Boosting the secret key rate in a shared quantum and classical fibre communication system
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https://doi.org/10.1038/s42005-019-0238-1
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Boosting the secret key rate in a shared quantum
and classical fibre communication system
Davide Bacco 1,6*, Beatrice Da Lio1,6*, Daniele Cozzolino 1, Francesco Da Ros1, Xueshi Guo2,
Yunhong Ding 1, Yusuke Sasaki3, Kazuhiko Aikawa3, Shigehito Miki4, Hirotaka Terai 4, Taro Yamashita5,
Jonas S. Neergaard-Nielsen 2, Michael Galili1, Karsten Rottwitt1, Ulrik L. Andersen2, Toshio Morioka1 &
Leif K. Oxenløwe 1
During the last 20 years, the advance of communication technologies has generated multiple
exciting applications. However, classical cryptography, commonly adopted to secure current
communication systems, can be jeopardised by the advent of quantum computers. Quantum
key distribution (QKD) is a promising technology aiming to solve such a security problem.
Unfortunately, current implementations of QKD systems show relatively low key rates,
demand low channel noise and use ad hoc devices. In this work, we picture how to overcome
the rate limitation by using a 37-core fibre to generate 2.86 Mbit s−1 per core that can be
space multiplexed into the highest secret key rate of 105.7 Mbit s−1 to date. We also
demonstrate, with off-the-shelf equipment, the robustness of the system by co-propagating a
classical signal at 370 Gbit s1 , paving the way for a shared quantum and classical communication network.
1 CoE SPOC, Dep. Photonics Eng., Technical University of Denmark, Kgs. Lyngby 2800, Denmark. 2 CoE bigQ, Dep. of Physics, Technical University of
Denmark, Kgs. Lyngby 2800, Denmark. 3 Advanced Technology Laboratory, Fujikura Ltd., 1440, Mutsuzaki, Sakura, Chiba 285-8550, Japan. 4 Advanced ICT
Res. Inst., National Institute of Information and Communications Technology, 588-2 Iwaoka, Nishi-ku, Kobe 651-2492, Japan. 5 Department of Electronics,
Graduate School of Engineering, Nagoya University, Furo-cho, Chikusa-ku, Nagoya, Japan. 6These authors contributed equally: Davide Bacco, Beatrice Da Lio.
*email: ;
COMMUNICATIONS PHYSICS | (2019)2:140 | https://doi.org/10.1038/s42005-019-0238-1 | www.nature.com/commsphys
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ARTICLE
COMMUNICATIONS PHYSICS | https://doi.org/10.1038/s42005-019-0238-1
O
ur society is based on the continuous exchange of billions
of data, and most of them travel in optical fibres. Nonetheless, most of the exchanged data are not protected
against upcoming threats, i.e., new algorithms able to break current
cyphers and the expected availability of quantum computers1. A
quantum computer is a machine based on the laws of quantum
physics, which will be able to crack some of the current cryptosystems, whose security relies on the limited computational power
of an eavesdropper2. As derived by Shannon, a way to achieve
information theoretical secure communications is to use OneTime-Pad encryption, which requires a pre-shared key of the same
size as the message to be sent3. However, other symmetric key
algorithms based on computationally hard problems are also used,
such as the Advanced Encryption Standard, since they require keys
of constant length (e.g. 128 or 256 bits)4. The symmetric key used
by these cryptosystems must be exchanged between the two parties, and this is usually achieved through public-key algorithms,
two of the most widely used being the Rivest–Shamir–Adler and
the elliptic curve cryptography5–7. A quantum computer can
however break both algorithms, leaving the task of distributing
keys to either post-quantum cryptography8 or to alternative
methods such as quantum cryptography. Within the latter,
quantum key distribution (QKD) addresses this challenge by
relying on the laws of quantum physics to provide the required
information-theoretic security9. During the last 30 years, multiple
demonstrations of free-space, underwater and fibre-based QKD
systems have shown the feasibility of such a technology10–16.
Nevertheless, multiple factors are limiting the global deployment of
QKD systems: the low information rate, the short propagation
distance and the compatibility with the existing network infrastructure. Indeed, most of QKD implementations have been realised in low noise environments (e.g. dark fibres), attesting to the
difficulty of integration with the bright signals used in classical
communications17–23. In this work, we show how to overcome the
low rate and compatibility limitations by exploiting a 37-core
multicore fibre (MCF) as a technology for quantum communications24. This technology allows for efficient key generation,
enabling the highest secret key rate presented to date. Moreover,
we co-propagate in all the 37 cores simultaneously a high-speed
classical signal, showing that the quantum communication is only
weakly perturbed by it, paving the way for a full-fleshed implementation in current communication infrastructures.
reducing the overall power budget, thus decreasing the total
power consumption25–27. As reported in Fig. 1a, through SDM
the achievable rate of an N-core MCF corresponds theoretically to
N times the achievable rate of a single mode fibre28. To achieve
these high rates, a low cross-talk between the different channels is
of extreme importance for SDM schemes. Indeed, cross-talk is the
measure of the leakage from one channel to another, leading
therefore to a larger insertion loss in the former and, more
importantly, to an extra noise source in the latter. As an example,
high-speed classical communication at 10:16 Pbit s1 has been
demonstrated thanks to SDM combined with dense wavelength
division multiplexing, polarisation modulation and advanced
coding29. Likewise, both multicore and few-mode fibres have
been exploited for encoding and transmitting high-dimensional
(Hi-D) quantum states30–32. In particular, the cores or the modes
of these special fibres have been used to increase the dimensionality of the Hilbert space, thus allowing higher photon
information efficiency. Although Hi-D quantum states are suitable for high rate quantum communications, in specific channel
conditions (low noise channel), it was experimentally demonstrated that SDM is suitable for very high rate secure communications33. The principle is based on the concatenation of
parallel keys acquired in each core/mode as shown in Fig. 1b33.
As a support of this statement, Fig. 2 shows a theoretical analysis
of the secret key rate as a function of the error rate for Hi-D and
parallel encoding when assuming transmission in a lossy bosonic
Gaussian channel (e.g. a fibre link)28. As a matter of fact, in the
low noise regime, the performance achieved by Hi-D protocols is
lower compared to the one obtained with the multiplexing of
parallel encoding (SDM). Note that, similarly to SDM in classical
communications, the generation of parallel keys is achieved when
each core/mode is used to transmit independent quantum states.
The receiver measures each core/mode individually and then after
distillation and reconciliation processes a longer key is available
between the two users. In our demonstration (...truncated)