Energy Consumption for Ion-Transport in a Segmented Paul Trap
There is recent interest in determining energy costs of shortcuts to adiabaticity (STA), but different definitions of ' cost' have been used. Wedemonstrate the importance of taking into account the control system (CS) for a fair assessment of energy flows and consumptions. Wemodel the ener...
| Autores: | , , |
|---|---|
| Tipo de recurso: | artículo |
| Fecha de publicación: | 2018 |
| País: | España |
| Institución: | Universidad del País Vasco |
| Repositorio: | Addi. Archivo Digital para la Docencia y la Investigación |
| OAI Identifier: | oai:addi.ehu.eus:10810/30256 |
| Acceso en línea: | http://hdl.handle.net/10810/30256 |
| Access Level: | acceso abierto |
| Palabra clave: | quantum control quantum thermodynamics shortcuts to adiabaticity quantum adiabaticity shortcuts dynamics |
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Energy Consumption for Ion-Transport in a Segmented Paul TrapTobalina Novo, AnderAlonso, JosebaMuga Francisco, Juan Gonzaloquantum controlquantum thermodynamicsshortcuts to adiabaticityquantumadiabaticityshortcutsdynamicsThere is recent interest in determining energy costs of shortcuts to adiabaticity (STA), but different definitions of ' cost' have been used. Wedemonstrate the importance of taking into account the control system (CS) for a fair assessment of energy flows and consumptions. Wemodel the energy consumption and power to transport an ion by a STA protocol in a multisegmented Paul trap. The ion is driven by an externally controlled, moving harmonic oscillator. Even if no net ion-energy is gained at destination, setting the time-dependent control parameters is a macroscopic operation that costs energy and results in energy dissipation for the short time scales implied by the intrinsically fast STA processes. The potential minimum is displaced by modulating the voltages on control (dc) electrodes. Asecondary effect of the modulation, usually ignored as it does not affect the ion dynamics, is the time-dependent energy shift of the potential minimum. The non trivial part of the energy consumption is due to the electromotive forces to set the electrode voltages through the low-pass filters required to preserve the electronic noise from decohering the ion's motion. The results for the macroscopic CS (the Paul trap) are compared to the microscopic power and energy of the ion alone. Similarities are found-and may be used quantitatively to minimize costs-only when the CS-dependent energy shift of the harmonic oscillator is included in the ion-energy.We thank Kihwan Kim for discussions. Weacknowledge funding by the Basque Government (Grant No. IT98616) and MINECO/FEDER, UE (Grant No. FIS2015-67161-P). The research is based upon work supported by the Office of the Director of National Intelligence (ODNI), Intelligence Advanced Research Projects Activity (IARPA), via the U.S. Army Research Office grant W911NF-16-1-0070. The views and conclusions contained herein are those of the authors and should not be interpreted as necessarily representing the official policies or endorsements, either expressed or implied, of the ODNI, IARPA, or the US Government. Any opinions, findings, and conclusions or recommendations expressed in this material are those of the author(s) and do not necessarily reflect the view of the US Army Research Office.IOP Publishing LTD201820182018info:eu-repo/semantics/articleapplication/pdfhttp://hdl.handle.net/10810/30256reponame:Addi. Archivo Digital para la Docencia y la Investigacióninstname:Universidad del País VascoInglésinfo:eu-repo/grantAgreement/MINECO/FIS2015-67161-P/http://iopscience.iop.org/article/10.1088/1367-2630/aac685/pdfinfo:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by/3.0/es/Attribution 3.0 Unported (CC BY 3.0) You are free to: Share — copy and redistribute the material in any medium or format Adapt — remix, transform, and build upon the material for any purpose, even commercially.Atribución 3.0 Españaoai:addi.ehu.eus:10810/302562026-06-18T09:23:17Z |
| dc.title.none.fl_str_mv |
Energy Consumption for Ion-Transport in a Segmented Paul Trap |
| title |
Energy Consumption for Ion-Transport in a Segmented Paul Trap |
| spellingShingle |
Energy Consumption for Ion-Transport in a Segmented Paul Trap Tobalina Novo, Ander quantum control quantum thermodynamics shortcuts to adiabaticity quantum adiabaticity shortcuts dynamics |
| title_short |
Energy Consumption for Ion-Transport in a Segmented Paul Trap |
| title_full |
Energy Consumption for Ion-Transport in a Segmented Paul Trap |
| title_fullStr |
Energy Consumption for Ion-Transport in a Segmented Paul Trap |
| title_full_unstemmed |
Energy Consumption for Ion-Transport in a Segmented Paul Trap |
| title_sort |
Energy Consumption for Ion-Transport in a Segmented Paul Trap |
| dc.creator.none.fl_str_mv |
Tobalina Novo, Ander Alonso, Joseba Muga Francisco, Juan Gonzalo |
| author |
Tobalina Novo, Ander |
| author_facet |
Tobalina Novo, Ander Alonso, Joseba Muga Francisco, Juan Gonzalo |
| author_role |
author |
| author2 |
Alonso, Joseba Muga Francisco, Juan Gonzalo |
| author2_role |
author author |
| dc.subject.none.fl_str_mv |
quantum control quantum thermodynamics shortcuts to adiabaticity quantum adiabaticity shortcuts dynamics |
| topic |
quantum control quantum thermodynamics shortcuts to adiabaticity quantum adiabaticity shortcuts dynamics |
| description |
There is recent interest in determining energy costs of shortcuts to adiabaticity (STA), but different definitions of ' cost' have been used. Wedemonstrate the importance of taking into account the control system (CS) for a fair assessment of energy flows and consumptions. Wemodel the energy consumption and power to transport an ion by a STA protocol in a multisegmented Paul trap. The ion is driven by an externally controlled, moving harmonic oscillator. Even if no net ion-energy is gained at destination, setting the time-dependent control parameters is a macroscopic operation that costs energy and results in energy dissipation for the short time scales implied by the intrinsically fast STA processes. The potential minimum is displaced by modulating the voltages on control (dc) electrodes. Asecondary effect of the modulation, usually ignored as it does not affect the ion dynamics, is the time-dependent energy shift of the potential minimum. The non trivial part of the energy consumption is due to the electromotive forces to set the electrode voltages through the low-pass filters required to preserve the electronic noise from decohering the ion's motion. The results for the macroscopic CS (the Paul trap) are compared to the microscopic power and energy of the ion alone. Similarities are found-and may be used quantitatively to minimize costs-only when the CS-dependent energy shift of the harmonic oscillator is included in the ion-energy. |
| publishDate |
2018 |
| dc.date.none.fl_str_mv |
2018 2018 2018 |
| dc.type.none.fl_str_mv |
info:eu-repo/semantics/article |
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article |
| dc.identifier.none.fl_str_mv |
http://hdl.handle.net/10810/30256 |
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http://hdl.handle.net/10810/30256 |
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Inglés |
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Inglés |
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info:eu-repo/grantAgreement/MINECO/FIS2015-67161-P/ http://iopscience.iop.org/article/10.1088/1367-2630/aac685/pdf |
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info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/3.0/es/ Atribución 3.0 España |
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openAccess |
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http://creativecommons.org/licenses/by/3.0/es/ Atribución 3.0 España |
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application/pdf |
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IOP Publishing LTD |
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IOP Publishing LTD |
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reponame:Addi. Archivo Digital para la Docencia y la Investigación instname:Universidad del País Vasco |
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Universidad del País Vasco |
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