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Superconducting nanowire single-photon detectors are optical and near-infrared single-photon detectors that are based on a current-biased superconducting nanowire.
The nanowire is biased with a DC current that is close to but less than its superconducting critical current, and it is cooled to a temperature well below its superconducting critical temperature. Cooper pairs are broken and the local critical current is lowered below the bias current by a photon incident on the nanowire.
A nanowire is a nanostructure that takes the shape of a wire and has a diameter of about one nanometer. More broadly, structures with a thickness or diameter restricted to tens of nanometers or less and an uncontrolled length are referred to as nanowires.
The Global Superconducting Nanowire Market accounted for $XX Billion in 2022 and is anticipated to reach $XX Billion by 2030, registering a CAGR of XX% from 2023 to 2030.
ID Quantique launches a new family of ID281 SNSPDs. The ID281 Series of superconducting nanowire single-photon detectors (SNSPDs) is heating up, with the best in single-photon detection getting even better. The ID281 Series has just received upgrades that make it possible to view individual photons faster and with even more accuracy than before, getting us closer to the very fabric of reality.
The laboratory will also become more efficient because the new detectors only need basic cryogenic equipment to function, allowing for the first time ever real 24/7 continuous operation at a cheaper cost.
The purpose of IDQ is to facilitate work in developing photonic and quantum applications. People all around the world are already learning how SNSPDs are enabling the impossible and advancing the development of the quantum internet. Aided by the spectrum of ID281 SNSPDs that are currently available, which have previously demonstrated nearly flawless detection efficiency, timing precision, ultra-low noise, and quick recovery times.
The new-recipe ID281 SNSPDs have significantly reduced timing jitter (uncertainty in detection pulse arrival time, as low as 25 ps FWHM) and recovery time (time for detection efficiency to reach 50% of its peak after a detection event, typ. 30 ns).