{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:6N4GL2MDLVNXLXU4MPSZFT5TWC","short_pith_number":"pith:6N4GL2MD","schema_version":"1.0","canonical_sha256":"f37865e9835d5b75de9c63e592cfb3b0b0b82fabf923534d03407c42e0e3b98a","source":{"kind":"arxiv","id":"2410.13815","version":1},"attestation_state":"computed","paper":{"title":"Observation of string-breaking dynamics in a quantum simulator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","hep-lat","hep-ph","nucl-th"],"primary_cat":"quant-ph","authors_text":"Alessio Lerose, Alexander Schuckert, Alexey V. Gorshkov, Arinjoy De, Brayden Ware, Christopher Monroe, De Luo, Elizabeth R. Bennewitz, Federica M. Surace, Kate S. Collins, Or Katz, William Morong, Zohreh Davoudi","submitted_at":"2024-10-17T17:46:07Z","abstract_excerpt":"Spontaneous particle-pair formation is a fundamental phenomenon in nature. It can, for example, appear when the potential energy between two particles increases with separation, as if they were connected by a tense string. Beyond a critical separation, new particle pairs can form, causing the string to break. String-breaking dynamics in quantum chromodynamics play a vital role in high-energy particle collisions and early universe evolution. Simulating string evolution and hadron formation is, therefore, a grand challenge in modern physics. Quantum simulators, well-suited for studying dynamics,"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2410.13815","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2024-10-17T17:46:07Z","cross_cats_sorted":["cond-mat.quant-gas","hep-lat","hep-ph","nucl-th"],"title_canon_sha256":"43b48326effc4a3d7b8afaf2dbee31d4f22dab4aefadadb8a1ad069e52e38076","abstract_canon_sha256":"7fba7de908864cf7d9bb415c5d6e60e1ecfece7d7949a447687215c469bd9f66"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:22:06.143366Z","signature_b64":"WSkcHKyh5HFpRt4ynk3dWVN3tNYYVsE0k407QaTJhFry1vrg2bMf5BoXBCbnVhb/7NYHw7gM1NlWo12FUd3VCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f37865e9835d5b75de9c63e592cfb3b0b0b82fabf923534d03407c42e0e3b98a","last_reissued_at":"2026-07-05T09:22:06.142872Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:22:06.142872Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Observation of string-breaking dynamics in a quantum simulator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","hep-lat","hep-ph","nucl-th"],"primary_cat":"quant-ph","authors_text":"Alessio Lerose, Alexander Schuckert, Alexey V. Gorshkov, Arinjoy De, Brayden Ware, Christopher Monroe, De Luo, Elizabeth R. Bennewitz, Federica M. Surace, Kate S. Collins, Or Katz, William Morong, Zohreh Davoudi","submitted_at":"2024-10-17T17:46:07Z","abstract_excerpt":"Spontaneous particle-pair formation is a fundamental phenomenon in nature. It can, for example, appear when the potential energy between two particles increases with separation, as if they were connected by a tense string. Beyond a critical separation, new particle pairs can form, causing the string to break. String-breaking dynamics in quantum chromodynamics play a vital role in high-energy particle collisions and early universe evolution. Simulating string evolution and hadron formation is, therefore, a grand challenge in modern physics. Quantum simulators, well-suited for studying dynamics,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2410.13815","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2410.13815/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2410.13815","created_at":"2026-07-05T09:22:06.142931+00:00"},{"alias_kind":"arxiv_version","alias_value":"2410.13815v1","created_at":"2026-07-05T09:22:06.142931+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2410.13815","created_at":"2026-07-05T09:22:06.142931+00:00"},{"alias_kind":"pith_short_12","alias_value":"6N4GL2MDLVNX","created_at":"2026-07-05T09:22:06.142931+00:00"},{"alias_kind":"pith_short_16","alias_value":"6N4GL2MDLVNXLXU4","created_at":"2026-07-05T09:22:06.142931+00:00"},{"alias_kind":"pith_short_8","alias_value":"6N4GL2MD","created_at":"2026-07-05T09:22:06.142931+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":16,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.07143","citing_title":"Hints for string breaking in QCD","ref_index":45,"is_internal_anchor":true},{"citing_arxiv_id":"2605.22915","citing_title":"Unified resonant-manifold framework for dynamical quantum phase transitions","ref_index":167,"is_internal_anchor":false},{"citing_arxiv_id":"2605.22915","citing_title":"Unified resonant-manifold framework for dynamical quantum phase transitions","ref_index":157,"is_internal_anchor":false},{"citing_arxiv_id":"2505.04704","citing_title":"Disorder-Free Localization and Fragmentation in a Non-Abelian Lattice Gauge Theory","ref_index":21,"is_internal_anchor":false},{"citing_arxiv_id":"2605.20417","citing_title":"Quantum Simulation of Gauge Theories for Particle and Nuclear Physics","ref_index":52,"is_internal_anchor":false},{"citing_arxiv_id":"2604.24896","citing_title":"Tightening energy-based boson truncation bound using Monte Carlo-assisted methods","ref_index":86,"is_internal_anchor":false},{"citing_arxiv_id":"2512.05210","citing_title":"A Framework for Quantum Simulations of Energy-Loss and Hadronization in Non-Abelian Gauge Theories: SU(2) Lattice Gauge Theory in 1+1D","ref_index":96,"is_internal_anchor":false},{"citing_arxiv_id":"2601.08825","citing_title":"The Quantum Complexity of String Breaking in the Schwinger Model","ref_index":42,"is_internal_anchor":false},{"citing_arxiv_id":"2602.02344","citing_title":"Large Nc Truncations for SU(Nc) Lattice Yang-Mills Theory with Fermions","ref_index":128,"is_internal_anchor":false},{"citing_arxiv_id":"2604.24896","citing_title":"Tightening energy-based boson truncation bound using Monte Carlo-assisted methods","ref_index":86,"is_internal_anchor":false},{"citing_arxiv_id":"2603.23948","citing_title":"Local Thermalization of SU(2) Lattice Gauge Fields on Quantum Computers","ref_index":102,"is_internal_anchor":false},{"citing_arxiv_id":"2604.24896","citing_title":"Tightening energy-based boson truncation bound using Monte Carlo-assisted methods","ref_index":86,"is_internal_anchor":false},{"citing_arxiv_id":"2605.05841","citing_title":"Non-Abelian String-Breaking Dynamics on a Qudit Quantum Computer","ref_index":21,"is_internal_anchor":false},{"citing_arxiv_id":"2605.04210","citing_title":"Nonlocal Nonstabilizerness from Holographic Schwinger Pair Production","ref_index":58,"is_internal_anchor":false},{"citing_arxiv_id":"2604.07435","citing_title":"Observation of glueball excitations and string breaking in a $2+1$D $\\mathbb{Z}_2$ lattice gauge theory on a trapped-ion quantum computer","ref_index":145,"is_internal_anchor":false},{"citing_arxiv_id":"2604.07436","citing_title":"Observation of genuine $2+1$D string dynamics in a U$(1)$ lattice gauge theory with a tunable plaquette term on a trapped-ion quantum computer","ref_index":139,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6N4GL2MDLVNXLXU4MPSZFT5TWC","json":"https://pith.science/pith/6N4GL2MDLVNXLXU4MPSZFT5TWC.json","graph_json":"https://pith.science/api/pith-number/6N4GL2MDLVNXLXU4MPSZFT5TWC/graph.json","events_json":"https://pith.science/api/pith-number/6N4GL2MDLVNXLXU4MPSZFT5TWC/events.json","paper":"https://pith.science/paper/6N4GL2MD"},"agent_actions":{"view_html":"https://pith.science/pith/6N4GL2MDLVNXLXU4MPSZFT5TWC","download_json":"https://pith.science/pith/6N4GL2MDLVNXLXU4MPSZFT5TWC.json","view_paper":"https://pith.science/paper/6N4GL2MD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2410.13815&json=true","fetch_graph":"https://pith.science/api/pith-number/6N4GL2MDLVNXLXU4MPSZFT5TWC/graph.json","fetch_events":"https://pith.science/api/pith-number/6N4GL2MDLVNXLXU4MPSZFT5TWC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6N4GL2MDLVNXLXU4MPSZFT5TWC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6N4GL2MDLVNXLXU4MPSZFT5TWC/action/storage_attestation","attest_author":"https://pith.science/pith/6N4GL2MDLVNXLXU4MPSZFT5TWC/action/author_attestation","sign_citation":"https://pith.science/pith/6N4GL2MDLVNXLXU4MPSZFT5TWC/action/citation_signature","submit_replication":"https://pith.science/pith/6N4GL2MDLVNXLXU4MPSZFT5TWC/action/replication_record"}},"created_at":"2026-07-05T09:22:06.142931+00:00","updated_at":"2026-07-05T09:22:06.142931+00:00"}