Robert D. Delaney, Lucas R. Sletten, Matthew J. Cich, Brian Estey, Maya I. Fabrikant, David Hayes, Ian M. Hoffman, James Hostetter, Christopher Langer, Steven A. Moses, Abigail R. Perry, Timothy A. Peterson, Andrew Schaffer, Curtis Volin, Grahame Vittorini, William Cody Burton
{"title":"基于网格的表面电极陷阱中的可扩展多物种离子传输","authors":"Robert D. Delaney, Lucas R. Sletten, Matthew J. Cich, Brian Estey, Maya I. Fabrikant, David Hayes, Ian M. Hoffman, James Hostetter, Christopher Langer, Steven A. Moses, Abigail R. Perry, Timothy A. Peterson, Andrew Schaffer, Curtis Volin, Grahame Vittorini, William Cody Burton","doi":"10.1103/physrevx.14.041028","DOIUrl":null,"url":null,"abstract":"Quantum processors based on linear arrays of trapped ions have achieved exceptional performance, but scaling to large qubit numbers requires realizing two-dimensional ion arrays as envisioned in the quantum charge-coupled device (QCCD) architecture. Here, we present a scalable method for the control of ion crystals in a grid-based surface-electrode Paul trap and characterize it in the context of transport operations that sort and reorder multispecies crystals. By combining cowiring of control electrodes at translationally symmetric locations in each grid site with the sitewise ability to exchange the voltages applied to two special electrodes gated by a binary input, site-dependent operations can be achieved using only a fixed number of analog voltage signals and a single digital input per site. In two separate experimental systems containing nominally identical grid traps, one using <mjx-container ctxtmenu_counter=\"21\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" overflow=\"linebreak\" role=\"tree\" sre-explorer- style=\"font-size: 100.7%;\" tabindex=\"0\"><mjx-math data-semantic-structure=\"(17 (7 (2 0 1) 3 4 5 6) 8 (16 (11 9 10) 12 13 14 15))\"><mjx-mrow data-semantic-children=\"7,16\" data-semantic-content=\"8\" data-semantic- data-semantic-owns=\"7 8 16\" data-semantic-role=\"subtraction\" data-semantic-speech=\"Superscript 171 Baseline upper Y b Superscript plus minus Superscript 138 Baseline upper B a Superscript plus\" data-semantic-type=\"infixop\"><mjx-mmultiscripts data-semantic-children=\"2,3,4,5,6\" data-semantic-collapsed=\"(7 2 3 4 5 6)\" data-semantic- data-semantic-owns=\"2 3 4 5 6\" data-semantic-parent=\"17\" data-semantic-role=\"unknown\" data-semantic-type=\"tensor\"><mjx-prescripts style=\"vertical-align: 0.555em;\"><mjx-row><mjx-cell><mjx-mrow 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data-semantic-parent=\"17\" data-semantic-role=\"subtraction\" data-semantic-type=\"operator\" style='font-family: MJX-STX-ZERO, \"Helvetica Neue\", Helvetica, Roboto, Arial, sans-serif;'><mjx-utext style=\"font-size: 90.6%; padding: 0.828em 0px 0.221em; width: 7px;\" variant=\"-explicitFont\">−</mjx-utext></mjx-mtext><mjx-mmultiscripts data-semantic-children=\"11,12,13,14,15\" data-semantic-collapsed=\"(16 11 12 13 14 15)\" data-semantic- data-semantic-owns=\"11 12 13 14 15\" data-semantic-parent=\"17\" data-semantic-role=\"unknown\" data-semantic-type=\"tensor\"><mjx-prescripts style=\"vertical-align: 0.506em;\"><mjx-row><mjx-cell><mjx-mrow size=\"s\"><mjx-mn data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"16\" data-semantic-role=\"leftsuper\" data-semantic-type=\"number\"><mjx-c noic=\"true\" style=\"padding-top: 0.647em;\">1</mjx-c><mjx-c noic=\"true\" style=\"padding-top: 0.647em;\">3</mjx-c><mjx-c style=\"padding-top: 0.647em;\">8</mjx-c></mjx-mn></mjx-mrow></mjx-cell></mjx-row><mjx-row style=\"height: 0.743em;\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic- data-semantic-parent=\"16\" data-semantic-role=\"leftsub\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row></mjx-prescripts><mjx-mrow><mjx-msup data-semantic-children=\"9,10\" data-semantic- data-semantic-owns=\"9 10\" data-semantic-parent=\"16\" data-semantic-role=\"unknown\" data-semantic-type=\"superscript\"><mjx-mrow><mjx-mi data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"11\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\"><mjx-c noic=\"true\" style=\"padding-top: 0.657em;\">B</mjx-c><mjx-c style=\"padding-top: 0.657em;\">a</mjx-c></mjx-mi></mjx-mrow><mjx-script style=\"vertical-align: 0.384em;\"><mjx-mrow size=\"s\"><mjx-mo data-semantic- data-semantic-parent=\"11\" data-semantic-role=\"addition\" data-semantic-type=\"operator\"><mjx-c>+</mjx-c></mjx-mo></mjx-mrow></mjx-script></mjx-msup></mjx-mrow><mjx-scripts style=\"vertical-align: 0.506em;\"><mjx-row><mjx-cell><mjx-none data-semantic-added=\"true\" data-semantic- data-semantic-parent=\"16\" data-semantic-role=\"rightsuper\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row><mjx-row style=\"height: 0.753em;\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic-added=\"true\" data-semantic- data-semantic-parent=\"16\" data-semantic-role=\"rightsub\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row></mjx-scripts></mjx-mmultiscripts></mjx-mrow></mjx-math></mjx-container> crystals and the other <mjx-container ctxtmenu_counter=\"22\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" overflow=\"linebreak\" role=\"tree\" sre-explorer- style=\"font-size: 100.7%;\" tabindex=\"0\"><mjx-math data-semantic-structure=\"(17 (7 (2 0 1) 3 4 5 6) 8 (16 (11 9 10) 12 13 14 15))\"><mjx-mrow 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style=\"height: 0.743em;\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic- data-semantic-parent=\"7\" data-semantic-role=\"leftsub\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row></mjx-prescripts><mjx-mrow><mjx-msup data-semantic-children=\"0,1\" data-semantic- data-semantic-owns=\"0 1\" data-semantic-parent=\"7\" data-semantic-role=\"unknown\" data-semantic-type=\"superscript\"><mjx-mrow><mjx-mi data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"2\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\"><mjx-c noic=\"true\" style=\"padding-top: 0.657em;\">B</mjx-c><mjx-c style=\"padding-top: 0.657em;\">a</mjx-c></mjx-mi></mjx-mrow><mjx-script style=\"vertical-align: 0.384em;\"><mjx-mrow size=\"s\"><mjx-mo data-semantic- data-semantic-parent=\"2\" data-semantic-role=\"addition\" data-semantic-type=\"operator\"><mjx-c>+</mjx-c></mjx-mo></mjx-mrow></mjx-script></mjx-msup></mjx-mrow><mjx-scripts style=\"vertical-align: 0.506em;\"><mjx-row><mjx-cell><mjx-none data-semantic-added=\"true\" data-semantic- data-semantic-parent=\"7\" data-semantic-role=\"rightsuper\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row><mjx-row style=\"height: 0.753em;\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic-added=\"true\" data-semantic- data-semantic-parent=\"7\" data-semantic-role=\"rightsub\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row></mjx-scripts></mjx-mmultiscripts><mjx-mtext data-semantic-annotation=\"general:text\" data-semantic- data-semantic-operator=\"infixop,−\" data-semantic-parent=\"17\" data-semantic-role=\"subtraction\" data-semantic-type=\"operator\" style='font-family: MJX-STX-ZERO, \"Helvetica Neue\", Helvetica, Roboto, Arial, sans-serif;'><mjx-utext style=\"font-size: 90.6%; padding: 0.828em 0px 0.221em; width: 7px;\" variant=\"-explicitFont\">−</mjx-utext></mjx-mtext><mjx-mmultiscripts data-semantic-children=\"11,12,13,14,15\" data-semantic-collapsed=\"(16 11 12 13 14 15)\" data-semantic- data-semantic-owns=\"11 12 13 14 15\" data-semantic-parent=\"17\" data-semantic-role=\"unknown\" data-semantic-type=\"tensor\"><mjx-prescripts style=\"vertical-align: 0.518em;\"><mjx-row><mjx-cell><mjx-mrow size=\"s\"><mjx-mn data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"16\" data-semantic-role=\"leftsuper\" data-semantic-type=\"number\"><mjx-c noic=\"true\" style=\"padding-top: 0.647em;\">8</mjx-c><mjx-c style=\"padding-top: 0.647em;\">8</mjx-c></mjx-mn></mjx-mrow></mjx-cell></mjx-row><mjx-row style=\"height: 0.756em;\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic- data-semantic-parent=\"16\" data-semantic-role=\"leftsub\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row></mjx-prescripts><mjx-mrow><mjx-msup data-semantic-children=\"9,10\" data-semantic- data-semantic-owns=\"9 10\" data-semantic-parent=\"16\" data-semantic-role=\"unknown\" data-semantic-type=\"superscript\"><mjx-mrow><mjx-mi data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"11\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\"><mjx-c noic=\"true\" style=\"padding-top: 0.669em;\">S</mjx-c><mjx-c style=\"padding-top: 0.669em;\">r</mjx-c></mjx-mi></mjx-mrow><mjx-script style=\"vertical-align: 0.396em;\"><mjx-mrow size=\"s\"><mjx-mo data-semantic- data-semantic-parent=\"11\" data-semantic-role=\"addition\" data-semantic-type=\"operator\"><mjx-c>+</mjx-c></mjx-mo></mjx-mrow></mjx-script></mjx-msup></mjx-mrow><mjx-scripts style=\"vertical-align: 0.518em;\"><mjx-row><mjx-cell><mjx-none data-semantic-added=\"true\" data-semantic- data-semantic-parent=\"16\" data-semantic-role=\"rightsuper\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row><mjx-row style=\"height: 0.765em;\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic-added=\"true\" data-semantic- data-semantic-parent=\"16\" data-semantic-role=\"rightsub\" data-semantic-type=\"empty\" size=\"s\"></mjx-none></mjx-cell></mjx-row></mjx-scripts></mjx-mmultiscripts></mjx-mrow></mjx-math></mjx-container>, we demonstrate this method by characterizing the conditional intrasite crystal reorder and the conditional exchange of ions between adjacent sites on the grid. Averaged across a multisite region of interest, we measure subquanta motional excitation in the axial in-phase and out-of-phase modes of the crystals following these operations at exchange rates of 2.5 kHz. In this initial demonstration, the logic controlling the voltage exchange occurs in software, but the applied signals mimic a proposed hardware implementation using crossover switches. These techniques can be further extended to implement other conditional operations in the QCCD architecture such as gates, initialization, and measurement.","PeriodicalId":20161,"journal":{"name":"Physical Review X","volume":"16 1","pages":""},"PeriodicalIF":11.6000,"publicationDate":"2024-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Scalable Multispecies Ion Transport in a Grid-Based Surface-Electrode Trap\",\"authors\":\"Robert D. Delaney, Lucas R. Sletten, Matthew J. Cich, Brian Estey, Maya I. Fabrikant, David Hayes, Ian M. Hoffman, James Hostetter, Christopher Langer, Steven A. Moses, Abigail R. Perry, Timothy A. Peterson, Andrew Schaffer, Curtis Volin, Grahame Vittorini, William Cody Burton\",\"doi\":\"10.1103/physrevx.14.041028\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Quantum processors based on linear arrays of trapped ions have achieved exceptional performance, but scaling to large qubit numbers requires realizing two-dimensional ion arrays as envisioned in the quantum charge-coupled device (QCCD) architecture. Here, we present a scalable method for the control of ion crystals in a grid-based surface-electrode Paul trap and characterize it in the context of transport operations that sort and reorder multispecies crystals. By combining cowiring of control electrodes at translationally symmetric locations in each grid site with the sitewise ability to exchange the voltages applied to two special electrodes gated by a binary input, site-dependent operations can be achieved using only a fixed number of analog voltage signals and a single digital input per site. In two separate experimental systems containing nominally identical grid traps, one using <mjx-container ctxtmenu_counter=\\\"21\\\" ctxtmenu_oldtabindex=\\\"1\\\" jax=\\\"CHTML\\\" overflow=\\\"linebreak\\\" role=\\\"tree\\\" sre-explorer- style=\\\"font-size: 100.7%;\\\" tabindex=\\\"0\\\"><mjx-math data-semantic-structure=\\\"(17 (7 (2 0 1) 3 4 5 6) 8 (16 (11 9 10) 12 13 14 15))\\\"><mjx-mrow data-semantic-children=\\\"7,16\\\" data-semantic-content=\\\"8\\\" data-semantic- data-semantic-owns=\\\"7 8 16\\\" data-semantic-role=\\\"subtraction\\\" data-semantic-speech=\\\"Superscript 171 Baseline upper Y b Superscript plus minus Superscript 138 Baseline upper B a Superscript plus\\\" data-semantic-type=\\\"infixop\\\"><mjx-mmultiscripts data-semantic-children=\\\"2,3,4,5,6\\\" data-semantic-collapsed=\\\"(7 2 3 4 5 6)\\\" data-semantic- data-semantic-owns=\\\"2 3 4 5 6\\\" data-semantic-parent=\\\"17\\\" data-semantic-role=\\\"unknown\\\" data-semantic-type=\\\"tensor\\\"><mjx-prescripts style=\\\"vertical-align: 0.555em;\\\"><mjx-row><mjx-cell><mjx-mrow size=\\\"s\\\"><mjx-mn data-semantic-font=\\\"normal\\\" data-semantic- data-semantic-parent=\\\"7\\\" data-semantic-role=\\\"leftsuper\\\" data-semantic-type=\\\"number\\\"><mjx-c noic=\\\"true\\\" style=\\\"padding-top: 0.639em;\\\">1</mjx-c><mjx-c noic=\\\"true\\\" style=\\\"padding-top: 0.639em;\\\">7</mjx-c><mjx-c style=\\\"padding-top: 0.639em;\\\">1</mjx-c></mjx-mn></mjx-mrow></mjx-cell></mjx-row><mjx-row style=\\\"height: 0.796em;\\\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic- data-semantic-parent=\\\"7\\\" data-semantic-role=\\\"leftsub\\\" data-semantic-type=\\\"empty\\\" size=\\\"s\\\"></mjx-none></mjx-cell></mjx-row></mjx-prescripts><mjx-mrow><mjx-msup data-semantic-children=\\\"0,1\\\" data-semantic- data-semantic-owns=\\\"0 1\\\" data-semantic-parent=\\\"7\\\" data-semantic-role=\\\"unknown\\\" 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data-semantic-added=\\\"true\\\" data-semantic- data-semantic-parent=\\\"7\\\" data-semantic-role=\\\"rightsub\\\" data-semantic-type=\\\"empty\\\" size=\\\"s\\\"></mjx-none></mjx-cell></mjx-row></mjx-scripts></mjx-mmultiscripts><mjx-mtext data-semantic-annotation=\\\"general:text\\\" data-semantic- data-semantic-operator=\\\"infixop,−\\\" data-semantic-parent=\\\"17\\\" data-semantic-role=\\\"subtraction\\\" data-semantic-type=\\\"operator\\\" style='font-family: MJX-STX-ZERO, \\\"Helvetica Neue\\\", Helvetica, Roboto, Arial, sans-serif;'><mjx-utext style=\\\"font-size: 90.6%; padding: 0.828em 0px 0.221em; width: 7px;\\\" variant=\\\"-explicitFont\\\">−</mjx-utext></mjx-mtext><mjx-mmultiscripts data-semantic-children=\\\"11,12,13,14,15\\\" data-semantic-collapsed=\\\"(16 11 12 13 14 15)\\\" data-semantic- data-semantic-owns=\\\"11 12 13 14 15\\\" data-semantic-parent=\\\"17\\\" data-semantic-role=\\\"unknown\\\" data-semantic-type=\\\"tensor\\\"><mjx-prescripts style=\\\"vertical-align: 0.506em;\\\"><mjx-row><mjx-cell><mjx-mrow size=\\\"s\\\"><mjx-mn data-semantic-font=\\\"normal\\\" data-semantic- data-semantic-parent=\\\"16\\\" data-semantic-role=\\\"leftsuper\\\" data-semantic-type=\\\"number\\\"><mjx-c noic=\\\"true\\\" style=\\\"padding-top: 0.647em;\\\">1</mjx-c><mjx-c noic=\\\"true\\\" style=\\\"padding-top: 0.647em;\\\">3</mjx-c><mjx-c style=\\\"padding-top: 0.647em;\\\">8</mjx-c></mjx-mn></mjx-mrow></mjx-cell></mjx-row><mjx-row style=\\\"height: 0.743em;\\\"></mjx-row><mjx-row><mjx-cell><mjx-none data-semantic- data-semantic-parent=\\\"16\\\" data-semantic-role=\\\"leftsub\\\" data-semantic-type=\\\"empty\\\" size=\\\"s\\\"></mjx-none></mjx-cell></mjx-row></mjx-prescripts><mjx-mrow><mjx-msup data-semantic-children=\\\"9,10\\\" data-semantic- data-semantic-owns=\\\"9 10\\\" data-semantic-parent=\\\"16\\\" data-semantic-role=\\\"unknown\\\" data-semantic-type=\\\"superscript\\\"><mjx-mrow><mjx-mi data-semantic-font=\\\"normal\\\" 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data-semantic-type=\\\"empty\\\" size=\\\"s\\\"></mjx-none></mjx-cell></mjx-row></mjx-scripts></mjx-mmultiscripts></mjx-mrow></mjx-math></mjx-container>, we demonstrate this method by characterizing the conditional intrasite crystal reorder and the conditional exchange of ions between adjacent sites on the grid. Averaged across a multisite region of interest, we measure subquanta motional excitation in the axial in-phase and out-of-phase modes of the crystals following these operations at exchange rates of 2.5 kHz. In this initial demonstration, the logic controlling the voltage exchange occurs in software, but the applied signals mimic a proposed hardware implementation using crossover switches. These techniques can be further extended to implement other conditional operations in the QCCD architecture such as gates, initialization, and measurement.\",\"PeriodicalId\":20161,\"journal\":{\"name\":\"Physical Review X\",\"volume\":\"16 1\",\"pages\":\"\"},\"PeriodicalIF\":11.6000,\"publicationDate\":\"2024-11-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physical Review X\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1103/physrevx.14.041028\",\"RegionNum\":1,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"PHYSICS, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical Review X","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevx.14.041028","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
Scalable Multispecies Ion Transport in a Grid-Based Surface-Electrode Trap
Quantum processors based on linear arrays of trapped ions have achieved exceptional performance, but scaling to large qubit numbers requires realizing two-dimensional ion arrays as envisioned in the quantum charge-coupled device (QCCD) architecture. Here, we present a scalable method for the control of ion crystals in a grid-based surface-electrode Paul trap and characterize it in the context of transport operations that sort and reorder multispecies crystals. By combining cowiring of control electrodes at translationally symmetric locations in each grid site with the sitewise ability to exchange the voltages applied to two special electrodes gated by a binary input, site-dependent operations can be achieved using only a fixed number of analog voltage signals and a single digital input per site. In two separate experimental systems containing nominally identical grid traps, one using 171Yb+−138Ba+ crystals and the other 137Ba+−88Sr+, we demonstrate this method by characterizing the conditional intrasite crystal reorder and the conditional exchange of ions between adjacent sites on the grid. Averaged across a multisite region of interest, we measure subquanta motional excitation in the axial in-phase and out-of-phase modes of the crystals following these operations at exchange rates of 2.5 kHz. In this initial demonstration, the logic controlling the voltage exchange occurs in software, but the applied signals mimic a proposed hardware implementation using crossover switches. These techniques can be further extended to implement other conditional operations in the QCCD architecture such as gates, initialization, and measurement.
期刊介绍:
Physical Review X (PRX) stands as an exclusively online, fully open-access journal, emphasizing innovation, quality, and enduring impact in the scientific content it disseminates. Devoted to showcasing a curated selection of papers from pure, applied, and interdisciplinary physics, PRX aims to feature work with the potential to shape current and future research while leaving a lasting and profound impact in their respective fields. Encompassing the entire spectrum of physics subject areas, PRX places a special focus on groundbreaking interdisciplinary research with broad-reaching influence.