{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2026,9,29]],"date-time":"2026-09-29T21:21:02Z","timestamp":1790716862977,"version":"4.1.0"},"reference-count":85,"publisher":"American Physical Society (APS)","issue":"1","license":[{"start":{"date-parts":[[2025,7,1]],"date-time":"2025-07-01T00:00:00Z","timestamp":1751328000000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0\/"}],"funder":[{"DOI":"10.13039\/100010665","name":"H2020 Marie Sk\u0142odowska-Curie Actions","doi-asserted-by":"publisher","award":["101034413"],"award-info":[{"award-number":["101034413"]}],"id":[{"id":"10.13039\/100010665","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/100000001","name":"National Science Foundation","doi-asserted-by":"publisher","award":["DMR-2143635"],"award-info":[{"award-number":["DMR-2143635"]}],"id":[{"id":"10.13039\/100000001","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100001659","name":"Deutsche Forschungsgemeinschaft","doi-asserted-by":"publisher","award":["HA 8206\/1-1.s"],"award-info":[{"award-number":["HA 8206\/1-1.s"]}],"id":[{"id":"10.13039\/501100001659","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100004189","name":"Max-Planck-Gesellschaft","doi-asserted-by":"publisher","id":[{"id":"10.13039\/501100004189","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100000781","name":"European Research Council","doi-asserted-by":"publisher","award":["101165667"],"award-info":[{"award-number":["101165667"]}],"id":[{"id":"10.13039\/501100000781","id-type":"DOI","asserted-by":"publisher"}]}],"content-domain":{"domain":["journals.aps.org"],"crossmark-restriction":true},"short-container-title":["Phys. Rev. B"],"accepted":{"date-parts":[[2025,6,13]]},"abstract":"<jats:p>\n                    Confinement is a prominent phenomenon in condensed-matter and high-energy physics that has recently become the focus of quantum-simulation experiments of lattice gauge theories (LGTs). As such, a theoretical understanding of the effect of confinement on LGT dynamics is not only of fundamental importance but also can lend itself to upcoming experiments. Here we show how confinement in a\n                    <a:math xmlns:a=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                      <a:msub>\n                        <a:mi mathvariant=\"double-struck\">Z<\/a:mi>\n                        <a:mn>2<\/a:mn>\n                      <\/a:msub>\n                    <\/a:math>\n                    LGT can be  avoided by proximity to a resonance between the fermion mass and the electric field strength. Furthermore, we show that this local deconfinement can become global for certain initial conditions, where information transport occurs over the entire chain. In addition, we show how this can lead to strong quantum many-body scarring starting in different initial states. Our findings provide deeper insights into the nature of confinement in\n                    <c:math xmlns:c=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                      <c:msub>\n                        <c:mi mathvariant=\"double-struck\">Z<\/c:mi>\n                        <c:mn>2<\/c:mn>\n                      <\/c:msub>\n                    <\/c:math>\n                    LGTs and can be tested on current and near-term quantum devices.\n                  <\/jats:p>","DOI":"10.1103\/mfg2-t6gb","type":"journal-article","created":{"date-parts":[[2025,6,13]],"date-time":"2025-06-13T11:29:37Z","timestamp":1749814177000},"update-policy":"https:\/\/doi.org\/10.1103\/crossmark-policy","source":"Crossref","is-referenced-by-count":6,"title":["Mass-assisted local deconfinement in a confined\n                    <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                      <mml:msub>\n                        <mml:mi mathvariant=\"double-struck\">Z<\/mml:mi>\n                        <mml:mn>2<\/mml:mn>\n                      <\/mml:msub>\n                    <\/mml:math>\n                    lattice gauge theory"],"prefix":"10.1103","volume":"112","author":[{"ORCID":"https:\/\/orcid.org\/0000-0002-3749-6375","authenticated-orcid":true,"given":"Jean-Yves","family":"Desaules","sequence":"first","affiliation":[{"id":[{"id":"https:\/\/ror.org\/03gnh5541","id-type":"ROR","asserted-by":"publisher"}],"name":"Institute of Science and Technology Austria"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-5145-6441","authenticated-orcid":true,"given":"Thomas","family":"Iadecola","sequence":"additional","affiliation":[{"id":[{"id":"https:\/\/ror.org\/04rswrd78","id-type":"ROR","asserted-by":"publisher"}],"name":"Iowa State University"},{"id":[{"id":"https:\/\/ror.org\/041m9xr71","id-type":"ROR","asserted-by":"publisher"}],"name":"Ames National Laboratory"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-0659-7990","authenticated-orcid":true,"given":"Jad C.","family":"Halimeh","sequence":"additional","affiliation":[{"id":[{"id":"https:\/\/ror.org\/05591te55","id-type":"ROR","asserted-by":"publisher"}],"name":"Ludwig-Maximilians-Universit\u00e4t M\u00fcnchen"},{"id":[{"id":"https:\/\/ror.org\/04xrcta15","id-type":"ROR","asserted-by":"publisher"}],"name":"Munich Center for Quantum Science and Technology"},{"id":[{"id":"https:\/\/ror.org\/046ak2485","id-type":"ROR","asserted-by":"publisher"}],"name":"Freie Universit\u00e4t Berlin"}],"role":[{"vocabulary":"crossref","role":"author"}]}],"member":"16","published-online":{"date-parts":[[2025,7,1]]},"reference":[{"key":"mfg2-t6gbCc1R1","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.10.2445","type":"journal-article"},{"key":"mfg2-t6gbCc2R1","doi-asserted-by":"crossref","DOI":"10.1142\/5674","type":"book","volume-title":"Lattice Gauge Theories: An Introduction","author":"H.\u00a0J. 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When an even site j is \u2193, this allows the term P\u0302jZ\u0302j+1Q\u0302j+2 to be +1. But at the same time, the odd site k=j+3 is \u2191, allowing Q\u0302kZ\u0302k+1P\u0302k+2 to be \u22121. 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All rights are reserved, including those for text and data mining, AI training, and similar technologies.","name":"copyright_statement","label":"Copyright statement","group":{"name":"copyright","label":"copyright"}},{"value":"2025","name":"copyright_year","label":"Copyright year","group":{"name":"copyright","label":"copyright"}},{"value":"https:\/\/creativecommons.org\/licenses\/by\/4.0\/","name":"creative_commons_license","label":"Creative Commons license","group":{"name":"licenses","label":"Licenses"}},{"value":"\u00a92025 The authors","name":"copyright_holder","label":"Copyright holder","group":{"name":"copyright","label":"copyright"}}],"article-number":"014301"}}