{"id":3870,"date":"2019-11-13T14:38:15","date_gmt":"2019-11-13T13:38:15","guid":{"rendered":"http:\/\/web.am.qub.ac.uk\/wp\/qo\/?page_id=3870"},"modified":"2019-11-13T14:38:15","modified_gmt":"2019-11-13T13:38:15","slug":"previous-2018-2004","status":"publish","type":"page","link":"https:\/\/blogs.qub.ac.uk\/qteq\/publications\/previous-2018-2004\/","title":{"rendered":"Previous (up to 2018)"},"content":{"rendered":"<h2>2018<\/h2>\n<p style=\"padding-left: 30px\"><strong>32. Unconditional preparation of nonclassical states via linear-and-quadratic optomechanics,<\/strong><\/p>\n<p style=\"padding-left: 30px\">M.\u00a0Brunelli,\u00a0O. Houhou,\u00a0D. W. Moore,\u00a0A. Nunnenkamp,\u00a0M. Paternostro, and\u00a0A. Ferraro<\/p>\n<p style=\"padding-left: 30px\"><em>Phys. Rev. A <strong>98<\/strong>, 063801 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1103\/PhysRevA.98.063801\">10.1103\/PhysRevA.98.063801<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>31. Resource theory of quantum non-Gaussianity and Wigner negativity,<\/strong><\/p>\n<p style=\"padding-left: 30px\">F.\u00a0Albarelli, M. G. Genoni, M. G. A. Paris, and A. Ferraro<\/p>\n<p style=\"padding-left: 30px\"><em>Phys. Rev.\u00a0A <strong>98<\/strong>, 052350 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1103\/PhysRevA.98.052350\">10.1103\/PhysRevA.98.052350<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>30. Reconciliation of quantum local master equations with thermodynamics,<\/strong><\/p>\n<p style=\"padding-left: 30px\">G.\u00a0De Chiara, G. Landi, A.\u00a0Hewgill, B. Reid, A. Ferraro, A. J. Roncaglia, and M. Antezza<\/p>\n<p style=\"padding-left: 30px\"><em>New J. Phys. <strong>20<\/strong>, 113024 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1088\/1367-2630\/aaecee\">10.1088\/1367-2630\/aaecee<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>29.\u00a0Approximate supervised learning of quantum gates via ancillary qubits,<\/strong><\/p>\n<p style=\"padding-left: 30px\">L.\u00a0Innocenti, L. Banchi, S. Bose, A. Ferraro, and M. Paternostro<\/p>\n<p style=\"padding-left: 30px\"><em>Int. J. Quantum Inf.\u00a0<strong>16<\/strong>, 1840004 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1142\/S021974991840004X\">10.1142\/S021974991840004X<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>28. Rhombi-chain Bose-Hubbard model: Geometric frustration and interactions,<\/strong><\/p>\n<p style=\"padding-left: 30px\">C.\u00a0Cartwright,\u00a0G. De Chiara, and\u00a0M. Rizzi<\/p>\n<p style=\"padding-left: 30px\"><em>Phys. Rev. B <strong>98<\/strong>, 184508 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<a href=\"https:\/\/doi.org\/10.1103\/PhysRevB.98.184508\"><strong>10.1103\/PhysRevB.98.184508<\/strong><\/a><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>27. Probing quantum features of photosynthetic organisms,<\/strong><\/p>\n<p style=\"padding-left: 30px\">T.\u00a0Krisnanda, C. Marletto, V. Vedral, M. Paternostro, and T. Paterek<\/p>\n<p style=\"padding-left: 30px\"><em>npj Quantum Information <strong>4<\/strong>, 60 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:<strong>\u00a0<\/strong><a href=\"https:\/\/doi.org\/10.1038\/s41534-018-0110-2\"><strong>10.1038\/s41534-018-0110-2<\/strong><\/a><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>26.\u00a0Experimental determination of irreversible entropy production in out-of-equilibrium mesoscopic quantum systems,<\/strong><\/p>\n<p style=\"padding-left: 30px\">M. Brunelli, L. Fusco, R. Landig, W. Wieczorek, J. Hoelscher-Obermaier, G. Landi, F.\u2009L. Semi\u00e3o, A. Ferraro, N. Kiesel, T. Donner, G. De Chiara, and M. Paternostro<\/p>\n<p style=\"padding-left: 30px\"><em>Phys. Rev. Lett. <strong>121<\/strong>, 160604 (2018) (Editor&#8217;s Suggestion &amp; <strong><a href=\"https:\/\/physics.aps.org\/synopsis-for\/10.1103\/PhysRevLett.121.160604\">Featured in Physics<\/a><\/strong>)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.121.160604\">10.1103\/PhysRevLett.121.160604<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>25. Quantum correlations and thermodynamic performances of two-qubit engines with local and common baths,<\/strong><\/p>\n<p style=\"padding-left: 30px\">A.\u00a0Hewgill, A. Ferraro, and G. De Chiara<\/p>\n<p style=\"padding-left: 30px\"><em>Phys. Rev. A\u00a0<strong>98<\/strong>, 042102\u00a0(2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1103\/PhysRevA.98.042102\">10.1103\/PhysRevA.98.042102<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>24. Nonequilibrium thermodynamics of continuously measured quantum systems: A circuit QED implementation,<\/strong><\/p>\n<p style=\"padding-left: 30px\">P. G. Di Stefano, J. J. Alonso, E. Lutz, G. Falci, and M. Paternostro<\/p>\n<p style=\"padding-left: 30px\"><em>Phys. Rev. B\u00a0<strong>98<\/strong>, 144514\u00a0(2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1103\/PhysRevB.98.144514\">10.1103\/PhysRevB.98.144514<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>23.\u00a0Unitary unraveling for the dissipative continuous spontaneous localization model: Application to optomechanical experiments,<\/strong><\/p>\n<p style=\"padding-left: 30px\">J. Nobakht, M. Carlesso, S. Donadi, M. Paternostro, and A. Bassi<\/p>\n<p style=\"padding-left: 30px\"><em>Phys. Rev. A <strong>98<\/strong>, 042109 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<a href=\"https:\/\/doi.org\/10.1103\/PhysRevA.98.042109\"><strong>10.1103\/PhysRevA.98.042109<\/strong><\/a><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>22.\u00a0\u200bNon-interferometric test of the continuous spontaneous localization model based on rotational optomechanics,<\/strong><\/p>\n<p style=\"padding-left: 30px\">M.\u00a0Carlesso, M. Paternostro, H. Ulbricht, A. Vinante, and A. Bassi<\/p>\n<p style=\"padding-left: 30px\"><em>New J. Phys. <strong>20<\/strong>, 083022 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1088\/1367-2630\/aad863\">10.1088\/1367-2630\/aad863<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>21. Performance of shortcut-to-adiabaticity quantum engines,<\/strong><\/p>\n<p style=\"padding-left: 30px\">O.\u00a0Abah, and E. Lutz<\/p>\n<p style=\"padding-left: 30px\"><em>Phys. Rev.\u00a0\u200bE\u00a0<strong>98<\/strong>, 032121 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1103\/PhysRevE.98.032121\">10.1103\/PhysRevE.98.032121<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>20. Characterizing irreversibility in open quantum systems,<\/strong><\/p>\n<p style=\"padding-left: 30px\">T. B. Batalhao, S. Gherardini, J. P. Santos, G. T. Landi, and M. Paternostro<\/p>\n<p style=\"padding-left: 30px\"><em>\u200b<\/em>In\u00a0<em>Thermodynamics in the Quantum Regime (Eds. F.\u00a0Binder, L. A. Correa, C. Gogolin, J. Anders, and G. Adesso), pages\u00a0887-896<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1007\/978-3-319-99046-0_16\">10.1007\/978-3-319-99046-0_16<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>19. Ancilla-assisted measurement of quantum work,<\/strong><\/p>\n<p style=\"padding-left: 30px\">G.\u00a0De Chiara,\u00a0P. Solinas,\u00a0F. Cerisola, and A.\u00a0J. Roncaglia<\/p>\n<p style=\"padding-left: 30px\"><em>\u200b<\/em>In\u00a0<em>Thermodynamics in the Quantum Regime (Eds. F.\u00a0Binder, L. A. Correa, C. Gogolin, J. Anders, and G. Adesso), pages\u00a0337-362<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1007\/978-3-319-99046-0_14\">10.1007\/978-3-319-99046-0_14<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>18. Single atom heat engine in a tapered ion trap,<\/strong><\/p>\n<p style=\"padding-left: 30px\">S. T. Dawkins, O. Abah, K. Singer, S. Deffner<\/p>\n<p style=\"padding-left: 30px\"><em>\u200b<\/em>In\u00a0<em>Thermodynamics in the Quantum Regime (Eds. F. Binder, L. A. Correa, C. Gogolin, J. Anders, and G. Adesso), pages\u00a0887-896<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1007\/978-3-319-99046-0_36\">10.1007\/978-3-319-99046-0_36<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>17.\u00a0Schmidt gap in random spin chains,<\/strong><\/p>\n<p style=\"padding-left: 30px\">G.\u00a0Torlai,\u00a0K. D. McAlpine, and\u00a0G. De Chiara<\/p>\n<p style=\"padding-left: 30px\"><em>Phys. Rev.\u00a0\u200bB <strong>98<\/strong>, 085153 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1103\/PhysRevB.98.085153\">10.1103\/PhysRevB.98.085153<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>16. Experimental signature of quantum Darwinism in photonic cluster states,<\/strong><\/p>\n<p style=\"padding-left: 30px\">M.\u00a0A. Ciampini, G. Pinna, P. Mataloni, and M. Paternostro<\/p>\n<p style=\"padding-left: 30px\"><em>Phys. Rev.\u00a0\u200bA\u00a0<strong>98<\/strong>, 020101(R) (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1103\/PhysRevA.98.020101\">10.1103\/PhysRevA.98.020101<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>15.\u00a0Genuine quantum correlations in quantum many-body systems: a review of recent progress,<\/strong><\/p>\n<p style=\"padding-left: 30px\">G.\u00a0De Chiara, and A. Sanpera<\/p>\n<p style=\"padding-left: 30px\"><em>Rep. Prog. Phys. <strong>81<\/strong>, 074002 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1088\/1361-6633\/aabf61\">10.1088\/1361-6633\/aabf61<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>14. Coherent merging of counterpropagating exciton-polariton superfluids,<\/strong><\/p>\n<p style=\"padding-left: 30px\">T. Boulier, S. Pigeon, E. Cancellieri, P. Robin, E. Giacobino, Q. Glorieux, and A. Bramati<\/p>\n<p style=\"padding-left: 30px\"><em>Phys. Rev. B <strong>98<\/strong>, 024503 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1103\/PhysRevB.98.024503\">10.1103\/PhysRevB.98.024503<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>13.\u00a0Information-reality complementarity in photonic weak measurements,<\/strong><\/p>\n<p style=\"padding-left: 30px\">L.\u00a0Mancino, M. Sbroscia, E. Roccia, I. Gianani, V. Cimini, M. Paternostro, and M. Barbieri<\/p>\n<p style=\"padding-left: 30px\"><em>Phys. Rev.\u00a0\u200bA <strong>97<\/strong>, 062108 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1103\/PhysRevA.97.062108\">10.1103\/PhysRevA.97.062108<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>12. Connecting nth order generalised quantum Rabi models: Emergence of nonlinear spin-boson coupling via spin rotations,<\/strong><\/p>\n<p style=\"padding-left: 30px\">J.\u00a0Casanova, R. Puebla, H. Moya-Cessa, and M. B. Plenio<\/p>\n<p style=\"padding-left: 30px\"><i>npj Quantum Information <strong>4<\/strong>, 47 (2018)<\/i><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<a href=\"https:\/\/doi.org\/10.1038\/s41534-018-0096-9\"><strong>10.1038\/s41534-018-0096-9<\/strong><\/a><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>11. Relative resilience to noise of standard and sequential approaches to measurement-based quantum computation,<\/strong><\/p>\n<p style=\"padding-left: 30px\">C. B. Gallagher, and A. Ferraro<\/p>\n<p style=\"padding-left: 30px\"><em>Phys. Rev.\u00a0A\u00a0<strong>97<\/strong>, 052305 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<a href=\"https:\/\/doi.org\/10.1103\/PhysRevA.97.052305\"><strong>10.1103\/PhysRevA.97.052305<\/strong><\/a><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>10.\u00a0Spin-phase-space-entropy production,<\/strong><\/p>\n<p style=\"padding-left: 30px\">J.\u00a0P. Santos, L.\u00a0C. C\u00e9leri,\u00a0F. Brito, G. T. Landi, and M. Paternostro<\/p>\n<p style=\"padding-left: 30px\"><em>Phys. Rev.\u00a0A\u00a0<strong>97<\/strong>, 052123 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1103\/PhysRevA.97.052123\">10.1103\/PhysRevA.97.052123<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>9. Irreversibility at zero temperature from the perspective of the environment,<\/strong><\/p>\n<p style=\"padding-left: 30px\">J.\u00a0P. Santos, A. L. de Paula, R. Drumond, G. T. Landi, and M. Paternostro<\/p>\n<p style=\"padding-left: 30px\"><em>Phys. Rev.\u00a0A <strong>97<\/strong>, 050101(R) (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1103\/PhysRevA.97.050101\">10.1103\/PhysRevA.97.050101<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>8. Phase-space interference in extensive and nonextensive quantum heat engines\u200b,<\/strong><\/p>\n<p style=\"padding-left: 30px\">A. \u00dc. C. Hardal, M. Paternostro, and \u00d6. E. M\u00fcstecapl\u0131o\u011flu<\/p>\n<p style=\"padding-left: 30px\"><em>Phys. Rev. E <strong>97<\/strong>, 042127 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1103\/PhysRevE.97.042127\">10.1103\/PhysRevE.97.042127<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>7. Entanglement scaling at first order quantum phase transitions,<\/strong><\/p>\n<p style=\"padding-left: 30px\">A. Yuste, C. Cartwright, G. De Chiara, and A. Sanpera<\/p>\n<p style=\"padding-left: 30px\"><em>New J. Phys. <strong>20<\/strong>, 043006 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1088\/1367-2630\/aab2db\">10.1088\/1367-2630\/aab2db<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>6. The entropic cost of quantum generalized measurements,<\/strong><\/p>\n<p style=\"padding-left: 30px\">L.\u00a0Mancino,\u00a0M. Sbroscia, E. Roccia, I. Gianani, F. Somma, P. Mataloni, M. Paternostro, and M. Barbieri<\/p>\n<p style=\"padding-left: 30px\"><em>npj Quantum Information <strong>4<\/strong>, 20 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1038\/s41534-018-0069-z\">10.1038\/s41534-018-0069-z<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>5. A self-contained quantum harmonic engine,<\/strong><\/p>\n<p style=\"padding-left: 30px\">B. Reid, S. Pigeon, M. Antezza, and G. De Chiara<\/p>\n<p style=\"padding-left: 30px\"><em>EPL <strong>120<\/strong>, 60006 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1209\/0295-5075\/120\/60006\">10.1209\/0295-5075\/120\/60006<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>4. Operational Markov condition for quantum processes,<\/strong><\/p>\n<p style=\"padding-left: 30px\">F.\u00a0A. Pollock, C.\u00a0Rodr\u00edguez-Rosario, T. Frauenheim, M.\u00a0Paternostro, and K.\u00a0Modi<\/p>\n<p style=\"padding-left: 30px\"><em>Phys.\u00a0Rev. Lett.\u00a0<strong>120<\/strong>,\u00a0040405 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.120.040405\">10.1103\/PhysRevLett.120.040405<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>3. Cavity assisted measurements of heat and work in optical lattices,<\/strong><\/p>\n<p style=\"padding-left: 30px\">L. Villa, and G. De Chiara<\/p>\n<p style=\"padding-left: 30px\"><em>Quantum <strong>2<\/strong>, 42 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.22331\/q-2018-01-04-42\">10.22331\/q-2018-01-04-42<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>2. Non-Markovian quantum processes: Complete framework and efficient characterization,<\/strong><\/p>\n<p style=\"padding-left: 30px\">F. A. Pollock, C. Rodr\u00edguez-Rosario, T. Frauenheim, M. Paternostro, and K. Modi<\/p>\n<p style=\"padding-left: 30px\"><em>Phys.\u00a0Rev. A <strong>97<\/strong>, 012127 (2018)<\/em><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1103\/PhysRevA.97.012127\">10.1103\/PhysRevA.97.012127<\/a><\/strong><\/p>\n<hr \/>\n<p style=\"padding-left: 30px\"><strong>1. Robust quantum state engineering through coherent localization in biased-coin quantum walks,<\/strong><\/p>\n<p style=\"padding-left: 30px\">H.\u00a0Majury,\u00a0J. Boutari,\u00a0E. O\u2019Sullivan,\u00a0A. Ferraro, and M. Paternostro<\/p>\n<p style=\"padding-left: 30px\"><i>EPJ Quantum Technology <strong>5<\/strong>, 1 (2018)<\/i><\/p>\n<p style=\"padding-left: 30px\">doi:\u00a0<strong><a href=\"https:\/\/doi.org\/10.1140\/epjqt\/s40507-017-0065-9\">10.1140\/epjqt\/s40507-017-0065-9<\/a><\/strong><\/p>\n","protected":false},"excerpt":{"rendered":"<p>2018 32. Unconditional preparation of nonclassical states via linear-and-quadratic optomechanics, M.\u00a0Brunelli,\u00a0O. Houhou,\u00a0D. W. Moore,\u00a0A. Nunnenkamp,\u00a0M. Paternostro, and\u00a0A. Ferraro Phys. Rev. A 98, 063801 (2018) doi:\u00a010.1103\/PhysRevA.98.063801 31. Resource theory of quantum non-Gaussianity and Wigner negativity, F.\u00a0Albarelli, M. G. Genoni, M. G. A. Paris, and A. Ferraro Phys. Rev.\u00a0A 98, 052350 (2018) doi:\u00a010.1103\/PhysRevA.98.052350 30. Reconciliation of quantum [&hellip;]<\/p>\n","protected":false},"author":1556,"featured_media":0,"parent":29,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-3870","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/blogs.qub.ac.uk\/qteq\/wp-json\/wp\/v2\/pages\/3870","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/blogs.qub.ac.uk\/qteq\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/blogs.qub.ac.uk\/qteq\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/blogs.qub.ac.uk\/qteq\/wp-json\/wp\/v2\/users\/1556"}],"replies":[{"embeddable":true,"href":"https:\/\/blogs.qub.ac.uk\/qteq\/wp-json\/wp\/v2\/comments?post=3870"}],"version-history":[{"count":0,"href":"https:\/\/blogs.qub.ac.uk\/qteq\/wp-json\/wp\/v2\/pages\/3870\/revisions"}],"up":[{"embeddable":true,"href":"https:\/\/blogs.qub.ac.uk\/qteq\/wp-json\/wp\/v2\/pages\/29"}],"wp:attachment":[{"href":"https:\/\/blogs.qub.ac.uk\/qteq\/wp-json\/wp\/v2\/media?parent=3870"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}