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Computers, materials & continua/Computers, materials & continua (Print)

Device-Independent Quantum Key Distribution Protocol Based on Hyper-Entanglement

Yan Chang, Shibin Zhang, Lili Yan, Xue-Yang Li, Tian Cao, Qirun Wang

Published Jan 1, 2020• 4 citations
Publisher

Abstract

The secure key rate of quantum key distribution (QKD) is greatly reduced because of the untrusted devices. In this paper, to raise the secure key rate of QKD, a device-independent quantum key distribution (DIQKD) protocol... | Find, read and cite all the research you need on Tech Science Press
DOI
10.32604/cmc.2020.010042

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Quantum mechanics and its underlying principles assures better security then classical world which are unable to provide unconditional security. A quantum entanglement phenomenon helps us to minimize the required assumptions needs to be made about devices, resulting towards Device Independent Quantum Key Distribution (DIQKD). What about guarantying security of the QKD protocol in case of quantum devices used in protocol are untrusted? DIQKD provides unconditional security without assuming anything about internal working of quantum devices. DIQKD allows users to not focus on integrity of devices being used in protocol. Quantum physical phenomena non-local correlations and no information exchange within and between the laboratories of Alice and Bob are bases of DIQKD. As quantum computing started becoming mature and commercially viable, need for quantum error correction became obvious. Quantum error correction can be accommodated in quantum key distribution to gain better efficiency with reference to error rate. Post processing quantum error correcting techniques can remove noise once the procedure is performed. Real time quantum error correction will lead towards large scale quantum computation.
Quantum key distribution (QKD) is a method to distribute secret key among sender and receiver by the transmission of quantum particles (e.g. photons). Device-independent quantum key distribution (DIQKD) is a version of quantum key distribution with a stronger security demand in that sender and receiver do not need to rely on the inner workings of their device, which consequently can come from an untrusted vendor. We study the rate at which DIQKD can be carried out for a given quantum channel connecting sender and receiver and provide a technique to upper bound the achievable rate. As a result, we show that the rate of device independent secure key can for some channels be much smaller (even arbitrarily so) than that of QKD. We do so, by first providing definition of device independent secure key rate, which is of independent interest. For bipartite states we formulate a sufficient condition for a gap between QKD and DIQKD key rates and examples of 8-qubit bipartite state exhibiting the gap between device dependent and device independent key.
Quantum key distribution (QKD) is a provably secure way for two distant parties to establish a common secret key, which then can be used in a classical cryptographic scheme. Using quantum entanglement, one can reduce the necessary assumptions that the parties have to make about their devices, giving rise to device-independent QKD (DIQKD). However, in all existing protocols to date the parties need to have an initial (at least partially) random seed as a resource. In this work, we show that this requirement can be dropped. Using recent advances in the fields of randomness amplification and randomness expansion, we demonstrate that it is sufficient for the message the parties want to communicate to be (partially) unknown to the adversaries---an assumption without which any type of cryptography would be pointless to begin with. One party can use her secret message to locally generate a secret sequence of bits, which can then be openly used by herself and the other party in a DIQKD protocol. Hence our work reduces the requirements needed to perform secure DIQKD and establish safe communication.
Quantum key distribution (QKD) is a method that distributes a secret key to a sender and a receiver by the transmission of quantum particles (e.g., photons). Device-independent quantum key distribution (DIQKD) is a version of QKD with a stronger notion of security, in that the sender and receiver base their protocol only on the statistics of input and outputs of their devices as inspired by Bell's theorem. We study the rate at which DIQKD can be carried out for a given bipartite quantum state distributed between the sender and receiver or a quantum channel connecting them. We provide upper bounds on the achievable rate going beyond upper bounds possible for QKD. In particular, we construct states and channels where the QKD rate is significant while the DIQKD rate is negligible. This gap is illustrated for a practical case arising when using standard postprocessing techniques for entangled two-qubit states.
Abstract Device-independent quantum key distribution (DIQKD) is the art of using untrusted devices to distribute secret keys in an insecure 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. 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, we significantly narrow 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. By using two randomly chosen key generating bases instead of one, we show that our protocol significantly improves over the original DIQKD protocol, enabling positive keys in the high noise regime for the first time. We also compute the finite-key security of the protocol for general attacks, showing that approximately 10 8 –10 10 measurement rounds are needed to achieve positive rates using state-of-the-art experimental parameters. Our proposed DIQKD protocol thus represents a highly promising path towards the first realisation of DIQKD in practice.
Quantum cryptography is based on the discovery that the laws of quantum mechanics allow levels of security that are impossible to replicate in a classical world [2, 8, 12]. Can such levels of security be guaranteed even when the quantum devices on which the protocol relies are untrusted? This fundamental question in quantum cryptography dates back to the early nineties when the challenge of achieving device independent quantum key distribution, or DIQKD, was first formulated [9]. We answer this challenge affirmatively by exhibiting a robust protocol for DIQKD and rigorously proving its security. The protocol achieves a linear key rate while tolerating a constant noise rate in the devices. The security proof assumes only that the devices can be modeled by the laws of quantum mechanics and are spatially isolated from each other and any adversary's laboratory. In particular, we emphasize that the devices may have quantum memory. All previous proofs of security relied either on the use of many independent pairs of devices [6, 4, 7], or on the absence of noise [10, 1].