Correlation-boosted quantum engine: A proof-of principle demonstration
Employing currently available quantum technology, we design and implement a nonclassically correlated SWAP heat engine that allows to achieve an efficiency above the standard Carnot limit. Such an engine also boosts the amount of extractable work, in a wider parameter window, with respect to engine’...
- Autores:
-
Herrera Trujillo, Alba Marcela
Reina, John H.
D'Amico, Irene
Serra, Roberto M.
- Tipo de recurso:
- Article of investigation
- Fecha de publicación:
- 2023
- Institución:
- Universidad Autónoma de Occidente
- Repositorio:
- RED: Repositorio Educativo Digital UAO
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- eng
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- oai:red.uao.edu.co:10614/15866
- Acceso en línea:
- https://hdl.handle.net/10614/15866
https://red.uao.edu.co/
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- openAccess
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- Derechos reservados - American Physical Society, 2023
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Correlation-boosted quantum engine: A proof-of principle demonstration |
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Correlation-boosted quantum engine: A proof-of principle demonstration |
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Correlation-boosted quantum engine: A proof-of principle demonstration |
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Correlation-boosted quantum engine: A proof-of principle demonstration |
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Correlation-boosted quantum engine: A proof-of principle demonstration |
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Correlation-boosted quantum engine: A proof-of principle demonstration |
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Correlation-boosted quantum engine: A proof-of principle demonstration |
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Correlation-boosted quantum engine: A proof-of principle demonstration |
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Herrera Trujillo, Alba Marcela Reina, John H. D'Amico, Irene Serra, Roberto M. |
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Herrera Trujillo, Alba Marcela Reina, John H. D'Amico, Irene Serra, Roberto M. |
| description |
Employing currently available quantum technology, we design and implement a nonclassically correlated SWAP heat engine that allows to achieve an efficiency above the standard Carnot limit. Such an engine also boosts the amount of extractable work, in a wider parameter window, with respect to engine’s cycle in the absence of initial quantum correlations in the working substance. The boosted efficiency arises from a trade-off between the entropy production and the consumption of quantum correlations during the full thermodynamic cycle. We derive a generalized second-law limit for the correlated cycle and implement a proof-of-principle demonstration of the engine efficiency enhancement by effectively tailoring the thermal engine on a cloud quantum processors |
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Herrera Trujillo, A. M.; Reina, J. H.; D'Amico, I. y Serra, R. M. (2023). Correlation-boosted quantum engine: A proof-of principle demonstration. Physical review research. volumen 5. 11 p. DOI:https://doi.org/10.1103/PhysRevResearch.5.043104 |
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https://hdl.handle.net/10614/15866 |
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DOI:https://doi.org/10.1103/PhysRevResearch.5.043104 |
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26431564 |
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Universidad Autónoma de Occidente |
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Respositorio Educativo Digital UAO |
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https://red.uao.edu.co/ |
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Herrera Trujillo, A. M.; Reina, J. H.; D'Amico, I. y Serra, R. M. (2023). Correlation-boosted quantum engine: A proof-of principle demonstration. Physical review research. volumen 5. 11 p. DOI:https://doi.org/10.1103/PhysRevResearch.5.043104 DOI:https://doi.org/10.1103/PhysRevResearch.5.043104 26431564 Universidad Autónoma de Occidente Respositorio Educativo Digital UAO |
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https://hdl.handle.net/10614/15866 https://red.uao.edu.co/ |
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eng |
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eng |
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Physical review research |
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Crooks, Entropy production fluctuation theorem and the nonequilibrium work relation for free energy differences, Phys. Rev. E 60, 2721 (1999). [8] C. Jarzynski, Nonequilibrium equality for free energy differences, Phys. Rev. Lett. 78, 2690 (1997). [9] M. Esposito, U. Harbola and S. Mukamel, Nonequilibrium fluctuations, fluctuation theorems, and counting statistics in quantum systems, Rev. Mod. Phys. 81, 1665 (2009). [10] M. Campisi, P. Hänggi, and P. Talkner, Quantum fluctuation relations: Foundations and applications, Rev. Mod. Phys. 83, 771 (2011). [11] M. Herrera, J. P. S. Peterson, R. M. Serra, and I. D’Amico, Easy access to energy fluctuations in nonequilibrium quantum manybody systems, Phys. Rev. Lett. 127, 030602 (2021). [12] A. Auffèves, Quantum technologies need a quantum energy initiative, Phys. Rev. X Quantum 3, 020101 (2022). [13] T. Hugel, N. B. Holland, A. Cattani, L. Moroder, M. Seitz, and H. E. Gaub, Single-molecule optomechanical cycle, Science 296, 1103 (2002). [14] P. G. Steeneken, K. Le Phan, M. J. Goossens, G. E. J. Koops, G. J. A. M. Brom, C. van der Avoort, and J. T. M. van Beek, Piezoresistive heat engine and refrigerator, Nat. Phys. 7, 354 (2011). [15] V. Blickle and C. Bechinger, Realization of a micrometresized stochastic heat engine, Nat. Phys. 8, 143 (2012). [16] J.-P. Brantut, C. Grenier, J. Meineke, D. Stadler, S. Krinner, C. Kollath, T. Esslinger, and A. Georges, A thermoelectric heat engine with ultracold atoms, Science 342, 713 (2013). [17] J. Roßnagel, O. Abah, F. Schmidt-Kaler, K. Singer, and E. Lutz, Nanoscale heat engine beyond the carnot limit, Phys. Rev. Lett. 112, 030602 (2014). [18] H. Thierschmann, R. Sánchez, B. Sothmann, F. Arnold, C. Heyn, W. Hansen, H. Buhmann, and L. W. Molenkamp, Threeterminal energy harvester with coupled quantum dots, Nat. Nanotechnol. 10, 854 (2015). [19] J. Roßsnagel, S. T. Dawkins, K. N. Tolazzi, O. Abah, E. Lutz, F. Schmidt-Kaler, and K. Singer, A single-atom heat engine, Science 352, 325 (2016). [20] F. Schmidt, A. Magazzú, A. Callegari, L. Biancofiore, F. Cichos, and G. Volpe, Microscopic engine powered by critical demixing, Phys. Rev. Lett. 120, 068004 (2018). [21] Y. Zou, Y. Jiang, Y. Mei, X. Guo, and S. Du, Quantum heat engine using electromagnetically induced transparency, Phys. Rev. Lett. 119, 050602 (2017). [22] R. J. de Assis, T. M. de Mendonça, C. J. Villas-Boas, A. M. de Souza, R. S. Sarthour, I. S. Oliveira and N. G. de Almeida, Efficiency of a quantum otto heat engine operating under a reservoir at effective negative temperatures, Phys. Rev. Lett. 122, 240602 (2019). [23] J. Klatzow, J. Becker, P. Ledingham, C. Weinzetl, K. Kaczmarek, D. Saunders, J. Nunn, I. Walmsley, R. Uzdin, E. Poem, Experimental demonstration of quantum effects in the operation of microscopic heat engines, Phys. Rev. Lett. 122, 110601 (2019). [24] J. P. S. Peterson, T. B. Batalhão, M. Herrera, A. M. Souza, R. S. Sarthour, I. S. Oliveira, and R. M. Serra, Experimental characterization of a spin quantum heat engine, Phys. Rev. Lett. 123, 240601 (2019). [25] T. Denzler, J. F. G. Santos, E. Lutz, and R. M. Serra, Nonequilibrium fluctuations of a quantum heat engine, arXiv:2104.13427 v1. [26] A. Solfanelli, A. Santini, and M. Campisi, Experimental verification of fluctuation relations with a quantum computer, PRX Quantum 2, 030353 (2021). [27] N. M. Myers, O. Abah, and S. Deffner, Quantum thermodynamic devices: From theoretical proposals to experimental reality, AVS Quantum Sci. 4, 027101 (2022). [28] G. Lebon, D. Jou, and J. Casas-Vázques, Understanding Non-Equilibrium Thermodynamics: Foundations, Applications, Frontiers (Springer-Verlag, Berlin, 2008). [29] T. B. Batalhão, A. M. Souza, L. Mazzola, R. Auccaise, R. S. Sarthour, I. S. Oliveira, J. Goold, G. De Chiara, M. Paternostro, and R. M. 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Lett. 123, 090604 (2019). [66] At this point, we note note that non-classical correlations could be provided in various ways, e.g., by cooling an interacting many-body fluid to its ground/low-energy state with related creation of (thermal) entanglement. This kind of non-classical correlations which are present in many-body thermal states could be used in further applications to obtain some quantum advantage in thermal protocols. [67] H. Ollivier and W. H. Zurek, Quantum discord: A measure of the quantumness of correlations, Phys. Rev. Lett. 88, 017901 (2001). [68] QISKIT tomography. https://ignis.verification.tomography. [69] B. Daki´c, V. Vedral, and ˇc. Brukner, Necessary and sufficient condition for nonzero quantum discord, Phys. Rev. Lett. 105, 190502 (2010). [70] D. Girolami, and G. Adesso, Observable measure of bipartite quantum correlations, Phys. Rev. Lett. 108, 150403 (2012). |
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Herrera Trujillo, Alba Marcelavirtual::5734-1Reina, John H.D'Amico, IreneSerra, Roberto M.2024-10-15T20:15:36Z2024-10-15T20:15:36Z2023Herrera Trujillo, A. M.; Reina, J. H.; D'Amico, I. y Serra, R. M. (2023). Correlation-boosted quantum engine: A proof-of principle demonstration. Physical review research. volumen 5. 11 p. DOI:https://doi.org/10.1103/PhysRevResearch.5.043104https://hdl.handle.net/10614/15866DOI:https://doi.org/10.1103/PhysRevResearch.5.04310426431564Universidad Autónoma de OccidenteRespositorio Educativo Digital UAOhttps://red.uao.edu.co/Employing currently available quantum technology, we design and implement a nonclassically correlated SWAP heat engine that allows to achieve an efficiency above the standard Carnot limit. Such an engine also boosts the amount of extractable work, in a wider parameter window, with respect to engine’s cycle in the absence of initial quantum correlations in the working substance. The boosted efficiency arises from a trade-off between the entropy production and the consumption of quantum correlations during the full thermodynamic cycle. We derive a generalized second-law limit for the correlated cycle and implement a proof-of-principle demonstration of the engine efficiency enhancement by effectively tailoring the thermal engine on a cloud quantum processors11 páginasapplication/pdfengAmerican Physical SocietyDerechos reservados - American Physical Society, 2023https://creativecommons.org/licenses/by-nc-nd/4.0/info:eu-repo/semantics/openAccessAtribución-NoComercial-SinDerivadas 4.0 Internacional (CC BY-NC-ND 4.0)http://purl.org/coar/access_right/c_abf2Correlation-boosted quantum engine: A proof-of principle demonstrationArtículo de revistahttp://purl.org/coar/resource_type/c_2df8fbb1Textinfo:eu-repo/semantics/articlehttp://purl.org/redcol/resource_type/ARTinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/version/c_970fb48d4fbd8a851115Physical review research[1] Thermodynamics in the Quantum Regime: Fundamental Aspects and New Directions, edited by F. Binder, L. A. Correa, C. Gogolin, J. Anders, and G. Adesso (Springer International, Cham, Swtizerland, 2018).[2] S. Deffner and S. Campbell, Quantum Thermodynamics - An Introduction to the Thermodynamics of Quantum Information (Morgan & Claypool, San Rafael, CA, 2019).[3] R. Kosloff, Quantum thermodynamics: A dynamical viewpoint, Entropy 15, 2100 (2013).[4] J. Goold, M. Huber, A. Riera, L. del Rio, and P. Skrzypczyk, The role of quantum information in thermodynamics - a topical review, J. Phys. A: Math. Theor. 49, 143001 (2016).[5] S. Vinjanampathy and J. Anders, Quantum thermodynamics, Contemp. Phys. 57, 545 (2016).[6] F. Brandão, M. Horodecki, N. Ng, J. Oppenheim, and S. Wehner, The second laws of quantum thermodynamics, Proc. Natl. Acad. Sci. USA 112, 3275 (2015).[7] G. E. Crooks, Entropy production fluctuation theorem and the nonequilibrium work relation for free energy differences, Phys. Rev. E 60, 2721 (1999).[8] C. Jarzynski, Nonequilibrium equality for free energy differences, Phys. Rev. Lett. 78, 2690 (1997).[9] M. Esposito, U. Harbola and S. Mukamel, Nonequilibrium fluctuations, fluctuation theorems, and counting statistics in quantum systems, Rev. Mod. Phys. 81, 1665 (2009).[10] M. Campisi, P. Hänggi, and P. Talkner, Quantum fluctuation relations: Foundations and applications, Rev. Mod. Phys. 83, 771 (2011).[11] M. Herrera, J. P. S. Peterson, R. M. Serra, and I. D’Amico, Easy access to energy fluctuations in nonequilibrium quantum manybody systems, Phys. Rev. Lett. 127, 030602 (2021).[12] A. Auffèves, Quantum technologies need a quantum energy initiative, Phys. Rev. X Quantum 3, 020101 (2022).[13] T. Hugel, N. B. Holland, A. Cattani, L. Moroder, M. Seitz, and H. E. Gaub, Single-molecule optomechanical cycle, Science 296, 1103 (2002).[14] P. G. Steeneken, K. Le Phan, M. J. Goossens, G. E. J. Koops, G. J. A. M. Brom, C. van der Avoort, and J. T. M. van Beek, Piezoresistive heat engine and refrigerator, Nat. Phys. 7, 354 (2011).[15] V. Blickle and C. Bechinger, Realization of a micrometresized stochastic heat engine, Nat. Phys. 8, 143 (2012).[16] J.-P. Brantut, C. Grenier, J. Meineke, D. Stadler, S. Krinner, C. Kollath, T. Esslinger, and A. Georges, A thermoelectric heat engine with ultracold atoms, Science 342, 713 (2013).[17] J. Roßnagel, O. Abah, F. Schmidt-Kaler, K. Singer, and E. Lutz, Nanoscale heat engine beyond the carnot limit, Phys. Rev. Lett. 112, 030602 (2014).[18] H. Thierschmann, R. Sánchez, B. Sothmann, F. Arnold, C. Heyn, W. Hansen, H. Buhmann, and L. W. Molenkamp, Threeterminal energy harvester with coupled quantum dots, Nat. Nanotechnol. 10, 854 (2015).[19] J. Roßsnagel, S. T. Dawkins, K. N. Tolazzi, O. Abah, E. Lutz, F. Schmidt-Kaler, and K. Singer, A single-atom heat engine, Science 352, 325 (2016).[20] F. Schmidt, A. Magazzú, A. Callegari, L. Biancofiore, F. Cichos, and G. Volpe, Microscopic engine powered by critical demixing, Phys. Rev. Lett. 120, 068004 (2018).[21] Y. Zou, Y. Jiang, Y. Mei, X. Guo, and S. 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