{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:F2DHA7W3UYDOVT3VMFBTVJM3QX","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"0618aff035d1041af29f7d6df14b238219e7da0ee350f74da96f805107cf7f78","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2024-01-15T20:19:07Z","title_canon_sha256":"4f6eecf4b5c3be0d0eb2d44f8accf6c2ab33efb370934d9969eaf683f8d6e1d9"},"schema_version":"1.0","source":{"id":"2401.07946","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2401.07946","created_at":"2026-07-05T11:26:41Z"},{"alias_kind":"arxiv_version","alias_value":"2401.07946v1","created_at":"2026-07-05T11:26:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2401.07946","created_at":"2026-07-05T11:26:41Z"},{"alias_kind":"pith_short_12","alias_value":"F2DHA7W3UYDO","created_at":"2026-07-05T11:26:41Z"},{"alias_kind":"pith_short_16","alias_value":"F2DHA7W3UYDOVT3V","created_at":"2026-07-05T11:26:41Z"},{"alias_kind":"pith_short_8","alias_value":"F2DHA7W3","created_at":"2026-07-05T11:26:41Z"}],"graph_snapshots":[{"event_id":"sha256:431466577d4a597cfd06d06b885b8080fb09fe763bdb25143c5da59f73b9e8f1","target":"graph","created_at":"2026-07-05T11:26:41Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2401.07946/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The Aharonov-Bohm effect is a physical phenomenon where the vector potential induces a phase shift of electron wavepackets in regions with zero magnetic fields. It is often referred to as evidence for the physical reality of the vector potential. A similar effect can be observed in solid-state systems, where the Berry connection can influence electron dynamics. Here, we show that in chiral-symmetric processes the Berry connection determines an observable effect on the mean chiral displacement of delocalized wavefunctions. This finding is supported by a photonic experiment realizing a topologic","authors_text":"Alessio D'Errico, Ebrahim Karimi, Filippo Cardano, Francesco Di Colandrea, Nazanin Dehghan","cross_cats":["physics.optics","quant-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2024-01-15T20:19:07Z","title":"Manifestation of the Berry connection in chiral lattice systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2401.07946","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:8476e1504f2bb9b9b1e134dfcd5da7e519b341564b6542aed2d51af0a36a2b69","target":"record","created_at":"2026-07-05T11:26:41Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"0618aff035d1041af29f7d6df14b238219e7da0ee350f74da96f805107cf7f78","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2024-01-15T20:19:07Z","title_canon_sha256":"4f6eecf4b5c3be0d0eb2d44f8accf6c2ab33efb370934d9969eaf683f8d6e1d9"},"schema_version":"1.0","source":{"id":"2401.07946","kind":"arxiv","version":1}},"canonical_sha256":"2e86707edba606eacf7561433aa59b85d78ca431f59f6321e07c5f04842f44ff","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2e86707edba606eacf7561433aa59b85d78ca431f59f6321e07c5f04842f44ff","first_computed_at":"2026-07-05T11:26:41.614801Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:26:41.614801Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"FQTIr1eYTUT3nGHUMRgbjd+txFjrq4BAuMCJu9JjpFfJIdHGd2SkvcjMlP/n7temxVmqnIp4SApFG99QX911Aw==","signature_status":"signed_v1","signed_at":"2026-07-05T11:26:41.615278Z","signed_message":"canonical_sha256_bytes"},"source_id":"2401.07946","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8476e1504f2bb9b9b1e134dfcd5da7e519b341564b6542aed2d51af0a36a2b69","sha256:431466577d4a597cfd06d06b885b8080fb09fe763bdb25143c5da59f73b9e8f1"],"state_sha256":"ef53d1bf19c4d1fc6c185eecccfeba7164a535d560e239d91165995c1faf6927"}