{"id":1077,"date":"2016-07-05T11:13:02","date_gmt":"2016-07-05T09:13:02","guid":{"rendered":"https:\/\/webs.uab.cat\/giq\/seminar\/higher-order-interference-versus-quantum-theory\/"},"modified":"2016-07-05T11:13:02","modified_gmt":"2016-07-05T09:13:02","slug":"higher-order-interference-versus-quantum-theory","status":"publish","type":"seminar","link":"https:\/\/webs.uab.cat\/giq\/seminar\/higher-order-interference-versus-quantum-theory\/","title":{"rendered":"Higher order interference versus quantum theory"},"content":{"rendered":"<p>We (Ududec, Barnum, and Emerson) adapt Rafael Sorkin&#8217;s hierarchy of<br \/>orders of interference in physical theories to the framework of<br \/>&#8220;general probabilistic theories&#8221;, defining a notion of k-path<br \/>interference experiment and of k-th order coherence in such theories<br \/>and showing that k-th order interference in such an experiment is<br \/>equivalent to k-th order coherence between faces of the state spaces<br \/>associated with paths in the experiment. We also show that<br \/>Jordan-algebraic theories have at most second-order interference (the<br \/>first nontrivial level, and the one exhibited by quantum theory).<br \/>Barnum, Mueller and Ududec used the absence of 3rd order interference<br \/>(the first non-quantum order) as one of four postulates characterizing<br \/>the finite-dimensional complex quantum state and effect spaces: (1)<br \/>abstract spectrality (2) strong symmetry (3) no higher-order<br \/>interference and (4) energy observability. I will explain this result<br \/>and discuss whether or not all four are needed for a reasonable<br \/>thermodynamics. With a slight strengthening of (1), to unique<br \/>spectrality, and a significant weakening of (2), to the conjunction of<br \/>(a) projectivity (an abstraction of certain aspects of the quantum<br \/>projection postulate (L\u00b8ders&#8217; version)) and (b) symmetry of transition<br \/>probabilities under exchange of states with the unique finegrained<br \/>effects they make certain, we have the property, important in quantum<br \/>thermodynamics, that the outcome probabilities for any fine-grained<br \/>measurement are majorized by the spectrum of a state, and hence that<br \/>measurement-probability-based generalizations of classical<br \/>entropy-like functions are given by the classical function applied to<br \/>the spectrum.<\/p>\n<p>This is joint work with Cozmin Ududec and Joe Emerson (interference<br \/>and coherence), Markus Mueller and Cozmin Ududec (characterization of<br \/>quantum formalism) and with Jonathan Barrett, Marius Krumm, and Markus<br \/>Mueller (thermodynamics).<\/p>\n","protected":false},"excerpt":{"rendered":"<p>We (Ududec, Barnum, and Emerson) adapt Rafael Sorkin&#8217;s hierarchy oforders of interference in physical theories to the framework of&#8220;general probabilistic theories&#8221;, defining a notion of k-pathinterference experiment and of k-th order coherence in such theoriesand showing that k-th order interference in such an experiment isequivalent to k-th order coherence between faces of the state spacesassociated [&hellip;]<\/p>\n","protected":false},"author":20,"featured_media":0,"template":"","class_list":["post-1077","seminar","type-seminar","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/webs.uab.cat\/giq\/wp-json\/wp\/v2\/seminar\/1077","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=1077"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}