{"id":1129,"date":"2018-05-07T12:15:17","date_gmt":"2018-05-07T10:15:17","guid":{"rendered":"https:\/\/webs.uab.cat\/giq\/seminar\/quantum-metrology-with-one-dimensional-superradiant-photonic-states\/"},"modified":"2018-05-07T12:15:17","modified_gmt":"2018-05-07T10:15:17","slug":"quantum-metrology-with-one-dimensional-superradiant-photonic-states","status":"publish","type":"seminar","link":"https:\/\/webs.uab.cat\/giq\/seminar\/quantum-metrology-with-one-dimensional-superradiant-photonic-states\/","title":{"rendered":"Quantum metrology with one-dimensional superradiant photonic states"},"content":{"rendered":"<p>Photonic states with large and fixed photon numbers, such as Fock states, enable quantum-enhanced&nbsp;metrology but remain an experimentally elusive resource. A potentially simple, deterministic&nbsp;and scalable way to generate these states consists of fully exciting N quantum emitters&nbsp;equally coupled to a common photonic reservoir, which leads to a collective decay known as Dicke&nbsp;superradiance. The emitted N-photon state turns out to be a highly entangled multimode state, and&nbsp;to characterise its metrological properties in this work we: (i) develop theoretical tools to compute&nbsp;the Quantum Fisher Information of general multimode photonic states; (ii) use it to show that&nbsp;Dicke superradiant photons in 1D waveguides achieve Heisenberg scaling, which can be saturated&nbsp;by a parity measurement; (iii) and study the robustness of these states to experimental limitations&nbsp;in state-of-art atom-waveguide QED setups.<\/p>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Photonic states with large and fixed photon numbers, such as Fock states, enable quantum-enhanced&nbsp;metrology but remain an experimentally elusive resource. A potentially simple, deterministic&nbsp;and scalable way to generate these states consists of fully exciting N quantum emitters&nbsp;equally coupled to a common photonic reservoir, which leads to a collective decay known as Dicke&nbsp;superradiance. The emitted N-photon [&hellip;]<\/p>\n","protected":false},"author":20,"featured_media":0,"template":"","class_list":["post-1129","seminar","type-seminar","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/webs.uab.cat\/giq\/wp-json\/wp\/v2\/seminar\/1129","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\/20"}],"wp:attachment":[{"href":"https:\/\/webs.uab.cat\/giq\/wp-json\/wp\/v2\/media?parent=1129"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}