{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:M3PXMUIU3H4PJOABIY36LVKWM4","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":"cdfabbef8383df6091867a0b45b00b429a9f3af69ca28542c1dadb122d260212","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2026-03-30T07:45:17Z","title_canon_sha256":"56a535133bd6a87455161aa684405495e1b47b031887935eda101d20a385373d"},"schema_version":"1.0","source":{"id":"2603.28127","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2603.28127","created_at":"2026-07-03T01:17:19Z"},{"alias_kind":"arxiv_version","alias_value":"2603.28127v3","created_at":"2026-07-03T01:17:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2603.28127","created_at":"2026-07-03T01:17:19Z"},{"alias_kind":"pith_short_12","alias_value":"M3PXMUIU3H4P","created_at":"2026-07-03T01:17:19Z"},{"alias_kind":"pith_short_16","alias_value":"M3PXMUIU3H4PJOAB","created_at":"2026-07-03T01:17:19Z"},{"alias_kind":"pith_short_8","alias_value":"M3PXMUIU","created_at":"2026-07-03T01:17:19Z"}],"graph_snapshots":[{"event_id":"sha256:a6e607581d520a0c183e0d19ca8811a5317423ef2996545c7685d9df61e88445","target":"graph","created_at":"2026-07-03T01:17:19Z","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/2603.28127/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Emergent Dirac fields, exhibiting effective relativistic physics, are most commonly associated with bulk and surface states in materials such as graphene and topological insulators. Here we identify a previously unexplored class of Dirac states that propagate along branch-cut defects in a complex Dirac mass field, unlike the well-known Jackiw-Rebbi and Jackiw-Rossi states localized at domain-wall and vortex defects. These traveling-wave defect states, termed Dirac branch-cut (DBC) modes, obey an effective one-dimensional relativistic Dirac equation with a reduced mass determined by the phase d","authors_text":"Baile Zhang, Bofeng Zhu, Chengzhi Ma, Gui-Geng Liu, Qiang Wang, Qi Jie Wang, Xiuhai Zhang, Y. D. Chong, Zheyu Cheng","cross_cats":["cond-mat.mtrl-sci"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2026-03-30T07:45:17Z","title":"Dirac branch-cut modes with relativistic transport"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2603.28127","kind":"arxiv","version":3},"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:ec5778dc4ed5047722d1fae80bb001ad26e6136cf4fd24191f782586c8869ac0","target":"record","created_at":"2026-07-03T01:17:19Z","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":"cdfabbef8383df6091867a0b45b00b429a9f3af69ca28542c1dadb122d260212","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2026-03-30T07:45:17Z","title_canon_sha256":"56a535133bd6a87455161aa684405495e1b47b031887935eda101d20a385373d"},"schema_version":"1.0","source":{"id":"2603.28127","kind":"arxiv","version":3}},"canonical_sha256":"66df765114d9f8f4b8014637e5d5566735c4a716dea2f759ed5daeff4902fc9e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"66df765114d9f8f4b8014637e5d5566735c4a716dea2f759ed5daeff4902fc9e","first_computed_at":"2026-07-03T01:17:19.998264Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-03T01:17:19.998264Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"o//IvmewMpIwj37zpuwWmGc/DBqnozWeCaMWmLC+N2mTvYl3H65cLAP5bEi1R0ES49jB8MnsOfbs+SR8MyVvAw==","signature_status":"signed_v1","signed_at":"2026-07-03T01:17:19.998747Z","signed_message":"canonical_sha256_bytes"},"source_id":"2603.28127","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ec5778dc4ed5047722d1fae80bb001ad26e6136cf4fd24191f782586c8869ac0","sha256:a6e607581d520a0c183e0d19ca8811a5317423ef2996545c7685d9df61e88445"],"state_sha256":"b256a0d22fb18874d81abed4c7a10187dfdfadcfbd3b807df7f375676cba70b3"}