{"id":1097,"date":"2017-02-14T12:34:28","date_gmt":"2017-02-14T10:34:28","guid":{"rendered":"https:\/\/webs.uab.cat\/giq\/seminar\/gaussian-optimizers-in-quantum-information\/"},"modified":"2017-02-14T12:34:28","modified_gmt":"2017-02-14T10:34:28","slug":"gaussian-optimizers-in-quantum-information","status":"publish","type":"seminar","link":"https:\/\/webs.uab.cat\/giq\/seminar\/gaussian-optimizers-in-quantum-information\/","title":{"rendered":"Gaussian optimizers in quantum information"},"content":{"rendered":"<p>We determine the p-&gt;q norms of the one-mode quantum-limited attenuator and amplifier, and prove that&nbsp;they are achieved by Gaussian states. The proof technique is completely new: it is based on a new logarithmic&nbsp;Sobolev inequality, and it can be used to determine the p-&gt;q norms of any quantum semigroup. Our result&nbsp;extends to noncommutative probability the seminal theorem &#8220;Gaussian kernels have only Gaussian maximizers&#8221;&nbsp;[Lieb, Invent. Math. 102, 179 (1990)], stating that Gaussian functions achieve the p-&gt;q norms of Gaussian&nbsp;integral kernels.<br \/>\nWe then exploit our result to prove the longstanding conjecture stating that Gaussian thermal input states&nbsp;minimize the output von Neumann entropy of one-mode phase-covariant quantum Gaussian channels among all&nbsp;the input states with a given entropy. Phase-covariant quantum Gaussian channels model the attenuation and the&nbsp;noise that affect any electromagnetic signal in the quantum regime. This result is crucial to prove the converse&nbsp;theorems for both the triple trade-off region and the capacity region for broadcast communication of the Gaussian&nbsp;quantum-limited amplifier. This result also extends to the quantum regime the Entropy Power Inequality that plays&nbsp;a key role in classical information theory. The proof technique can be applied to any quantum channel.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>We determine the p-&gt;q norms of the one-mode quantum-limited attenuator and amplifier, and prove that&nbsp;they are achieved by Gaussian states. The proof technique is completely new: it is based on a new logarithmic&nbsp;Sobolev inequality, and it can be used to determine the p-&gt;q norms of any quantum semigroup. Our result&nbsp;extends to noncommutative probability the seminal [&hellip;]<\/p>\n","protected":false},"author":20,"featured_media":0,"template":"","class_list":["post-1097","seminar","type-seminar","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/webs.uab.cat\/giq\/wp-json\/wp\/v2\/seminar\/1097","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=1097"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}