<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Francesco Arzani | LIP6 - Équipe QI</title><link>https://qi.lip6.fr/fr/people/francesco-arzani/</link><atom:link href="https://qi.lip6.fr/fr/people/francesco-arzani/index.xml" rel="self" type="application/rss+xml"/><description>Francesco Arzani</description><generator>Hugo Blox Builder (https://hugoblox.com)</generator><language>fr</language><copyright>© 2022 LIP6 Quantum Information Team</copyright><lastBuildDate>Mon, 05 Aug 2019 00:00:00 +0000</lastBuildDate><image><url>https://qi.lip6.fr/media/icon_hu_bdeccd9e706ea09d.png</url><title>Francesco Arzani</title><link>https://qi.lip6.fr/fr/people/francesco-arzani/</link></image><item><title>Random coding for sharing bosonic quantum secrets</title><link>https://qi.lip6.fr/fr/publication/2285301-random-coding-for-sharing-bosonic-quantum-secrets/</link><pubDate>Mon, 05 Aug 2019 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/2285301-random-coding-for-sharing-bosonic-quantum-secrets/</guid><description>&lt;p&gt;We consider a protocol for sharing quantum states using continuous variable systems. Specifically we introduce an encoding procedure where bosonic modes in arbitrary secret states are mixed with several ancillary squeezed modes through a passive interferometer. We derive simple conditions on the interferometer for this encoding to define a secret sharing protocol and we prove that they are satisfied by almost any interferometer. This implies that, if the interferometer is chosen uniformly at random, the probability that it may not be used to implement a quantum secret sharing protocol is zero. Furthermore, we show that the decoding operation can be obtained and implemented efficiently with a Gaussian unitary using a number of single-mode squeezers that is at most twice the number of modes of the secret, regardless of the number of players. We benchmark the quality of the reconstructed state by computing the fidelity with the secret state as a function of the input squeezing.&lt;/p&gt;</description></item><item><title>Violating Bell inequalities with entangled optical frequency combs and multi-pixel homodyne detection</title><link>https://qi.lip6.fr/fr/publication/1931758-violating-bell-inequalities-with-entangled-optical-frequency-combs-and-multi-pixel-homodyne-detection/</link><pubDate>Mon, 01 Jan 2018 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/1931758-violating-bell-inequalities-with-entangled-optical-frequency-combs-and-multi-pixel-homodyne-detection/</guid><description>&lt;p&gt;We have theoretically investigated the possibility of using any of several continuous-variable Bell-type inequalities - for which the dichotomic measurements are achieved with coarse-grained quadrature (homodyne) measurements - in a multi-party configuration where each participant is given a section, in the frequency domain, of the output of an optical parametric oscillator which has been synchronously-pumped with a frequency comb. Such light sources are undergoing intense study due to their novel properties, including the potential for production of light entangled in many hundreds of physical modes - a critical component for many proposals in optical or hybrid-optical quantum computation proposals. The situation we study notably uses only highly-efficient optical homodyne detection, meaning that in such systems the fair-sampling loophole would be relatively easy to avoid.&lt;/p&gt;</description></item></channel></rss>