⟩)/√2 is typically around 98–99.5%, with matching two‑photon interference visibilities in both HV and diagonal bases, indicating extremely robust polarization correlations.

A key advantage of this source is its integrated optical routing and spectral management. The device incorporates a built‑in optical switch that allows users to choose between a single, common output port or separated signal and idler outputs. When the internal wavelength division multiplexer (WDM) is engaged, the signal and idler photons are directed to two distinct output ports, pre‑separated in wavelength for straightforward connection to downstream instruments, such as single‑photon detectors, analyzers, or quantum memories. This integrated functionality reduces the need for external components, minimizes optical losses, and simplifies system integration for multi‑channel experiments or deployed quantum links.

The EPS‑1000 is purpose‑built for real‑world deployment scenarios where stability, compactness, and ease of use are more important than laboratory‑style adjustability. It offers turn‑key, room‑temperature operation with low power consumption, making it suitable for continuous use in field environments, rack‑mounted systems, or mobile platforms. The all‑fiber, fusion‑spliced design is inherently rugged and mechanically stable, with no free‑space optics or moving alignment stages that could drift over time. As a result, the system is attractive for space‑constrained environments, including satellite payloads, airborne platforms, and remote quantum network nodes where long‑term unattended operation is required.

In terms of physical packaging, the unit comes in a compact enclosure with approximate dimensions of 39 cm (width) × 34.4 cm (depth) × 8.6 cm (height) and a weight of about 4 kg. This footprint is well suited for benchtop use as well as integration into 19‑inch rack systems or custom instrumentation chassis. Fiber pigtails or panel‑mounted connectors (depending on configuration) provide straightforward interfacing with standard single‑mode telecom fibers, enabling direct connection to existing fiber networks, testbeds, or quantum communication setups without extensive optical realignment.

The performance level and architectural choices of this broadband polarization‑entangled source position it competitively among modern entanglement generators used in quantum technology laboratories worldwide. Compared to traditional periodically‑poled lithium niobate or bulk BBO‑based systems, the PPSF‑based EPS‑1000 shows superior environmental robustness, reduced sensitivity to temperature and vibration, and significantly simplified operation, especially at telecom wavelengths. Users working in quantum imaging, quantum metrolo<

OZ Optics Broadband Polarization Entangled Photon Source Telecom Quantum PPSF

Specifications

Operating Wavelength: 1566 nm
Wavelength Stability: -2 – 2 nm
Coincidence-to-accidental Ratio Min: 100
Biphoton Bandwidth Coverage: >80 nm
Photon Pair Wavelength Band: Telecom C- and L-bands
Operating Temperature: Room temperature
Fiber Type: Periodically-poled silica fiber (PPSF)
Operation Mode: Continuous-wave (CW)
Weight: ~4 kg
Height: 8.6 cm
Depth: 34.4 cm
Width: 39 cm
Two-photon Interference Visibility Max: 99.5%
Two-photon Interference Visibility Min: 97%
Two-photon Interference Visibility Typical: 98%
Fidelity To |Ψ⟩=(|HV⟩+|VH⟩)/√2 Max: 99.5%
Fidelity To |Ψ⟩=(|HV⟩+|VH⟩)/√2 Min: 97%
Fidelity To |Ψ⟩=(|HV⟩+|VH⟩)/√2 Typical: 98%
Part Number: EPS-1000-3A3A3A-1566-9/125-S
Coincidence-to-accidental Ratio Typical: 1000
Pair-generation Rate Max: 4×10^6 pairs/second
Pair-generation Rate Min: 1×10^6 pairs/second
Pair-generation Rate Typical: 2×10^6 pairs/second
Signal/Idler Sum Frequency Bandwidth (3 DB) Max: 0.4 nm
Signal/Idler Sum Frequency Bandwidth (3 DB) Min: 0.1 nm
Signal/Idler Sum Frequency Bandwidth (3 DB) Typical: 0.2 nm
Biphoton Bandwidth (3 DB) Max: >120 nm
Biphoton Bandwidth (3 DB) Min: 60 nm
Biphoton Bandwidth (3 DB) Typical: 80 nm
Signal/Idler Degeneracy Wavelength Accuracy: ±2 nm
Signal/Idler Degeneracy Wavelength (max): 1580 nm
Signal/Idler Degeneracy Wavelength (min): 1530 nm
Signal/Idler Degeneracy Wavelength: 1566 ±2 nm

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Features

  • Broadband Polarization-Entangled Photon Pairs – Generates high-quality polarization-entangled photon pairs with >80 nm usable bandwidth (3 dB bandwidth typically ~80 nm, >120 nm max), ideal for dense quantum information protocols and WDM-based systems.
  • Telecom-Wavelength Operation (C- & L-Bands) – Signal/Idler degeneracy centered at 1566 nm (±2 nm), conveniently spanning the C- and L-band region (1530–1580 nm), compatible with standard fiber-optic components, DWDM/WDM infrastructure, and long-distance fiber transmission.
  • Fiber-Based PPSF (Periodically-Poled Silica Fiber) Technology – Uses quasi-phase-matched PPSF for efficient spontaneous parametric down-conversion, providing stable, alignment-free entanglement generation directly in standard 9/125 µm single-mode fiber.
  • High Pair-Generation Rate – Delivers a typical entangled pair generation rate of 2 × 106 pairs/second (up to 4 × 106 pairs/second max) under CW pumping, enabling high data-rate quantum communication and fast coincidence measurements.
  • Exceptional Entanglement Quality – Offers high-fidelity polarization entanglement to the Bell state |Ψ⟩ = (|HV⟩ + |VH⟩)/√2 with typical fidelity of 98–99.5% and two-photon interference visibility of 98–99.5% (no accidental subtraction), supporting demanding quantum information and metrology experiments.
  • Excellent Coincidence-to-Accidental Ratio (CAR) – Provides a typical CAR of ~1000 (min. 100) measured over 16 nm FWHM signal/idler bandwidths, ensuring clean quantum correlations and low noise for high-precision quantum measurements.
  • Built-In Optical Switch and Wavelength-Division Multiplexer – Integrated optical switch routes output either to a common port or through a built-in WDM that separates Signal and Idler photons into two dedicated output ports, allowing flexible use in single-path or dual-path configurations.
  • Turn-Key, Room-Temperature Operation – Fully integrated source with no user alignment required; operates at room temperature with low power consumption, simplifying deployment in laboratories, field systems, and OEM platforms.
  • Rugged, All-Fiber, Alignment-Free Design – Entire optical path is fiber-based, delivering excellent long-term stability against vibration, temperature drifts, and mechanical shocks—well suited for challenging environments, including space-based and mobile quantum instruments.
  • Environmentally Stable & Low-Maintenance – No free-space bulk optics or moving alignment stages; stability of polarization and phase is inherently maintained in fiber, reducing recalibration needs and total cost of ownership compared with bulk-crystal entangled photon sources.
  • Compact & Lightweight Platform – Enclosed unit with approximate dimensions of 39 × 34.4 × 8.6 cm and ~4 kg weight, enabling easy integration into standard racks, optical tables, portable quantum testbeds, and space-/weight-constrained systems.
  • Optimized for Quantum Networking & QKD – Broadband output around telecom bands supports wavelength-division-multiplexed quantum key distribution, multi-channel entanglement distribution, and integration with existing fiber networks, similar to leading entangled sources used in metropolitan-scale quantum links.
  • Ideal for Advanced Quantum Applications – Tailored for quantum imaging, quantum metrology/sensing, quantum key distribution networks, quantum computing, and general quantum information processing, providing a reliable entanglement resource out of the box.
  • Customizable Degeneracy Wavelength – Degeneracy wavelength can be customized within the 1530–1580 nm range on request, allowing optimization for specific DWDM grids or experimental requirements.
  • Narrow Sum-Frequency Bandwidth – Offers a signal/idler sum-frequency (pump) bandwidth of 0.1–0.4 nm (3 dB), beneficial for high spectral purity biphoton generation and enhanced performance in quantum interference and time-bin-sensitive protocols.

Applications

  • Quantum Key Distribution (QKD) Networks – Deployment as a high‑quality entangled photon source for fiber‑based QKD protocols (BBM92, E91, entanglement‑based decoy‑state schemes) over C‑ and L‑band telecom fibers.
  • WDM‑Based Quantum Communication – Multi‑channel entanglement distribution using the broad (>80 nm) bandwidth to populate many wavelength‑division‑multiplexed channels in metropolitan and long‑haul quantum networks.
  • Quantum Repeaters and Entanglement Swapping – Use as a stable entanglement source for elementary links in quantum repeater nodes, entanglement swapping experiments, and quantum memory interfacing at telecom wavelengths.
  • Multi‑User Quantum Networks – Support of star and mesh quantum network architectures, enabling simultaneous entanglement delivery to multiple users over standard DWDM/CWDM infrastructure.
  • Quantum Teleportation Experiments – Generation of high‑fidelity polarization‑entangled photon pairs for laboratory and field‑deployed quantum state teleportation over installed telecom fiber.
  • Device and Protocol Benchmarking – Characterization and stress‑testing of quantum receivers, entanglement‑based protocols, and error‑correction schemes using a bright, stable, and alignment‑free entangled source.
  • Quantum Computing and Photonic Quantum Processors – Entanglement resource for linear‑optical quantum computing experiments, small‑scale cluster‑state generation, and photonic quantum logic gates in integrated platforms.
  • Entanglement‑Based Quantum Simulators – Implementation of small photonic quantum simulators of many‑body systems, quantum walks, and spin models requiring high‑visibility two‑photon interference.
  • Quantum Information Processing Education – Turn‑key entanglement source for university laboratories and training centers teaching quantum information, allowing rapid setup of advanced experiments with minimal alignment.
  • Fundamental Tests of Quantum Mechanics – Bell‑inequality violations, tests of non‑locality, contextuality, and Leggett‑type inequalities using polarization‑entangled photons with high coincidence‑to‑accidental ratio.
  • Quantum State and Process Tomography – Precise characterization of quantum states and operations in fiber‑based and integrated‑optical systems, leveraging high fidelity to |Ψ⟩ = (|HV⟩ + |VH⟩)/√2.
  • Two‑Photon Interference and Hong–Ou–Mandel Experiments – High‑visibility interference measurements in telecom fiber networks and photonic chips for alignment, calibration, and performance validation.
  • Quantum Imaging and Ghost Imaging – Non‑classical imaging schemes, ghost imaging, and sub‑shot‑noise imaging using broadband entangled photon pairs for improved spatial resolution and sensitivity.
  • Quantum Metrology and Sensing – Phase‑sensitive and time‑correlated measurements for precision metrology, dispersion characterization, and non‑linear response studies at single‑photon levels.
  • Entanglement‑Enhanced Interferometry – Fiber‑based interferometric setups exploiting polarization and frequency entanglement to achieve higher sensitivity than classical light in sensing applications.
  • Characterization of Telecom Components – Evaluation of WDMs, filters, polarizers, beam splitters, and integrated photonic circuits via entanglement visibility and coincidence measurements across C‑ and L‑bands.
  • Integrated Quantum Photonics Testing – Feeding on‑chip interferometers, directional couplers, and phase shifters with entangled photons for wafer‑level and packaged‑device characterization.
  • Time‑Bin and Hybrid Entanglement Schemes – Generation and analysis of hybrid polarization–time‑bin or polarization–frequency entangled states for robust long‑distance communication in deployed fibers.
  • Satellite and Space‑Based Quantum Links – Use in environmentally demanding platforms (e.g., satellite payload breadboards, stratospheric balloons) where rugged, alignment‑free all‑fiber design is critical.
  • Field Trials of Quantum Networks – Mobile or rack‑mounted deployment in real‑world testbeds, demonstrating entanglement distribution, synchronization, and long‑term stability over existing telecom infrastructure.
  • Quantum Random Number Generation (QRNG) – Entanglement‑based randomness extraction from measurement outcomes in complementary polarization bases for high‑quality, certifiable random bit streams.

Frequently Asked Questions

What is the OZ Optics Broadband Polarization‑Entangled Photon Source and what makes it different from crystal‑based sources?
The OZ Optics Broadband Polarization‑Entangled Photon Source (model EPS‑1000‑3A3A3A‑1566‑9/125‑S) is a compact, fiber‑based generator of polarization‑entangled photon pairs at telecom wavelengths. Unlike bulk‑crystal SPDC sources, it uses periodically‑poled silica fiber (PPSF) and an all‑fiber architecture. This gives it turnkey, room‑temperature operation, excellent environmental stability, and no free‑space alignment. It offers high‑quality polarization and frequency entanglement across a very broad bandwidth (typically ~80 nm, >60 nm guaranteed) around 1566 nm, covering the C‑ and L‑bands for telecom‑compatible quantum communication, sensing, and quantum information processing.
What are the key optical specifications of this entangled photon source (wavelength, bandwidth, and pair generation rate)?
Under continuous‑wave (CW) operation, the EPS‑1000 source provides polarization‑entangled photon pairs with a signal/idler degeneracy wavelength typically set to 1566 ± 2 nm (customizable between ~1530 and 1580 nm, usually at the C/L‑band boundary). The biphoton bandwidth (3 dB, before separating signal and idler) is typically about 80 nm, with a minimum of 60 nm and often exceeding 120 nm. The sum‑frequency bandwidth of the signal/idler is very narrow (0.1–0.4 nm), indicative of strong energy‑time correlations. The typical pair‑generation rate is about 2×10^6 pairs per second (1×10^6 min., 4×10^6 max.) under the specified CW conditions, providing a bright and spectrally broad entangled photon source for WDM and broadband quantum applications.
How high is the entanglement quality (fidelity, visibility, and CAR) and how are these values measured?
The EPS‑1000 broadband polarization‑entangled photon source is designed for high‑quality polarization entanglement. Typical coincidence‑to‑accidental ratio (CAR) values are around 1000 (with a minimum of 100) when measured with free‑running SPAD detectors with ~5 kHz dark counts, 16 nm FWHM filters on signal and idler, and a 0.65 ns coincidence window. The measured fidelity to the Bell state |Ψ⟩ = (|HV⟩ + |VH⟩)/√2 is typically about 98–99.5% over conjugate signal/idler pairs of 1 nm FWHM bandwidth across an 80 nm range centered at degeneracy, without subtracting accidentals. Two‑photon interference visibility in HV and AD bases is also typically 98–99.5%, limited primarily by detector dark counts. These metrics place the device among state‑of‑the‑art fiber‑based entangled photon sources used in quantum key distribution, metrology, and quantum information experiments.
How does the built‑in optical switch and wavelength division multiplexer (WDM) work and what output configurations are available?
The EPS‑1000 includes an internal optical switch and an integrated wavelength division multiplexer (WDM) to provide flexible output configurations. In one mode, the built‑in optical switch directs the entangled photon pairs to a common output port, where signal and idler share the same fiber and can be separated externally with user‑defined filters or WDMs. In another mode, the switch routes the light through the internal WDM so that signal and idler photons of each entangled pair are separated into two distinct output ports according to their wavelengths. This simplifies setups for coincidence measurements, quantum key distribution, and multi‑channel WDM‑based quantum networks, because the user can choose between a single‑fiber broadband output or already separated signal/idler channels without additional bulk optics.
What are the physical characteristics and environmental advantages of this all‑fiber PPSF entangled photon source?
The device is built as a rugged, all‑fiber module using periodically‑poled silica fiber (PPSF) technology. Its enclosure has approximate dimensions of 39 × 34.4 × 8.6 cm (width × depth × height) and weighs about 4 kg, making it compact and relatively lightweight compared with many free‑space bulk‑optic entanglement sources. The all‑fiber design eliminates the need for daily alignment, is less sensitive to vibration and temperature changes, and supports room‑temperature operation with low power consumption. These characteristics make it suitable for deployment in field systems, long‑term lab experiments, and even space‑constrained or space‑qualified platforms where robustness and environmental stability are critical.
What applications is the broadband polarization‑entangled photon source best suited for?
This broadband, telecom‑wavelength polarization‑entangled photon source is optimized for advanced quantum optics and quantum information applications. Typical use cases include quantum key distribution (QKD) over standard fiber networks, especially WDM‑based multi‑channel QKD schemes leveraging the broad C‑ and L‑band coverage; quantum computing and quantum information processing experiments that require high‑fidelity polarization entanglement; quantum imaging and ghost imaging that benefit from strong spatial and spectral correlations; and quantum metrology or sensing protocols that rely on two‑photon interference and energy‑time entanglement. Because it operates in standard telecom bands and is all‑fiber, it integrates readily with existing fiber‑optic components, filters, DWDM systems, and single‑photon detectors.
Can the degeneracy wavelength or operating band be customized, and how does this affect integration with telecom systems?
The specified model EPS‑1000‑3A3A3A‑1566‑9/125‑S has a typical degeneracy wavelength of 1566 ± 2 nm, chosen near the boundary of the C‑ and L‑bands to maximize compatibility with telecom infrastructure. According to the datasheet, the degeneracy wavelength can be customized within the approximate 1530–1580 nm range to align with particular DWDM grids, specific ITU channels, or application‑specific bands. Adjusting the degeneracy wavelength allows users to target desired signal/idler wavelength combinations while still benefiting from the broad biphoton bandwidth and narrow sum‑frequency bandwidth. This flexibility simplifies integration into existing fiber‑optic networks, quantum key distribution testbeds, and multi‑channel quantum experiments that must coexist with classical telecom traffic.

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