{"id":2097,"date":"2023-06-15T15:41:09","date_gmt":"2023-06-15T13:41:09","guid":{"rendered":"https:\/\/webs.uab.cat\/giq\/?post_type=seminar&#038;p=2097"},"modified":"2023-06-15T15:41:09","modified_gmt":"2023-06-15T13:41:09","slug":"dynamics-based-certification-of-quantumness","status":"publish","type":"seminar","link":"https:\/\/webs.uab.cat\/giq\/seminar\/dynamics-based-certification-of-quantumness\/","title":{"rendered":"Dynamics-based certification of quantumness"},"content":{"rendered":"\n<p>n this talk, I shall present our new technique to detect non-classicality under the assumption that the dynamics is known [1,2,3], based on an early insight by Tsirelson [4]. Most of the talk will focus on one and two harmonic oscillators, although the results can be widely generalized (we have shown them for precessing&nbsp;discrete systems [1], as well as for continuous&nbsp;systems with arbitrary time-independent Hamiltonian dynamics [3]). Among the highlights you can expect are the following:<\/p>\n\n\n\n<p>a) The criterion is an inequality that no classical model can violate. (This is particularly unusual for entanglement of continuous variable systems [2], where most of the witnesses rely on uncertainty relations, which can be violated by imprecise or badly calibrated measurements).<\/p>\n\n\n\n<p>b) The criterion requires a single measurement per round; and it is a quadrature measurement, thus routinely feasible. This is a major advantage over tests that require more measurements and constraining assumptions, like Leggett-Garg type tests (which require two sequential measurements and the assumption of non-invasiveness) or tests based on &#8220;contextuality&#8221; (which require the assumption that several measurements commute).<\/p>\n\n\n\n<p>c) The states that are detected have a symmetry that makes them suitable for bosonic error correcting codes.<\/p>\n\n\n\n<p>But most importantly, I shall insist on the main surprise: one can use the very classical dynamics of the harmonic oscillator to detect non-classicality [4].<\/p>\n\n\n\n<p>[1] L.T. Zaw et al., hys. Rev. A 106, 032222 (2022)&nbsp;<a href=\"https:\/\/arxiv.org\/abs\/2204.10498\" target=\"_blank\" rel=\"noreferrer noopener\">https:\/\/arxiv.org\/abs\/2204.10498<\/a><\/p>\n\n\n\n<p>[2] P. Jayachandran et al., Phys. Rev. Lett. 130, 160201 (2023)&nbsp;<a href=\"https:\/\/arxiv.org\/abs\/2210.10357\" target=\"_blank\" rel=\"noreferrer noopener\">https:\/\/arxiv.org\/abs\/2210.10357<\/a><\/p>\n\n\n\n<p>[3] L.T. Zaw and V.S.,&nbsp;<a href=\"https:\/\/arxiv.org\/abs\/2212.06017\" target=\"_blank\" rel=\"noreferrer noopener\">https:\/\/arxiv.org\/abs\/2212.06017<\/a><\/p>\n\n\n\n<p>[4] B. Tsirelson,&nbsp;<a href=\"https:\/\/arxiv.org\/abs\/quant-ph\/0611147\" target=\"_blank\" rel=\"noreferrer noopener\">https:\/\/arxiv.org\/abs\/quant-ph\/0611147<\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>n this talk, I shall present our new technique to detect non-classicality under the assumption that the dynamics is known [1,2,3], based on an early insight by Tsirelson [4]. Most of the talk will focus on one and two harmonic oscillators, although the results can be widely generalized (we have shown them for precessing&nbsp;discrete systems [&hellip;]<\/p>\n","protected":false},"author":2608,"featured_media":0,"template":"","class_list":["post-2097","seminar","type-seminar","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/webs.uab.cat\/giq\/wp-json\/wp\/v2\/seminar\/2097","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/webs.uab.cat\/giq\/wp-json\/wp\/v2\/seminar"}],"about":[{"href":"https:\/\/webs.uab.cat\/giq\/wp-json\/wp\/v2\/types\/seminar"}],"author":[{"embeddable":true,"href":"https:\/\/webs.uab.cat\/giq\/wp-json\/wp\/v2\/users\/2608"}],"wp:attachment":[{"href":"https:\/\/webs.uab.cat\/giq\/wp-json\/wp\/v2\/media?parent=2097"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}