{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:4TAMZFDNNRUG4U64GBVT3PT5EK","short_pith_number":"pith:4TAMZFDN","schema_version":"1.0","canonical_sha256":"e4c0cc946d6c686e53dc306b3dbe7d228d144f6715ac3fb04c0f43815638ce80","source":{"kind":"arxiv","id":"2607.22288","version":1},"attestation_state":"computed","paper":{"title":"Understanding interaction-driven transport in flux lattices with evolution-path symmetry","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["cond-mat.str-el","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Jian-Song Pan, Wei Yi, Xiaofan Zhou","submitted_at":"2026-07-24T13:25:32Z","abstract_excerpt":"The destruction of Aharonov-Bohm (AB) caging by interaction and the emergence of interaction-induced chiral currents in flux lattices are two paradigmatic examples of interaction-driven quantum transport. While various mechanisms, such as bound-state formation and chiral spectral imbalance, have been proposed, a unifying physical picture remains elusive. Here, we employ the concept of \\textit{evolution-path symmetry} (EPS) and its interaction-induced breaking as a framework to understand interaction-induced delocalization in flux lattices. EPS is defined as the invariance of a path's contribut"},"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":"2607.22288","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2026-07-24T13:25:32Z","cross_cats_sorted":["cond-mat.str-el","quant-ph"],"title_canon_sha256":"ae4fd489ccc9b077e62a3378d6c57a58ce99d8626f8bcce5830e968affbc2cee","abstract_canon_sha256":"10685eb65b47260a3433e315b345e0e193697777fbd090874b3cdb53d763f799"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-27T01:20:57.946809Z","signature_b64":"l3JmzDupgJB+7OnXg/jfpVekYvUgS9Hrh30YLx2jqg09bRe44vZhS32+mz5NqZ1a/VORH+keRq5PXxHKeyhpDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e4c0cc946d6c686e53dc306b3dbe7d228d144f6715ac3fb04c0f43815638ce80","last_reissued_at":"2026-07-27T01:20:57.945929Z","signature_status":"signed_v1","first_computed_at":"2026-07-27T01:20:57.945929Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Understanding interaction-driven transport in flux lattices with evolution-path symmetry","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["cond-mat.str-el","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Jian-Song Pan, Wei Yi, Xiaofan Zhou","submitted_at":"2026-07-24T13:25:32Z","abstract_excerpt":"The destruction of Aharonov-Bohm (AB) caging by interaction and the emergence of interaction-induced chiral currents in flux lattices are two paradigmatic examples of interaction-driven quantum transport. While various mechanisms, such as bound-state formation and chiral spectral imbalance, have been proposed, a unifying physical picture remains elusive. Here, we employ the concept of \\textit{evolution-path symmetry} (EPS) and its interaction-induced breaking as a framework to understand interaction-induced delocalization in flux lattices. EPS is defined as the invariance of a path's contribut"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.22288","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/2607.22288/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":"2607.22288","created_at":"2026-07-27T01:20:57.946394+00:00"},{"alias_kind":"arxiv_version","alias_value":"2607.22288v1","created_at":"2026-07-27T01:20:57.946394+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.22288","created_at":"2026-07-27T01:20:57.946394+00:00"},{"alias_kind":"pith_short_12","alias_value":"4TAMZFDNNRUG","created_at":"2026-07-27T01:20:57.946394+00:00"},{"alias_kind":"pith_short_16","alias_value":"4TAMZFDNNRUG4U64","created_at":"2026-07-27T01:20:57.946394+00:00"},{"alias_kind":"pith_short_8","alias_value":"4TAMZFDN","created_at":"2026-07-27T01:20:57.946394+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4TAMZFDNNRUG4U64GBVT3PT5EK","json":"https://pith.science/pith/4TAMZFDNNRUG4U64GBVT3PT5EK.json","graph_json":"https://pith.science/api/pith-number/4TAMZFDNNRUG4U64GBVT3PT5EK/graph.json","events_json":"https://pith.science/api/pith-number/4TAMZFDNNRUG4U64GBVT3PT5EK/events.json","paper":"https://pith.science/paper/4TAMZFDN"},"agent_actions":{"view_html":"https://pith.science/pith/4TAMZFDNNRUG4U64GBVT3PT5EK","download_json":"https://pith.science/pith/4TAMZFDNNRUG4U64GBVT3PT5EK.json","view_paper":"https://pith.science/paper/4TAMZFDN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2607.22288&json=true","fetch_graph":"https://pith.science/api/pith-number/4TAMZFDNNRUG4U64GBVT3PT5EK/graph.json","fetch_events":"https://pith.science/api/pith-number/4TAMZFDNNRUG4U64GBVT3PT5EK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4TAMZFDNNRUG4U64GBVT3PT5EK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4TAMZFDNNRUG4U64GBVT3PT5EK/action/storage_attestation","attest_author":"https://pith.science/pith/4TAMZFDNNRUG4U64GBVT3PT5EK/action/author_attestation","sign_citation":"https://pith.science/pith/4TAMZFDNNRUG4U64GBVT3PT5EK/action/citation_signature","submit_replication":"https://pith.science/pith/4TAMZFDNNRUG4U64GBVT3PT5EK/action/replication_record"}},"created_at":"2026-07-27T01:20:57.946394+00:00","updated_at":"2026-07-27T01:20:57.946394+00:00"}