<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Francisco Escudero Gutierrez | LIP6 - QI Team</title><link>https://qi.lip6.fr/people/francisco-escudero-gutierrez/</link><atom:link href="https://qi.lip6.fr/people/francisco-escudero-gutierrez/index.xml" rel="self" type="application/rss+xml"/><description>Francisco Escudero Gutierrez</description><generator>Hugo Blox Builder (https://hugoblox.com)</generator><language>en-us</language><copyright>© 2022 LIP6 Quantum Information Team</copyright><lastBuildDate>Wed, 08 Jul 2026 00:00:00 +0000</lastBuildDate><image><url>https://qi.lip6.fr/media/icon_hu_bdeccd9e706ea09d.png</url><title>Francisco Escudero Gutierrez</title><link>https://qi.lip6.fr/people/francisco-escudero-gutierrez/</link></image><item><title>Francisco Escudero Gutierrez - Nearly optimal algorithms to learn sparse quantum Hamiltonians in physically motivated distances
Room</title><link>https://qi.lip6.fr/seminars/2026-07-08-francisco-escudero-gutierrez/</link><pubDate>Wed, 08 Jul 2026 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/seminars/2026-07-08-francisco-escudero-gutierrez/</guid><description>&lt;h2 id="nearly-optimal-algorithms-to-learn-sparse-quantum-hamiltonians-in-physically-motivated-distances"&gt;Nearly optimal algorithms to learn sparse quantum Hamiltonians in physically motivated distances&lt;/h2&gt;
&lt;p&gt;Room
This seminar, given by Francisco Escudero Gutierrez, will happend on 08 July 2026, at 12:0.
It will take place in Room 24-25/405.&lt;/p&gt;
&lt;p&gt;Find a map of the campus &lt;a href="https://sciences.sorbonne-universite.fr/vie-de-campus-sciences/accueil-vie-pratique/plan-du-campus" target="_blank" rel="noopener"&gt;here&lt;/a&gt;.&lt;/p&gt;
&lt;h2 id="abstract"&gt;Abstract&lt;/h2&gt;
&lt;p&gt;We study the problem of learning Hamiltonians (H) that are (s)-sparse in the Pauli basis, given access to their time evolution. Although Hamiltonian learning has been extensively investigated, two issues recur in much of the existing literature: the absence of matching lower bounds and the use of mathematically convenient but physically opaque error measures.&lt;/p&gt;
&lt;p&gt;We address both challenges by introducing two physically motivated distances between Hamiltonians and designing a nearly optimal algorithm with respect to one of these metrics. The first, &lt;em&gt;time-constrained distance&lt;/em&gt;, quantifies distinguishability through dynamical evolution up to a bounded time. The second, &lt;em&gt;temperature-constrained distance&lt;/em&gt;, captures distinguishability through thermal states at bounded inverse temperatures.&lt;/p&gt;
&lt;p&gt;We show that (s)-sparse Hamiltonians with bounded operator norm can be learned in both distances with (O(s\log(1/\varepsilon))) experiments and (O(s^2/\varepsilon)) evolution time. For the time-constrained distance, we further establish lower bounds of (\Omega((s/n)\log(1/\varepsilon)+s)) experiments and (\Omega(s\sqrt{1/\varepsilon})) evolution time, demonstrating near-optimality in the number of experiments.&lt;/p&gt;
&lt;p&gt;As an intermediate result, we obtain an algorithm that learns every Pauli coefficient of (s)-sparse Hamiltonians up to error (\varepsilon) in (O(s\log(1/\varepsilon))) experiments and (O(s/\varepsilon)) evolution time, improving upon several recent results.&lt;/p&gt;
&lt;p&gt;The source of this improvement is a new isolation technique, inspired by the Valiant–Vazirani theorem (STOC &amp;lsquo;85), which shows that NP is as easy as detecting unique solutions. This technique allows us to query the time evolution of a single Pauli coefficient of a sparse Hamiltonian—even when the Pauli support of the Hamiltonian is unknown—ultimately enabling us to recover the Pauli support itself.&lt;/p&gt;
&lt;p&gt;Based on joint work (arXiv:2509.09813) with Amira Abbas, Nunzia Cerrato, Dmitry Grinko, Francesco Anna Mele, and Pulkit Sinha.&lt;/p&gt;</description></item></channel></rss>