Koon Tong Goh

Device-independent quantum key distribution (DIQKD) is the art of using untrusted devices to distribute secret keys in an unsecure network. It thus represents the ultimate form of cryptography, offering not only information-theoretic security against channel attacks, but also against attacks exploiting implementation loopholes~\cite{lydersen2010hacking}. At its heart, DIQKD utilises nonlocal correlations---detected and certified by a Bell inequality---to establish secret correlations between the users. In recent years, much progress has been made towards realising the first DIQKD experiments, but current proposals are just out of reach of today’s loophole-free Bell experiments. Here, in this work, we close the gap between the theory and practice of DIQKD with a simple variant of the original protocol based on the celebrated Clauser-Horne-Shimony-Holt (CHSH) Bell inequality. In using two randomly chosen key generating bases instead of one, we show that the noise tolerance of DIQKD can be significantly improved. In particular, the extended feasibility region now covers some of the most recent loophole-free CHSH experiments, hence indicating that the first realisation of DIQKD already lies within the range of these experiments.

Measurement-device-independent quantum key distribution (MDI-QKD) is the only known QKD scheme that can completely overcome the problem of detection side-channel attacks. Yet, despite its practical importance, there is no standard approach towards proving the security of MDI-QKD. Here, we present a simple numerical method that can efficiently compute almost-tight security bounds for any discretely modulated MDI-QKD protocol. To demonstrate the broad utility of our method, we use it to analyze the security of coherent-state MDI-QKD, decoy-state MDI-QKD with leaky sources, and a variant of twin-field QKD called phase-matching QKD. In all of the numerical simulations (using realistic detection models) we find that our method gives significantly higher secret key rates than those obtained with current security proof techniques. Interestingly, we also find that phase-matching QKD using only two coherent test states is enough to overcome the fundamental rate-distance limit of QKD. Taken together, these findings suggest that our security proof method enables a versatile, fast, and possibly optimal approach towards the security validation of practical MDI-QKD systems.

In this QCRYPT submission, we present a numerical toolbox that is capable of producing non-trivial lower bounds on the asymptotic secret key rate of any device-independent quantum key distribution (DIQKD) protocol. The main mechanism of our toolbox is a new method for estimating the entropy production of a quantum channel, giving rise to bounds that can be computed using the family of semidefinite programs (SDPs) known as the Navascues-Pironio-Acin (NPA) hierarchy.

The power of quantum random number generation is more than just the ability to create truly random numbers. It can also enable self-testing, which allows the user to verify the implementation integrity of critical quantum components with minimal assumptions. In this work, we develop and implement a self-testing quantum random number generator (QRNG) chipset capable of generating 15.33 Mbits of certifiable randomness in each run, producing an expansion rate of 5.11×10-4 at a repetition rate of 10 MHz. The chip design is based on a highly loss-and-noise tolerant measurement-device-independent protocol, where random coherent states encoded using quadrature phase shift keying (QPSK) are used to self-test the quantum homodyne detection unit, well-known to be challenging to characterise in practice. Importantly, this proposal opens up the possibility to implement miniaturised self-testing QRNG devices at production scale using standard silicon photonics foundry platforms.

By making reasonable assumptions on realistic systems, we propose and implement the first ultra-high-speed CHSH experiment working at 40GHz demonstrating a gigabit quantum certified random number throughput. Moreover, our scheme is suitable for optical chip design since it only requires standard optical components and balanced detectors. Furthermore, our scheme paves the way for the promising research direction to utilise noisy detectors for quantum system construction, which might be helpful for certain noise-sensitive applications, e.g. quantum sensing and quantum computing.