• Infrared single-photon detector
Infrared single-photon detector
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Infrared single-photon detector


Single-photon detectors are instruments for detecting weak signals at the single-photon level, playing an indispensable role in numerous fields such as quantum optics, biophotonics, and laser ranging. In recent years, single-photon detectors have been widely used in the field of quantum cryptography and have become the core device for photoelectric conversion of quantum signals.

Keywords:

Infrared single-photon detector

Product Overview

Single-photon detectors are instruments used for detecting weak signals at the single-photon level, playing an indispensable role in numerous fields such as quantum optics, biophotonics, and laser ranging. In recent years, single-photon detectors have been widely applied in the field of quantum cryptography and have become the core device for photoelectric conversion of quantum signals.

The WT-SPD series infrared single-photon detectors are low-cost, low-dark-count-rate, and highly stable optoelectronic instruments developed on the basis of research into quantum cryptographic communication systems. The device employs an InGaAs/InP single-photon avalanche diode as its photosensitive element. In addition to adopting a range of internationally recognized noise-reduction and afterpulse-suppression techniques—including gated operation and dead-time suppression—it also incorporates an original differential filtering scheme. This innovative approach not only maintains high detection efficiency but further reduces the dark count rate.

Product Parameters

● Dark count rate

The products are categorized into three models based on their dark count rates: Ultra-Low Noise (ULN), Low Noise (LN), and Standard (STD). The dark count rate requirements for each model under gate widths of 1 ns, 2 ns, and 3 ns are shown in the table below.

Product Model Effective door width 10% 15% 20% 25%
WT-SPD300-ULN 1ns <2.00×10 -6 <4.00×10 -6 <8.00×10 -6 <2.00×10 -5
2ns <5.00×10 -6 <1.00×10 -5 <2.00×10 -5 <5.00×10 -5
3ns <1.50×10 -5 <3.00×10 -5 <6.00×10 -5 <1.50×10 -4
WT-SPD300-LN 1ns <5.00×10 -6 <1.00×10 -5 <2.00×10 -5 <5.00×10 -5
2ns <1.25×10 -5 <2.50×10 -5 <5.00×10 -5 <1.25×10 -4
3ns <3.75×10 -5 <7.50×10 -5 <1.50×10 -4 <3.75×10 -4
WT-SPD300-STD 1ns <1.00×10 -5 <2.00×10 -5 <4.00×10 -5 <1.00×10 -4
2ns <2.50×10 -5 <5.00×10 -5 <1.00×10 -4 <2.50×10 -4
3ns <7.50×10 -5 <1.50×10 -4 <3.00×10 -4 <7.50×10 -4

● Detection efficiency

The detection efficiency is set in four levels: 10%, 15%, 20%, and 25%. The deviations between the actual detection efficiencies and the nominal values under different detector gate widths and operating temperatures are shown in the table below.

Effective door width Nominal efficiency ( % ) Actual Efficiency ( % )
1ns 20 20 ± 2
1ns 25 25 ± 3
2ns 10 10 ± 2
2ns 15 15 ± 3
2ns 20 20 ± 5
2ns 25 25 ± 5
3ns 10 10 ± 3
3ns 15 15 ± 4
3ns 20 20 ± 7
3ns 25 25 ± 9

● Effective door width

Door width (ns) Detection efficiency (%) Effective door width range (ns)
1 10% 0.1–0.4
20% 0.2 to 0.6
2 10% 0.3–1.0
20% 0.6–1.2
3 10% 0.8–2.1
20% 1.0–2.5

● Post-pulse rate

The post-pulse rate is less than or equal to 3% (@100 MHz detector trigger frequency, 10 MHz laser trigger frequency, optical pulse duration of 50 ps, 0.1 photon per pulse, 1 ns detection gate width, 10% detection efficiency, and a dead time greater than or equal to 100 ns).

Scope of application

● Quantum Cryptographic Communication

● Quantum optics, biophotonics

● Laser rangefinding

● Atmospheric and water environment monitoring

● Fluorescence Lifetime and Fluorescence Spectroscopy

● Time-resolved single-molecule spectroscopy

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Contact Us

Landline: +86-551-63637001
Tel: +86-13514953141
Address: No. 2800, Innovation Avenue, High-Tech Zone, Hefei City, Anhui Province, Innovation Industrial Park Phase II, E2-901/902

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