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arXiv:2610.41709

A Highly Nondegenerate Photon-Pair Source for Detector-Matched Quantum Key Distribution

Sander van Haagen, Bora Ulu, Alper Ozulker, Wardah Mahmood, Michal Krelina, Utku Tefek, Kadir Durak

quant-phSubmitted Oct 30, 2026• Announced Nov 2, 2026
arXivHTMLPDF

Abstract

In a commercial entanglement-distribution system over telecom fibre, the single-photon detectors are the largest part of the hardware cost. In entanglement-based quantum key distribution (QKD), both photons of each pair must be detected. With two telecom photons, each arm needs either an InGaAs single-photon avalanche diode (SPAD) of low efficiency or a superconducting nanowire single-photon detector (SNSPD) with its own cryostat. We study a highly nondegenerate photon-pair source that needs a telecom detector on one arm only. Two periodically poled KTiOPO$_4$ (ppKTP) crystals pumped at 405~nm emit pairs at 548 and 1550~nm. A Si-SPAD with 82\% efficiency detects the 548~nm photon at the source node, and only the 1550~nm photon travels through fibre. A first, unoptimised module in a polarisation-correlated configuration generates about $1.5\times10^6$ pairs/s per mW of pump power. It collects 13\% of the pairs on the 548~nm arm and 23\% on the 1550~nm arm. In an asymptotic BBM92 model, we compare its links with generic $2\times1550$~nm links that use a bright published source at the same pump power. At 50~km, our link with one SNSPD costs about 25\% more per secret bit than the generic link with one SNSPD. With optimistic target values of 52\% collection and twice the brightness, it costs about 40\% as much as the generic link with two SNSPDs. Our link without a cryostat then costs about 70\% less than the generic link with one SNSPD. If every link runs at its own best pump power, the two-SNSPD link is again the cheapest. The source can also serve clock synchronisation and detector calibration, which need only time-correlated pairs. All key rates assume the entangled configuration of the source, which is under development.

AI Summary

The paper asks whether highly nondegenerate photon pairs can reduce detector costs in fibre-based entanglement QKD by keeping a visible photon local and transmitting only its telecom partner. It characterises a compact, 405-nm-pumped, crossed-ppKTP source emitting at 548 and 1550 nm. Singles and coincidence measurements give an inferred generation rate of approximately $1.5\times10^6$ pairs/s/mW; dead-time-corrected heralding efficiencies, divided by detector efficiencies, imply collection efficiencies of 13.5% and 23.0%, respectively. An asymptotic BBM92 rate model includes detector dead time, afterpulsing and accidental coincidences, and compares Si-SPAD/telecom-detector links with published-source-based $2\times1550$-nm configurations. At 50 km and equal 14.5-mW pump power, the measured-source parameters predict about 11 kbit/s with one SNSPD, costing $376/Gbit over two years versus $301/Gbit for the generic one-SNSPD link. A target source with 52% collection on both arms, twice the brightness and improved loop transmission predicts 150 kbit/s and $27/Gbit, versus $66/Gbit for two SNSPDs. Optimising each link’s pump power instead makes the two-SNSPD comparator cheapest, at $15/Gbit versus $23/Gbit for the target source. Crucially, the measured configuration is expected to be separable and cannot generate BBM92 key: all key rates assume an entangled Sagnac configuration still under development. Other stated limitations include unverified simultaneous brightness and collection targets, residual afterpulsing, approximate component prices, omitted finite-key effects and fibre dispersion, assumed polarisation compensation, and count-rate-dependent timing jitter. The main rate comparisons also omit a dead-time-attack countermeasure whose estimated penalties are reported separately.

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In a commercial entanglement-distribution system over telecom fibre, the single-photon detectors are the largest part of the hardware cost. In entanglement-based quantum key distribution (QKD), both photons of each pair must be detected. With two telecom photons, each arm needs either an InGaAs single-photon avalanche diode (SPAD) of low efficiency or a superconducting nanowire single-photon detector (SNSPD) with its own cryostat. We study a highly nondegenerate photon-pair source that needs a telecom detector on one arm only. Two periodically poled KTiOPO4_44​ (ppKTP) crystals pumped at 405nm emit pairs at 548 and 1550nm. A Si-SPAD with 82% efficiency detects the 548nm photon at the source node, and only the 1550nm photon travels through fibre. A first, unoptimised module in a polarisation-correlated configuration generates about 1.5×1061.5\times10^61.5×106 pairs/s per mW of pump power. It collects 13% of the pairs on the 548nm arm and 23% on the 1550nm arm. In an asymptotic BBM92 model, we compare its links with generic 2×15502\times15502×1550nm links that use a bright published source at the same pump power. At 50km, our link with one SNSPD costs about 25% more per secret bit than the generic link with one SNSPD. With optimistic target values of 52% collection and twice the brightness, it costs about 40% as much as the generic link with two SNSPDs. Our link without a cryostat then costs about 70% less than the generic link with one SNSPD. If every link runs at its own best pump power, the two-SNSPD link is again the cheapest. The source can also serve clock synchronisation and detector calibration, which need only time-correlated pairs. All key rates assume the entangled configuration of the source, which is under development.
The paper asks whether highly nondegenerate photon pairs can reduce detector costs in fibre-based entanglement QKD by keeping a visible photon local and transmitting only its telecom partner. It characterises a compact, 405-nm-pumped, crossed-ppKTP source emitting at 548 and 1550 nm. Singles and coincidence measurements give an inferred generation rate of approximately 1.5×1061.5\times10^61.5×106 pairs/s/mW; dead-time-corrected heralding efficiencies, divided by detector efficiencies, imply collection efficiencies of 13.5% and 23.0%, respectively.
An asymptotic BBM92 rate model includes detector dead time, afterpulsing and accidental coincidences, and compares Si-SPAD/telecom-detector links with published-source-based 2×15502\times15502×1550-nm configurations. At 50 km and equal 14.5-mW pump power, the measured-source parameters predict about 11 kbit/s with one SNSPD, costing 376/Gbitovertwoyearsversus376/Gbit over two years versus 376/Gbitovertwoyearsversus301/Gbit for the generic one-SNSPD link. A target source with 52% collection on both arms, twice the brightness and improved loop transmission predicts 150 kbit/s and 27/Gbit,versus27/Gbit, versus 27/Gbit,versus66/Gbit for two SNSPDs. Optimising each link’s pump power instead makes the two-SNSPD comparator cheapest, at 15/Gbitversus15/Gbit versus 15/Gbitversus23/Gbit for the target source.
Crucially, the measured configuration is expected to be separable and cannot generate BBM92 key: all key rates assume an entangled Sagnac configuration still under development. Other stated limitations include unverified simultaneous brightness and collection targets, residual afterpulsing, approximate component prices, omitted finite-key effects and fibre dispersion, assumed polarisation compensation, and count-rate-dependent timing jitter. The main rate comparisons also omit a dead-time-attack countermeasure whose estimated penalties are reported separately.
Entangled photon sources (EPSs) are essential building blocks for scalable quantum communication and quantum key distribution (QKD). We present a stable, highly nondegenerate EPS based on type-0 spontaneous parametric down-conversion (SPDC) in a crossed-crystal configuration, generating photon pairs at 680~nm and 1550~nm when pumped by a 473~nm laser. This wavelength combination, reported here for the first time, simultaneously benefits from the peak detection efficiency of the most of the Si-SPADs in the visible/near-infrared spectral range and the low-loss fiber transmission of the telecom C-band. This configuration provides the most favorable balance between performance and cost for detection using Si-SPADs and InGaAs detectors. The source exhibits a measured spectral bandwidth of 300~GHz, corresponding to a spectral brightness of up to 1.9×1031.9\times 10^31.9×103~pairs~s−1^{-1}−1~mW−1^{-1}−1~GHz−1^{-1}−1. Heralding efficiencies reach 18~\% (signal) and 34~\% (idler) with Si-SPAD and superconducting nanowire single-photon detectors (SNSPD) detection. The entangled state achieves visibilities of (97.3±1.0) %(97.3\pm 1.0)\,\%(97.3±1.0)% in the H/V basis and (94.9±1.6) %(94.9\pm1.6)\,\%(94.9±1.6)% in the D/A basis, yielding a fidelity of ≥(96.1±1.3) %\geq(96.1\pm1.3)\,\%≥(96.1±1.3)%. These results establish the presented EPS as a practical wavelength-hybrid platform for fiber-based QKD and emerging long-haul quantum network architectures.
We present experimental results from a Quantum Key Distribution (QKD) setup based on entanglement, where polarization entangled photon pairs are distributed after narrowband filtering and followed by detection employing polarization-based receivers. A comparative analysis of the performance of InGaAs single photon avalanche detectors (SPADs) and superconducting nanowire single photon detectors (SNSPDs), reveals a notable advantage of SNSPDs for QKD applications. The entangled photon pairs are generated using a Sagnac-based polarization entanglement source, and subsequently split by Dense Wavelength Division Multiplexers (DWDMs). These entangled photon pairs are sent to two polarization-based receivers facilitating the comparison between the detection using InGaAs SPADs and SNSPDs. The results emphasize the superior performance of SNSPDs reflected in an around 80 times higher coincidence rate, therefore tolerating around 8 dB higher attenuation values. For both configurations and all considered attenuation levels, the fidelity and quantum bit error rate (QBER) are well inside the respective bounds for secure key generation. This work provides valuable insights for the optimization of QKD systems.
Quantum cryptography with entangled photon pairs can be more powerful than protocols based onsingle photons or weak coherent pulses: they can tolerate higher losses and thus allow thedistribution of quantum secret keys (QKD) over longer distances [1], they also provide a waytowards device-independent quantum cryptography [2]. However, in order to enable a wide use ofentangled photon pairs in future quantum telecommunication systems, further developments areneeded to demonstrate performant sources that can be easily fabricated and integrated into Telecomfiber networks.Here we present a source consisting of an aluminium gallium arsenide waveguide generatingphoton pairs in the Telecom band by type II spontaneous parametric down-conversion [3]. Such adevice has already been proven to work under electrical pumping [4]. Thanks to the very smallbirefringence of the guided modes, the pairs are directly generated in a polarization-entangled Bellstate, without the need for any post-compensation. Moreover, as the photons are emitted over alarge bandwidth (about 100 nm) with a joint spectrum that exhibits frequency anticorrelation, thesame source can be used to simultaneously distribute keys among multiple pairs of users by usingstandard Telecom wavelength demultiplexers [5]. Here, we experimentally show the distribution ofquantum secret keys with the BBM92 QKD protocol [6] between four different pairs of users with acommercial 100 GHz demultiplexer (0.8 nm channel width and spacing). Under CW pumpingconditions, using free-running InGaAs single-photon detectors, we achieve a secret key rate of 0.21bits/s and a qubit error rate (QBER) of 6.9% over 50 km of standard optical fiber.Our results, obtained with a robust and simple experimental set-up, open the way towards theimplementation of practical device-independent quantum communication protocols.
Two approaches to single-photon detection at telecom wavelengths have been investigated, using semiconductor and superconductor technologies. The low temperature operation of free-running InGaAs/InP negative feedback avalanche diodes (NFADs) was studied, demonstrating that they can operate with an extremely low dark count rate, which opens up a host of new applications. Secondly, superconducting nanowire single-photon detectors (SNSPDs) based on amorphous materials were developed, fabricated and characterized. These detectors are highly attractive because they can achieve excellent attributes simultaneously, such as high efficiency, low noise, good temporal resolution, no afterpulsing and high count rates. Finally, it was demonstrated that the use of NFADs can enable record distance quantum key distribution (QKD) over 307 km of optical fiber. A next generation QKD system has been proposed and numerically analyzed, aiming at extending the record distance by an additional 100 km and increasing the state-of-the-art secret key rate by over an order of magnitude.
In any quantum communication system, such as a quantum key distribution (QKD) system, data rates are mainly limited by the system clock rate and the various link losses. While the transmission clock rate is limited by the temporal resolution of the single-photon detectors, losses in a fiber-based quantum communication system can be minimized by operating in the near infrared range (NIR), at 1310 nm or 1550 nm. Commercially available InGaAs-based avalanche photo-diodes (APDs) can be operated as single-photon detectors in this wavelength range [Hadfield, 2009]. Due to the severe after-pulsing, InGaAs APDs are typically used in a gated mode and this can limit their application in high-speed quantum communications systems. Superconducting single-photon detectors (SSPDs) can work in the NIR wavelength range with good performance [Gol’tsman et al. 2001; Hadfield, 2009]. However, SSPDs require cryogenic temperatures, and are not widely available on the commercial market at present. In addition, InGaAs/InP based photomultiplier tubes (PMT) can operate in the NIR range, but its performance is limited by very low detection efficiency (1 % at 1600 nm) and large timing jitter (1.5 ns) [Hamamatsu, 2005]. Microchannel plates (MCP) are micro-capillary electron multipliers coated with an electron-emissive material and multiply photon-excited electrons from a photon cathode [Wiza, 1979]. MCPs usually have faster rise times and lower timing jitter than is achievable with PMTs. InGaAs MCPs can work in the NIR range. These MCPs, but are limited by low detection efficiency (~1 %) [Martin, J. & Hink P. 2003]. On the other hand, silicon based avalanche photo-diodes (Si APDs) are compact, relatively inexpensive, and can be operated at ambient temperatures with high detection efficiency and low noise in the visible or near-visible range. Unfortunately they do not work at wavelengths longer than 1000 nm. For those wavelengths, an up-conversion technique has been developed that uses sum-frequency generation (SFG) in a non-linear optical medium to convert the signal photons to a higher frequency (shorter wavelength) in the visible or near visible range. The up-converted photons can then be detected by a Si APD. Up-conversion detectors use commercially available components and devices, and are a practical solution for many applications in quantum communications. To date, several groups have successfully developed highly efficient up-conversion single-photon detectors in the nearinfrared range using periodically poled lithium niobate (PPLN) waveguides [Diamanti et al., 2005; Langrock et al., 2005; Thew et al., 2006; Tanzilli et al., 2005; Xu et al., 2007;] and bulk crystals [Vandevender & Kwiat, 2004].
Distributing entanglement through standard telecommunication fiber is particularly important for quantum key distribution protocols with low vulnerability over metropolitan distances. However, entanglement distribution over long distance through optical fiber so far could only be accomplished with moderate photon pair rates. In this work, we present entanglement distribution over 50 km of standard telecommunication fiber with a pair rate of more than 10 000 ${\mathrm{s}}^{\ensuremath{-}1}$ using a bright nondegenerate photon pair source. Signal and idler wavelengths of this source are optimized for low dispersion in optical fiber and high efficiency for single-photon avalanche diode detectors, respectively. The resulting modest hardware requirement and high rate of detected entangled photon pairs could significantly enhance practical entanglement-based quantum key distribution in existing metropolitan fiber networks.