<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Filippus S. Roux | LIP6 - Équipe QI</title><link>https://qi.lip6.fr/fr/people/filippus-s.-roux/</link><atom:link href="https://qi.lip6.fr/fr/people/filippus-s.-roux/index.xml" rel="self" type="application/rss+xml"/><description>Filippus S. Roux</description><generator>Hugo Blox Builder (https://hugoblox.com)</generator><language>fr</language><copyright>© 2022 LIP6 Quantum Information Team</copyright><lastBuildDate>Wed, 01 Jan 2020 00:00:00 +0000</lastBuildDate><image><url>https://qi.lip6.fr/media/icon_hu_bdeccd9e706ea09d.png</url><title>Filippus S. Roux</title><link>https://qi.lip6.fr/fr/people/filippus-s.-roux/</link></image><item><title>Entanglement of truncated quantum states</title><link>https://qi.lip6.fr/fr/publication/2907279-entanglement-of-truncated-quantum-states/</link><pubDate>Wed, 01 Jan 2020 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/2907279-entanglement-of-truncated-quantum-states/</guid><description>&lt;p&gt;We investigate the impact of Hilbert-space truncation upon the entanglement of an initially maximally entangled m × m bipartite quantum state, after propagation under an entanglement-preserving n × n (n ≥ m) unitary. Truncation-physically enforced, e.g., by a detector&amp;rsquo;s finite cross section-projects the state onto an s × s-dimensional subspace (3 ≤ s ≤ n). For a random local unitary evolution, we obtain a simple analytical formula that expresses the truncation-induced entanglement loss as a function of n, m and s.&lt;/p&gt;</description></item></channel></rss>