<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Juan Miguel Arrazola | LIP6 - Équipe QI</title><link>https://qi.lip6.fr/fr/people/juan-miguel-arrazola/</link><atom:link href="https://qi.lip6.fr/fr/people/juan-miguel-arrazola/index.xml" rel="self" type="application/rss+xml"/><description>Juan Miguel Arrazola</description><generator>Hugo Blox Builder (https://hugoblox.com)</generator><language>fr</language><copyright>© 2022 LIP6 Quantum Information Team</copyright><lastBuildDate>Thu, 01 Nov 2018 00:00:00 +0000</lastBuildDate><image><url>https://qi.lip6.fr/media/icon_hu_bdeccd9e706ea09d.png</url><title>Juan Miguel Arrazola</title><link>https://qi.lip6.fr/fr/people/juan-miguel-arrazola/</link></image><item><title>Quantum superiority for verifying NP-complete problems with linear optics</title><link>https://qi.lip6.fr/fr/publication/1671939-quantum-superiority-for-verifying-np-complete-problems-with-linear-optics/</link><pubDate>Thu, 01 Nov 2018 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/1671939-quantum-superiority-for-verifying-np-complete-problems-with-linear-optics/</guid><description>&lt;p&gt;Demonstrating quantum superiority for some computational task will be a milestone for quantum technologies and would show that computational advantages are possible not only with a universal quantum computer but with simpler physical devices. Linear optics is such a simpler but powerful platform where classically-hard information processing tasks, such as Boson Sampling, can be in principle implemented. In this work, we study a fundamentally different type of computational task to achieve quantum superiority using linear optics, namely the task of verifying NP-complete problems. We focus on a protocol by Aaronson et al. (2008) that uses quantum proofs for verification. We show that the proof states can be implemented in terms of a single photon in an equal superposition over many optical modes. Similarly, the tests can be performed using linear-optical transformations consisting of a few operations: a global permutation of all modes, simple interferometers acting on at most four modes, and measurement using single-photon detectors. We also show that the protocol can tolerate experimental imperfections.&lt;/p&gt;</description></item></channel></rss>