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      A Quantum Enigma Machine: Experimentally Demonstrating Quantum Data Locking

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          Abstract

          Claude Shannon proved in 1949 that information-theoretic-secure encryption is possible if the encryption key is used only once, is random, and is at least as long as the message itself. Notwithstanding, when information is encoded in a quantum system, the phenomenon of quantum data locking allows one to encrypt a message with a shorter key and still provide information-theoretic security. We present one of the first feasible experimental demonstrations of quantum data locking for direct communication and propose a scheme for a quantum enigma machine that encrypts 6 bits per photon (containing messages, new encryption keys, and forward error correction bits) with less than 6 bits per photon of encryption key while remaining information-theoretically secure.

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          Communication Theory of Secrecy Systems*

          C. Shannon (1949)
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            Polynomial Codes Over Certain Finite Fields

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              Quantum key distribution using gaussian-modulated coherent states

              , , (2003)
              Quantum continuous variables are being explored as an alternative means to implement quantum key distribution, which is usually based on single photon counting. The former approach is potentially advantageous because it should enable higher key distribution rates. Here we propose and experimentally demonstrate a quantum key distribution protocol based on the transmission of gaussian-modulated coherent states (consisting of laser pulses containing a few hundred photons) and shot-noise-limited homodyne detection; squeezed or entangled beams are not required. Complete secret key extraction is achieved using a reverse reconciliation technique followed by privacy amplification. The reverse reconciliation technique is in principle secure for any value of the line transmission, against gaussian individual attacks based on entanglement and quantum memories. Our table-top experiment yields a net key transmission rate of about 1.7 megabits per second for a loss-free line, and 75 kilobits per second for a line with losses of 3.1 dB. We anticipate that the scheme should remain effective for lines with higher losses, particularly because the present limitations are essentially technical, so that significant margin for improvement is available on both the hardware and software.
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                Author and article information

                Journal
                2016-05-20
                2016-07-21
                Article
                10.1103/PhysRevA.94.022315
                1605.06556
                0e3387e9-5905-4c09-a97e-b396afb9b5eb

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                Phys. Rev. A 94, 022315 (2016)
                10 Figures
                quant-ph physics.optics

                Quantum physics & Field theory,Optical materials & Optics
                Quantum physics & Field theory, Optical materials & Optics

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