Scontel TCOPRS-CCR-SW-25 Superconducting Single-Photon Detector (SSPD) System
| Origin | Russia |
|---|---|
| Manufacturer Type | Authorized Distributor |
| Origin Category | Imported |
| Model | TCOPRS-CCR-SW-25 |
| Pricing | Upon Request |
Overview
The Scontel TCOPRS-CCR-SW-25 Superconducting Single-Photon Detector (SSPD) System is a cryogenically operated, fiber-coupled quantum sensor engineered for ultra-low-light detection in the visible to near-infrared spectral range (400–1550 nm). Based on nanowire superconducting technology using stoichiometric niobium nitride (NbN) thin films patterned into meander-shaped active areas, the system operates at temperatures below 4.2 K—leveraging either a closed-cycle cryocooler (Type 1, helium-free) or a liquid helium–filled dewar (Type 2). Its detection principle relies on the kinetic inductance modulation triggered by single-photon absorption, which induces a localized hotspot and measurable voltage pulse across the biased nanowire. This physical mechanism enables sub-50 ps timing jitter, photon-number-resolving capability (under specific bias and readout configurations), and intrinsic immunity to afterpulsing—distinguishing it from semiconductor-based avalanche photodiodes (APDs) and photomultiplier tubes (PMTs).
Key Features
- Ultra-low timing jitter: ≤50 ps full-width-at-half-maximum (FWHM), enabling time-of-flight measurements with picosecond resolution
- Low dark count rate: ≤10 counts per second (cps), ensuring high signal-to-noise ratio in weak-light experiments
- High maximum count rate: ≥100 MHz, supported by a dead time ≤10 ns—critical for high-flux quantum optics and time-correlated single-photon counting (TCSPC)
- Scalable channel architecture: Configurable 1–4 independent, electrically isolated detection channels with synchronized triggering
- Fiber-coupled input: Standardized FC/PC or FC/APC connectors compatible with SMF-28 or PM fibers; no alignment required post-installation
- Flexible output signaling: TTL, ECL, and LVDS logic-compatible voltage pulses (≤150 mV amplitude), facilitating direct integration with time-tagging electronics (e.g., IDQ ID900, PicoQuant HydraHarp)
- No parasitic pulses or bias-dependent drift: Inherent stability due to uniform nanowire morphology and cryogenic thermal anchoring
- Continuous operation capability: Type 1 closed-cycle cooler supports uninterrupted measurement campaigns exceeding three months without cryogen replenishment
Sample Compatibility & Compliance
The TCOPRS-CCR-SW-25 is designed for use with standard single-mode optical fibers and integrates seamlessly into vacuum-compatible optical tables, confocal microscopes, and free-space quantum communication testbeds. It complies with IEC 61326-1:2013 (EMC requirements for laboratory equipment) and meets mechanical safety standards per IEC 61010-1:2010. While not certified under FDA 21 CFR Part 11 or ISO 17025, its deterministic digital output format, timestamped event data, and hardware-level trigger synchronization support GLP/GMP-aligned experimental workflows when deployed with validated acquisition software. The system is routinely employed in laboratories adhering to ASTM E2861–18 (Standard Guide for Characterization of Superconducting Nanowire Single-Photon Detectors) and ISO/IEC 17025:2017 traceability frameworks for photon-counting metrology.
Software & Data Management
Scontel provides the SSPD Control Suite, a Windows-based application supporting real-time monitoring of bias current, base temperature, and channel-specific count rates. Raw TTL/ECL/LVDS pulses are timestamped via external time-to-digital converters (TDCs); the system does not embed onboard data storage. All output signals conform to NIM or LVDS electrical standards, ensuring compatibility with industry-standard TCSPC platforms—including Becker & Hickl SPC-150NX, Swabian Instruments Time Tagger Ultra, and ID Quantique ID900. Audit trails, parameter logging, and configuration versioning are maintained externally via user-defined LabVIEW, Python (PyVISA), or MATLAB control scripts. No proprietary drivers are required—USB 2.0 and Ethernet interfaces support remote operation and integration into automated quantum characterization pipelines.
Applications
- Quantum key distribution (QKD) systems operating at telecom wavelengths (1310/1550 nm), where low dark counts and high timing fidelity directly determine secure key rate and transmission distance
- Time-resolved fluorescence lifetime imaging (FLIM) and single-molecule FRET, particularly in cryogenic or high-background environments
- Optical time-domain reflectometry (OTDR) with millimeter-scale spatial resolution
- Entanglement verification and Bell inequality tests requiring high-efficiency, low-jitter coincidence detection
- Calibration of primary radiometric standards and transfer standards for national metrology institutes (NMIs)
- Raman spectroscopy under ultra-low-excitation conditions, enabling vibrational mode resolution without sample damage
FAQ
What cooling options are available for the TCOPRS-CCR-SW-25?
Two configurations are offered: Type 1 uses a Gifford-McMahon closed-cycle cryocooler (no liquid helium handling required); Type 2 employs a standard 4.2 K liquid helium dewar with continuous or batch-fill operation.
Is the system compatible with polarization-maintaining fiber inputs?
Yes—custom FC/APC or FC/PC connectors with PM fiber pigtails (e.g., Panda or Bow-tie) can be factory-installed upon request.
Can multiple TCOPRS units be synchronized for multi-channel coincidence measurements?
Yes—external trigger inputs and outputs support hardware-level synchronization across up to 16 channels using common clock distribution and delay-adjustable triggers.
Does the system provide photon-number resolution?
The standard TCOPRS-CCR-SW-25 operates in binary (click/no-click) mode; photon-number-resolving capability requires optional bias-current modulation and specialized readout electronics—not included in base configuration.
What is the typical system quantum efficiency across the operational wavelength range?
Peak system detection efficiency exceeds 80% at 1550 nm and remains above 40% from 400 nm to 1310 nm, depending on fiber coupling efficiency and optical interface design.

