{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:22XY5HC6Z7EBLECCTXQL3YUI37","short_pith_number":"pith:22XY5HC6","schema_version":"1.0","canonical_sha256":"d6af8e9c5ecfc81590429de0bde288dfc5e85112203b3c73a546261a894a8ec5","source":{"kind":"arxiv","id":"2407.06553","version":3},"attestation_state":"computed","paper":{"title":"Gravitational orbital Hall effect of vortex light in Lense-Thirring metric","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Dan-Dan Lian, Peng-Ming Zhang, Wei-Si Qiu","submitted_at":"2024-07-09T05:18:30Z","abstract_excerpt":"Vortex light, characterized by an intrinsic orbital angular momentum aligned with its propagation direction, is described through vortex electromagnetic waves. Similar to the gravitational spin Hall effect (SHE), vortex light is expected to exhibit intrinsic orbital angular momentum dependent trajectories and deviations from the null geodesic plane when propagating through a gravitational field, a phenomenon termed the gravitational orbital Hall effect (OHE). In this work, we model the vortex light as vortex Laguerre-Gaussian electromagnetic wave packets and analyze its motion by solving covar"},"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":"2407.06553","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2024-07-09T05:18:30Z","cross_cats_sorted":[],"title_canon_sha256":"c79afc2eee954ec450d11168a534afaab5b22f399796344d8f5442e54b56bab7","abstract_canon_sha256":"57a5859a1ba8153479b044e56079b356dc60bea57b65ae11bfcda5f430166a97"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:17:14.534654Z","signature_b64":"cvj12J0FwMi0xenmPR5rf6m9RJQc4B60LBjp4YvarTeHCb5Wzwdx1lU5yfzGpkgaUI0z9dEzCfd09VXNsQogCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d6af8e9c5ecfc81590429de0bde288dfc5e85112203b3c73a546261a894a8ec5","last_reissued_at":"2026-07-05T09:17:14.534141Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:17:14.534141Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gravitational orbital Hall effect of vortex light in Lense-Thirring metric","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Dan-Dan Lian, Peng-Ming Zhang, Wei-Si Qiu","submitted_at":"2024-07-09T05:18:30Z","abstract_excerpt":"Vortex light, characterized by an intrinsic orbital angular momentum aligned with its propagation direction, is described through vortex electromagnetic waves. Similar to the gravitational spin Hall effect (SHE), vortex light is expected to exhibit intrinsic orbital angular momentum dependent trajectories and deviations from the null geodesic plane when propagating through a gravitational field, a phenomenon termed the gravitational orbital Hall effect (OHE). In this work, we model the vortex light as vortex Laguerre-Gaussian electromagnetic wave packets and analyze its motion by solving covar"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2407.06553","kind":"arxiv","version":3},"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/2407.06553/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":"2407.06553","created_at":"2026-07-05T09:17:14.534197+00:00"},{"alias_kind":"arxiv_version","alias_value":"2407.06553v3","created_at":"2026-07-05T09:17:14.534197+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2407.06553","created_at":"2026-07-05T09:17:14.534197+00:00"},{"alias_kind":"pith_short_12","alias_value":"22XY5HC6Z7EB","created_at":"2026-07-05T09:17:14.534197+00:00"},{"alias_kind":"pith_short_16","alias_value":"22XY5HC6Z7EBLECC","created_at":"2026-07-05T09:17:14.534197+00:00"},{"alias_kind":"pith_short_8","alias_value":"22XY5HC6","created_at":"2026-07-05T09:17:14.534197+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.12053","citing_title":"Flyby Anomaly in the Variation Principle of General Relativity","ref_index":18,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/22XY5HC6Z7EBLECCTXQL3YUI37","json":"https://pith.science/pith/22XY5HC6Z7EBLECCTXQL3YUI37.json","graph_json":"https://pith.science/api/pith-number/22XY5HC6Z7EBLECCTXQL3YUI37/graph.json","events_json":"https://pith.science/api/pith-number/22XY5HC6Z7EBLECCTXQL3YUI37/events.json","paper":"https://pith.science/paper/22XY5HC6"},"agent_actions":{"view_html":"https://pith.science/pith/22XY5HC6Z7EBLECCTXQL3YUI37","download_json":"https://pith.science/pith/22XY5HC6Z7EBLECCTXQL3YUI37.json","view_paper":"https://pith.science/paper/22XY5HC6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2407.06553&json=true","fetch_graph":"https://pith.science/api/pith-number/22XY5HC6Z7EBLECCTXQL3YUI37/graph.json","fetch_events":"https://pith.science/api/pith-number/22XY5HC6Z7EBLECCTXQL3YUI37/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/22XY5HC6Z7EBLECCTXQL3YUI37/action/timestamp_anchor","attest_storage":"https://pith.science/pith/22XY5HC6Z7EBLECCTXQL3YUI37/action/storage_attestation","attest_author":"https://pith.science/pith/22XY5HC6Z7EBLECCTXQL3YUI37/action/author_attestation","sign_citation":"https://pith.science/pith/22XY5HC6Z7EBLECCTXQL3YUI37/action/citation_signature","submit_replication":"https://pith.science/pith/22XY5HC6Z7EBLECCTXQL3YUI37/action/replication_record"}},"created_at":"2026-07-05T09:17:14.534197+00:00","updated_at":"2026-07-05T09:17:14.534197+00:00"}