{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:52CJESBRV6BJM3QJFGGFFQGRFY","short_pith_number":"pith:52CJESBR","schema_version":"1.0","canonical_sha256":"ee84924831af82966e09298c52c0d12e063c79ff197f48507fe0300ab14e7bd3","source":{"kind":"arxiv","id":"2502.17551","version":2},"attestation_state":"computed","paper":{"title":"Emergent Hydrodynamic Mode on SU(2) Plaquette Chains and Quantum Simulation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","hep-lat","nucl-th","quant-ph"],"primary_cat":"hep-ph","authors_text":"Francesco Turro, Xiaojun Yao","submitted_at":"2025-02-24T19:00:00Z","abstract_excerpt":"We search for emergent hydrodynamic modes in real-time Hamiltonian dynamics of $2+1$-dimensional SU(2) lattice gauge theory on a quasi one dimensional plaquette chain, by numerically computing symmetric correlation functions of energy densities on lattice sizes of about $20$ with the local Hilbert space truncated at $j_{\\rm max}=\\frac{1}{2}$. Because of the Umklapp processes, we only find a mode for energy diffusion. The symmetric correlator exhibits transport peak near zero frequency with a width approximately proportional to momentum squared at small momentum, when the system is fully quantu"},"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":"2502.17551","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-02-24T19:00:00Z","cross_cats_sorted":["cond-mat.stat-mech","hep-lat","nucl-th","quant-ph"],"title_canon_sha256":"9afddaa2c8b4ef6b296b564be2fb30c1239b81b8e932bf02e6d8fb26836470ea","abstract_canon_sha256":"8292575dd9ee456a02e5d9df61ffcf0fd0cfa1d535e5ab29f0b614c7740fe2bc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:58:23.539070Z","signature_b64":"u9tr4itS76KcbQWPM/Q8LvEpAp3Mlk4j2SCJCwK/WndqeL3UDsIBx1Mj5hedSdaD+t04ARR59/ig85PFUkg5CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ee84924831af82966e09298c52c0d12e063c79ff197f48507fe0300ab14e7bd3","last_reissued_at":"2026-07-05T10:58:23.538495Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:58:23.538495Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Emergent Hydrodynamic Mode on SU(2) Plaquette Chains and Quantum Simulation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","hep-lat","nucl-th","quant-ph"],"primary_cat":"hep-ph","authors_text":"Francesco Turro, Xiaojun Yao","submitted_at":"2025-02-24T19:00:00Z","abstract_excerpt":"We search for emergent hydrodynamic modes in real-time Hamiltonian dynamics of $2+1$-dimensional SU(2) lattice gauge theory on a quasi one dimensional plaquette chain, by numerically computing symmetric correlation functions of energy densities on lattice sizes of about $20$ with the local Hilbert space truncated at $j_{\\rm max}=\\frac{1}{2}$. Because of the Umklapp processes, we only find a mode for energy diffusion. The symmetric correlator exhibits transport peak near zero frequency with a width approximately proportional to momentum squared at small momentum, when the system is fully quantu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.17551","kind":"arxiv","version":2},"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/2502.17551/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":"2502.17551","created_at":"2026-07-05T10:58:23.538561+00:00"},{"alias_kind":"arxiv_version","alias_value":"2502.17551v2","created_at":"2026-07-05T10:58:23.538561+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.17551","created_at":"2026-07-05T10:58:23.538561+00:00"},{"alias_kind":"pith_short_12","alias_value":"52CJESBRV6BJ","created_at":"2026-07-05T10:58:23.538561+00:00"},{"alias_kind":"pith_short_16","alias_value":"52CJESBRV6BJM3QJ","created_at":"2026-07-05T10:58:23.538561+00:00"},{"alias_kind":"pith_short_8","alias_value":"52CJESBR","created_at":"2026-07-05T10:58:23.538561+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.09984","citing_title":"Tame the Umklapp Processes in Real-Time Lattice Simulation for Hydrodynamics: An Ising Field Theory Study","ref_index":38,"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":64,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/52CJESBRV6BJM3QJFGGFFQGRFY","json":"https://pith.science/pith/52CJESBRV6BJM3QJFGGFFQGRFY.json","graph_json":"https://pith.science/api/pith-number/52CJESBRV6BJM3QJFGGFFQGRFY/graph.json","events_json":"https://pith.science/api/pith-number/52CJESBRV6BJM3QJFGGFFQGRFY/events.json","paper":"https://pith.science/paper/52CJESBR"},"agent_actions":{"view_html":"https://pith.science/pith/52CJESBRV6BJM3QJFGGFFQGRFY","download_json":"https://pith.science/pith/52CJESBRV6BJM3QJFGGFFQGRFY.json","view_paper":"https://pith.science/paper/52CJESBR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2502.17551&json=true","fetch_graph":"https://pith.science/api/pith-number/52CJESBRV6BJM3QJFGGFFQGRFY/graph.json","fetch_events":"https://pith.science/api/pith-number/52CJESBRV6BJM3QJFGGFFQGRFY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/52CJESBRV6BJM3QJFGGFFQGRFY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/52CJESBRV6BJM3QJFGGFFQGRFY/action/storage_attestation","attest_author":"https://pith.science/pith/52CJESBRV6BJM3QJFGGFFQGRFY/action/author_attestation","sign_citation":"https://pith.science/pith/52CJESBRV6BJM3QJFGGFFQGRFY/action/citation_signature","submit_replication":"https://pith.science/pith/52CJESBRV6BJM3QJFGGFFQGRFY/action/replication_record"}},"created_at":"2026-07-05T10:58:23.538561+00:00","updated_at":"2026-07-05T10:58:23.538561+00:00"}