{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:AY7VH2FMTT7G5TNAGVCYKPAEWB","short_pith_number":"pith:AY7VH2FM","schema_version":"1.0","canonical_sha256":"063f53e8ac9cfe6ecda03545853c04b079ebd33b2da0872bdf7b5aefedf21438","source":{"kind":"arxiv","id":"1206.2249","version":1},"attestation_state":"computed","paper":{"title":"Abelian geometric phase for a Dirac neutral particle in a Lorentz symmetry violation environment","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"H. Belich, K. Bakke","submitted_at":"2012-06-11T15:17:11Z","abstract_excerpt":"We introduce a new term into the Dirac equation based on the Lorentz symmetry violation background in order to make a theoretical description of the relativistic quantum dynamics of a spin-half neutral particle, where the wave function of the neutral particle acquires a relativistic Abelian quantum phase given by the interaction between a fixed time-like 4-vector background and crossed electric and magnetic fields, which is analogous to the geometric phase obtained by Wei \\textit{et al} [H. Wei, R. Han and X. Wei, Phys. Rev. Lett. \\textbf{75}, 2071 (1995)] for a spinless neutral particle with "},"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":"1206.2249","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-06-11T15:17:11Z","cross_cats_sorted":[],"title_canon_sha256":"9a5743014fb419571f71a5158242740cadff8e72a55f7728eed33738cbe2b35a","abstract_canon_sha256":"a1374e42da23021fc34338909315b905abe04b6fa58edd32213891bdd0aa4f54"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:53:53.031990Z","signature_b64":"6zGsBf1ccM843pbzVeUR/AHkZNRQYMH06AGGEtbfs2eqxhwnsKJ0Gik8JexfDb6Ndy0lDMSIEQ/+BUjhfzISDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"063f53e8ac9cfe6ecda03545853c04b079ebd33b2da0872bdf7b5aefedf21438","last_reissued_at":"2026-05-18T03:53:53.031455Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:53:53.031455Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Abelian geometric phase for a Dirac neutral particle in a Lorentz symmetry violation environment","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"H. Belich, K. Bakke","submitted_at":"2012-06-11T15:17:11Z","abstract_excerpt":"We introduce a new term into the Dirac equation based on the Lorentz symmetry violation background in order to make a theoretical description of the relativistic quantum dynamics of a spin-half neutral particle, where the wave function of the neutral particle acquires a relativistic Abelian quantum phase given by the interaction between a fixed time-like 4-vector background and crossed electric and magnetic fields, which is analogous to the geometric phase obtained by Wei \\textit{et al} [H. Wei, R. Han and X. Wei, Phys. Rev. Lett. \\textbf{75}, 2071 (1995)] for a spinless neutral particle with "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.2249","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":""},"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":"1206.2249","created_at":"2026-05-18T03:53:53.031549+00:00"},{"alias_kind":"arxiv_version","alias_value":"1206.2249v1","created_at":"2026-05-18T03:53:53.031549+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.2249","created_at":"2026-05-18T03:53:53.031549+00:00"},{"alias_kind":"pith_short_12","alias_value":"AY7VH2FMTT7G","created_at":"2026-05-18T12:26:58.693483+00:00"},{"alias_kind":"pith_short_16","alias_value":"AY7VH2FMTT7G5TNA","created_at":"2026-05-18T12:26:58.693483+00:00"},{"alias_kind":"pith_short_8","alias_value":"AY7VH2FM","created_at":"2026-05-18T12:26:58.693483+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/AY7VH2FMTT7G5TNAGVCYKPAEWB","json":"https://pith.science/pith/AY7VH2FMTT7G5TNAGVCYKPAEWB.json","graph_json":"https://pith.science/api/pith-number/AY7VH2FMTT7G5TNAGVCYKPAEWB/graph.json","events_json":"https://pith.science/api/pith-number/AY7VH2FMTT7G5TNAGVCYKPAEWB/events.json","paper":"https://pith.science/paper/AY7VH2FM"},"agent_actions":{"view_html":"https://pith.science/pith/AY7VH2FMTT7G5TNAGVCYKPAEWB","download_json":"https://pith.science/pith/AY7VH2FMTT7G5TNAGVCYKPAEWB.json","view_paper":"https://pith.science/paper/AY7VH2FM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1206.2249&json=true","fetch_graph":"https://pith.science/api/pith-number/AY7VH2FMTT7G5TNAGVCYKPAEWB/graph.json","fetch_events":"https://pith.science/api/pith-number/AY7VH2FMTT7G5TNAGVCYKPAEWB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AY7VH2FMTT7G5TNAGVCYKPAEWB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AY7VH2FMTT7G5TNAGVCYKPAEWB/action/storage_attestation","attest_author":"https://pith.science/pith/AY7VH2FMTT7G5TNAGVCYKPAEWB/action/author_attestation","sign_citation":"https://pith.science/pith/AY7VH2FMTT7G5TNAGVCYKPAEWB/action/citation_signature","submit_replication":"https://pith.science/pith/AY7VH2FMTT7G5TNAGVCYKPAEWB/action/replication_record"}},"created_at":"2026-05-18T03:53:53.031549+00:00","updated_at":"2026-05-18T03:53:53.031549+00:00"}