{"id":131360,"date":"2021-11-27T15:22:42","date_gmt":"2021-11-27T23:22:42","guid":{"rendered":"https:\/\/lifeboat.com\/blog\/2021\/11\/quantum-superposition-of-thermodynamic-evolutions-with-opposing-times-arrows"},"modified":"2021-11-27T15:22:42","modified_gmt":"2021-11-27T23:22:42","slug":"quantum-superposition-of-thermodynamic-evolutions-with-opposing-times-arrows","status":"publish","type":"post","link":"https:\/\/lifeboat.com\/blog\/2021\/11\/quantum-superposition-of-thermodynamic-evolutions-with-opposing-times-arrows","title":{"rendered":"Quantum superposition of thermodynamic evolutions with opposing time\u2019s arrows"},"content":{"rendered":"<p><a class=\"aligncenter blog-photo\" href=\"https:\/\/lifeboat.com\/blog.images\/quantum-superposition-of-thermodynamic-evolutions-with-opposing-times-arrows2.jpg\"><\/a><\/p>\n<p>Taking a gas enclosed in a vessel as a pictorial example, the aforementioned state can be constructed by entangling the position of the piston with a further auxiliary quantum system, thereby establishing a quantum superposition of the following two processes: (i) a process wherein the gas particles are initially in thermal equilibrium confined in one half of the vessel by a piston, and the piston is pulled outwards, and (ii) the reverse process, in which the piston is pushed towards the gas, starting from an initial state where the gas occupies the entire vessel in thermal equilibrium.<\/p>\n<p>We will now measure the work of the system undergoing the above-mentioned superposition of forward and time-reversal dynamics. In order to implement such a measurement, we formally construct a procedure described by a set of measurement operators forming a completely positive and trace-preserving (CPTP) map. In this regard, we will refer to a standard TPM procedure to measure work in quantum thermodynamic processes<sup><a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 13\" title=\"Campisi, M., H\u00e4nggi, P. & Talkner, P. Colloquium: quantum fluctuation relations: foundations and applications. Rev. Mod. Phys. 83771&ndash;791 (2011).\" href=\"https:\/\/www.nature.com\/articles\/s42005-021-00759-1#ref-CR13\" id=\"ref-link-section-d4639363e3655\">13<\/a><\/sup>. Implementations of the TPM in quantum setups<sup><a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" title=\"Dorner, R. et al. Extracting quantum work statistics and fluctuation theorems by single-qubit interferometry. Phys. Rev. Lett. 110, 230601 (2013).\" href=\"https:\/\/www.nature.com\/articles\/s42005-021-00759-1#ref-CR25\" id=\"ref-link-section-d4639363e3659\">25<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" title=\"Mazzola, L., De Chiara, G. & Paternostro, M. Measuring the characteristic function of the work distribution. Phys. Rev. Lett. 110, 230602 (2013).\" href=\"https:\/\/www.nature.com\/articles\/s42005-021-00759-1#ref-CR26\" id=\"ref-link-section-d4639363e3659_1\">26<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" title=\"Batalh\u00e3o, T. B. et al. Experimental reconstruction of work distribution and study of fluctuation relations in a closed quantum system. Phys. Rev. Lett. 113, 140601 (2014).\" href=\"https:\/\/www.nature.com\/articles\/s42005-021-00759-1#ref-CR27\" id=\"ref-link-section-d4639363e3659_2\">27<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" title=\"Roncaglia, A. J., Cerisola, F. & Paz, J. P. Work measurement as a generalized quantum measurement. Phys. Rev. Lett. 113, 250601 (2014).\" href=\"https:\/\/www.nature.com\/articles\/s42005-021-00759-1#ref-CR28\" id=\"ref-link-section-d4639363e3659_3\">28<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 29\" title=\"Chiara, G. D., Roncaglia, A. J. & Paz, J. P. Measuring work and heat in ultracold quantum gases. N. J. Phys. 17, 035004 (2015).\" href=\"https:\/\/www.nature.com\/articles\/s42005-021-00759-1#ref-CR29\" id=\"ref-link-section-d4639363e3662\">29<\/a><\/sup>, as well as suitable extensions<sup><a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" title=\"Perarnau-Llobet, M., B\u00e4umer, E., Hovhannisyan, K. V., Huber, M. & Acin, A. No-go theorem for the characterization of work fluctuations in coherent quantum systems. Phys. Rev. Lett. 118, 070601 (2017).\" href=\"https:\/\/www.nature.com\/articles\/s42005-021-00759-1#ref-CR30\" id=\"ref-link-section-d4639363e3666\">30<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" title=\"\u00c5berg, J. Fully quantum fluctuation theorems. Phys. Rev. X 8, 011019 (2018).\" href=\"https:\/\/www.nature.com\/articles\/s42005-021-00759-1#ref-CR31\" id=\"ref-link-section-d4639363e3666_1\">31<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" title=\"Debarba, T., Manzano, G., Guryanova, Y., Huber, M. & Friis, N. Work estimation and work fluctuations in the presence of non-ideal measurements. N. J. Phys. 21, 113002 (2019).\" href=\"https:\/\/www.nature.com\/articles\/s42005-021-00759-1#ref-CR32\" id=\"ref-link-section-d4639363e3666_2\">32<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 33\" title=\"Mohammady, M. H. & Romito, A. Conditional work statistics of quantum measurements. Quantum 3,175 (2019).\" href=\"https:\/\/www.nature.com\/articles\/s42005-021-00759-1#ref-CR33\" id=\"ref-link-section-d4639363e3669\">33<\/a><\/sup>, have recently received increasing attention. Our procedure can be seen as a generalisation of the TPM scheme to situations where different thermodynamic processes are allowed to be superposed, and can consequently interfere.<\/p>\n<p>In the TPM scheme, work is defined as the energy difference between the initial and final states of the system, which are measured through ideal projective measurements of the system Hamiltonian implemented before and after the thermodynamic process associated with the protocol \u039b<sup><a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 34\" title=\"Talkner, P., Lutz, E. & H\u00e4nggi, P. Fluctuation theorems: work is not an observable. Phys. Rev. E 75, 050102 (2007).\" href=\"https:\/\/www.nature.com\/articles\/s42005-021-00759-1#ref-CR34\" id=\"ref-link-section-d4639363e3676\">34<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 35\" title=\"Talkner, P. & H\u00e4nggi, P. Aspects of quantum work. Phys. Rev. E 93, 022131 (2016).\" href=\"https:\/\/www.nature.com\/articles\/s42005-021-00759-1#ref-CR35\" id=\"ref-link-section-d4639363e3679\">35<\/a><\/sup>. This measurement scheme can be performed, individually, both for the forward and the time-reversal processes, enabling the construction of the work probability distributions <i>P <\/i>(<i>W<\/i>) and \\(\\tilde{P}(W)\\) 0, respectively.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Taking a gas enclosed in a vessel as a pictorial example, the aforementioned state can be constructed by entangling the position of the piston with a further auxiliary quantum system, thereby establishing a quantum superposition of the following two processes: (i) a process wherein the gas particles are initially in thermal equilibrium confined in one [\u2026]<\/p>\n","protected":false},"author":427,"featured_media":0,"comment_status":"open","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[48,1617],"tags":[],"class_list":["post-131360","post","type-post","status-publish","format-standard","hentry","category-particle-physics","category-quantum-physics"],"_links":{"self":[{"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/posts\/131360","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/users\/427"}],"replies":[{"embeddable":true,"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/comments?post=131360"}],"version-history":[{"count":0,"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/posts\/131360\/revisions"}],"wp:attachment":[{"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/media?parent=131360"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/categories?post=131360"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/tags?post=131360"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}