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arXiv:2610.42041

Benchmarking Single-Photon Sources for Measurement-Device-Independent Quantum Key Distribution

Janka Memmen, Yvonne Lasars, Tobias Heindel, Nathan Walk, Anna Pappa

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

Abstract

Measurement-Device-Independent Quantum Key Distribution (MDI-QKD) enables secure communication without trusting the measurement devices, but its performance critically depends on the quality of the employed photon sources. We compare MDI-QKD implementations based on Weak Coherent Pulses (WCPs) with those employing Quantum Dot (QD) single-photon sources. WCP-based schemes are fundamentally limited by Poissonian photon-number statistics, imposing a trade-off between single- and multi-photon emissions, whereas QD sources exhibit sub-Poissonian statistics with low antibunching parameter $g^{(2)}(0)$. Using a decoy-state analysis for both source types, we find that even at moderate mean photon numbers, QD-based implementations outperform the best-case WCP configuration - where the mean photon number is optimised at each transmission distance - across the full range of transmission distances. We further incorporate the effect of imperfect photon indistinguishability via Hong-Ou-Mandel interference visibilities into the security framework and demonstrate that both source types are highly sensitive to even small deviations from ideal indistinguishability, significantly affecting achievable key rates and maximum transmission distance.

AI Summary

The paper compares quantum-dot (QD) single-photon sources with weak coherent pulses (WCPs) for polarization-encoded MDI-QKD, asking when sub-Poissonian emission improves key rates and how imperfect photon indistinguishability affects security. It calculates asymptotic decoy-state key rates for symmetric links with identical detector and channel parameters. WCP intensities are optimized at each loss; QD emission is truncated to vacuum, one- and two-photon components, with $g^{(2)}(0)=0.02$. Under perfect indistinguishability, QD sources at nominal brightness $\mu=0.3$ outperform optimized WCPs throughout the transmission range. The crossover brightness is approximately $0.26$ at low loss, decreasing toward $0.2$ at higher loss. A Fock-state interference calculation relates measured Hong–Ou–Mandel visibility to single-photon mode overlap $\gamma$. Existing fidelity and basis-imbalance bounds then translate distinguishability into a phase-error penalty, amplified by inverse single-photon yield. Under the assumed equal pairwise fidelities, even $\gamma=0.999999$ noticeably reduces performance. At $\gamma=0.9999$ and fixed $\mu=0.3$ for both sources, positive key rates extend to approximately $21$ dB for WCPs and $25$ dB for QDs, corresponding to about $25$ km and $40$ km with the chosen efficiencies. The stated limitations include asymptotic rather than finite-size analysis, symmetric channels, identical sources, and fixed antibunching. Remote-QD indistinguishability remains an experimental challenge. Measured visibility also includes apparatus imperfections; using calibrated intrinsic indistinguishability instead would require rigorous justification within the security model.

Little sign of AI-generated textIncrementalStrong assumptionsPossible errorOverclaims

Central claim may not hold: The abstract's all-distance QD advantage is established only for a restricted ideal-indistinguishability benchmark, whereas the paper's broader analysis makes that advantage conditional on source brightness and indistinguishability. Reduced HOM interference between Alice and Bob does not alone imply within-source basis leakage, so the claimed extreme security sensitivity depends on an additional assumption about fidelities among prepared states. The stated phase-error prescription incorrectly restores the ideal privacy entropy at Delta'=1/2 unless an unstated worst-case entropy restriction is imposed. The successful-event yield omits the acceptance probability of the specified linear-optical Bell measurement, compromising the quantitative key rates and loss-dependent security correction.

Written by gpt-6.1-sol from the paper's full text. Automated: it can be wrong.

Comments
13 pages, 4 figures

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Measurement-Device-Independent Quantum Key Distribution (MDI-QKD) enables secure communication without trusting the measurement devices, but its performance critically depends on the quality of the employed photon sources. We compare MDI-QKD implementations based on Weak Coherent Pulses (WCPs) with those employing Quantum Dot (QD) single-photon sources. WCP-based schemes are fundamentally limited by Poissonian photon-number statistics, imposing a trade-off between single- and multi-photon emissions, whereas QD sources exhibit sub-Poissonian statistics with low antibunching parameter g(2)(0)g^{(2)}(0)g(2)(0). Using a decoy-state analysis for both source types, we find that even at moderate mean photon numbers, QD-based implementations outperform the best-case WCP configuration - where the mean photon number is optimised at each transmission distance - across the full range of transmission distances. We further incorporate the effect of imperfect photon indistinguishability via Hong-Ou-Mandel interference visibilities into the security framework and demonstrate that both source types are highly sensitive to even small deviations from ideal indistinguishability, significantly affecting achievable key rates and maximum transmission distance.
The paper compares quantum-dot (QD) single-photon sources with weak coherent pulses (WCPs) for polarization-encoded MDI-QKD, asking when sub-Poissonian emission improves key rates and how imperfect photon indistinguishability affects security.
It calculates asymptotic decoy-state key rates for symmetric links with identical detector and channel parameters. WCP intensities are optimized at each loss; QD emission is truncated to vacuum, one- and two-photon components, with g(2)(0)=0.02g^{(2)}(0)=0.02g(2)(0)=0.02. Under perfect indistinguishability, QD sources at nominal brightness μ=0.3\mu=0.3μ=0.3 outperform optimized WCPs throughout the transmission range. The crossover brightness is approximately 0.260.260.26 at low loss, decreasing toward 0.20.20.2 at higher loss.
A Fock-state interference calculation relates measured Hong–Ou–Mandel visibility to single-photon mode overlap γ\gammaγ. Existing fidelity and basis-imbalance bounds then translate distinguishability into a phase-error penalty, amplified by inverse single-photon yield. Under the assumed equal pairwise fidelities, even γ=0.999999\gamma=0.999999γ=0.999999 noticeably reduces performance. At γ=0.9999\gamma=0.9999γ=0.9999 and fixed μ=0.3\mu=0.3μ=0.3 for both sources, positive key rates extend to approximately 212121 dB for WCPs and 252525 dB for QDs, corresponding to about 252525 km and 404040 km with the chosen efficiencies.
The stated limitations include asymptotic rather than finite-size analysis, symmetric channels, identical sources, and fixed antibunching. Remote-QD indistinguishability remains an experimental challenge. Measured visibility also includes apparatus imperfections; using calibrated intrinsic indistinguishability instead would require rigorous justification within the security model.
The ideal measurement-device-independent quantum key distribution (MDI-QKD), which is immune to all detector side-channel attacks, is built on the Bell state measurement of two single-photon states. However, in practical MDI-QKD where phase-randomized weak coherent pulses (PR-WCPs) are used, the mismatch between states preparation and measurement in X basis leads to the bit error rate of more than 25%, which poses a challenge to the security of QKD. In this paper, we provide a security analysis of practical MDI-QKD based on polarization coding. We analyze the Hong-Ou-Mandel interference of PR-WCPs and Poisson-distributed photon number states (PNs), and find that these two sources are equivalent in MDI-QKD. The security analysis based on entanglement distillation is carried out on PNs, and the measurement results in Z basis and X basis are averaged to overcome the noncorrelation of the error rates in these two bases. Compared with GLLP scheme, a tighter key rate is obtained in this work, and the key rate deviates from the linear key rate bound in a short distance due to the finite proportion of multiphoton terms.
Quantum cryptography has a strong security that classical cryptography cannot match, and quantum key distribution (QKD) is the most important method of quantum cryptography. Reference-frame-independent measurement-device-independent QKD (RFI-MDI-QKD) protocol can avoid the drift of the reference frame and all side channels of measurement devices. However, RFI MDI-QKD usually employs a weak coherent state (WCS) as the light source, which limits the transmission distance of secure keys. Here, by using heralded single-photon sources, we investigate an improved decoy-state RFI-MDI-QKD scheme. We perform numerical simulations for the scheme under different scenarios, such as considering the finite size and different drift angles. Compared with the scheme with WCS, our scheme can significantly improve the transmission distance of RFI-MDI-QKD.
The measurement-device-independent quantum key distribution (MDI-QKD) protocol has been proposed for the purpose of removing the detector side channel attacks. Due to the multiphoton events of coherent states sources, real-life implementations of MDI-QKD protocol must employ decoy states to beat the photon-number-splitting attack. Decoy states for MDI-QKD based on the weak coherent states (WCSs) have been studied recently. In this Letter, we propose to perform MDI-QKD protocol with modified coherent states (MCS) sources. We simulate the performance of MDI-QKD with the decoy states based on MCS sources. And our simulation indicates that both the secure-key rate and transmission distance can be improved evidently with MCS sources. The physics behind this improvement is that the probability of multiphoton events of the MCS is lower than that of WCSs while at the same time the probability of single-photon is higher.
Global quantum secure communication can be achieved using quantum key distribution (QKD) with orbiting satellites. Established techniques use attenuated lasers as weak coherent pulse (WCP) sources, with so-called decoy-state protocols, to generate the required single-photon-level pulses. While such approaches are elegant, they come at the expense of attainable final key due to inherent multi-photon emission, thereby constraining secure key generation over the high-loss, noisy channels expected for satellite transmissions. In this work we improve on this limitation by using true single-photon pulses generated from a semiconductor quantum dot (QD) embedded in a nanowire, possessing low multi-photon emission (<10−6<10^{-6}<10−6) and an extraction system efficiency of -15 dB (or 3.1%). Despite the limited efficiency, the key generated by the QD source is greater than that generated by a WCP source under identical repetition rate and link conditions representative of a satellite pass. We predict that with realistic improvements of the QD extraction efficiency to -4.0 dB (or 40%), the quantum-dot QKD protocol outperforms WCP-decoy-state QKD by almost an order of magnitude. Consequently, a QD source could allow generation of a secure key in conditions where a WCP source would simply fail, such as in the case of high channel losses. Our demonstration is the first specific use case that shows a clear benefit for QD-based single-photon sources in secure quantum communication, and has the potential to enhance the viability and efficiency of satellite-based QKD networks.
Measurement-device-independent quantum key distribution (MDI-QKD) is proposed to close the loopholes of the detection part in QKD systems, while it still requires the light source to be trusted. This assumption is not guaranteed in practice, leading to practical secure issues. In this paper, we propose a light source monitoring scheme with single-photon detectors for MDI-QKD, which can guarantee the security of the system under the untrusted source condition with both common decoy state method and the newly proposed five-intensity decoy state method. Moreover, our monitoring scheme performs almost the same as the ideal MDI protocol even considering the imperfect factors in practical systems. Compared to the previous scheme, our work improves the secure key rate and the transmission distance of practical MDI-QKD systems significantly.
A measurement-device-independent quantum key distribution (MDI-QKD) protocol is immune to all detection side-channel attacks and guarantees the information-theoretical security even with uncharacterized single photon detectors. A weak coherent source is used in the current MDI-QKD experiments, it inevitably contains a certain percentage of vacuum and multi-photon pulses. The security issues introduced by these source imperfections can be avoided by applying the decoy state method. Here, through modeling experimental devices, and taking into account the weak coherent source and the threshold detectors, we have evaluated the gain, the probability to get successful Bell measurement and incorrect Bell measurement, and the quantum bit error rate (QBER), given a practical setup. In our simulation, we show how QBER varies with different transmission distances in the cases when the average photon numbers per pulse from Alice and Bob are symmetric and asymmetric. Result shows that the multi-photon pulses do not cause error in the Z basis of polarization encoding scheme, but produce a large QBER in phase encoding scheme and in the X basis of polarization encoding scheme. QBER is affected by the dark count rate and the system optical error associated with the multi-photon pulses. For different encoding schemes, QBER caused by each kind of average photon numbers from Alice and Bob increases to different degrees with the transmission distance, and finally is close to 50%. With the increase of the transmission distance, the average photon number per pulse decreases and the fraction of the dark count rate causing QBER gradually increases. Under the same effect of the dark count rate, the smaller the average photon number per pulse, the bigger the QBER. After a certain transmission and at the same transmission distance, the QBER is largest when average photon numbers used by Alice and Bob are both smallest. For the short distance transmission of phase encoding scheme and the X basis, we find that QBER is larger when average photon numbers from the two arms are asymmetric, as compared to the symmetric case. For the Z basis, the QBER caused by the system optical error and the dark count rate is very small.