{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2007:2MVO2ZP7KKSFO2IMWTYJJWJD7G","short_pith_number":"pith:2MVO2ZP7","canonical_record":{"source":{"id":"hep-th/0701092","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2007-01-10T16:47:46Z","cross_cats_sorted":[],"title_canon_sha256":"a3f966fb64e10942b89c72e8bd68ab583d0ac397daaf0d66d5f3b2990400dc42","abstract_canon_sha256":"b8299ab155acbc796481b6b9e6059a997e89578bc560ff61fa151b2e32c1bc8e"},"schema_version":"1.0"},"canonical_sha256":"d32aed65ff52a457690cb4f094d923f9b31a5c11aded9898668319b6466ff67a","source":{"kind":"arxiv","id":"hep-th/0701092","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0701092","created_at":"2026-05-18T04:34:28Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0701092v2","created_at":"2026-05-18T04:34:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0701092","created_at":"2026-05-18T04:34:28Z"},{"alias_kind":"pith_short_12","alias_value":"2MVO2ZP7KKSF","created_at":"2026-05-18T12:25:54Z"},{"alias_kind":"pith_short_16","alias_value":"2MVO2ZP7KKSFO2IM","created_at":"2026-05-18T12:25:54Z"},{"alias_kind":"pith_short_8","alias_value":"2MVO2ZP7","created_at":"2026-05-18T12:25:54Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2007:2MVO2ZP7KKSFO2IMWTYJJWJD7G","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/0701092","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2007-01-10T16:47:46Z","cross_cats_sorted":[],"title_canon_sha256":"a3f966fb64e10942b89c72e8bd68ab583d0ac397daaf0d66d5f3b2990400dc42","abstract_canon_sha256":"b8299ab155acbc796481b6b9e6059a997e89578bc560ff61fa151b2e32c1bc8e"},"schema_version":"1.0"},"canonical_sha256":"d32aed65ff52a457690cb4f094d923f9b31a5c11aded9898668319b6466ff67a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:34:28.250127Z","signature_b64":"VliolI6cF308tv1sQSvfHZa1rwK5gxx/2N70+JYNwLwqtLT9zOgM8blN3WFZzp2Yi/Jz0X7NzSjTLm3KuFwACw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d32aed65ff52a457690cb4f094d923f9b31a5c11aded9898668319b6466ff67a","last_reissued_at":"2026-05-18T04:34:28.249478Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:34:28.249478Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/0701092","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:34:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lDeJIq9DnkoCeeDlySSaTiXp9wHHLWijuk4iTD1OAqHoFZ/QypBYl5wLEBy1tM0pp7n5PpsDYpD5wkBJ5eBXAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T20:49:44.118523Z"},"content_sha256":"675a702b0973d614a2a2a49cbc9b697a2a6981e51225e4d54aaa733f53fec811","schema_version":"1.0","event_id":"sha256:675a702b0973d614a2a2a49cbc9b697a2a6981e51225e4d54aaa733f53fec811"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2007:2MVO2ZP7KKSFO2IMWTYJJWJD7G","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Obtaining the equation of motion for a fermionic particle in a generalized Lorentz-violating system framework","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alex E. Bernardini, Roldao da Rocha","submitted_at":"2007-01-10T16:47:46Z","abstract_excerpt":"Using a generalized procedure for obtaining the dispersion relation and the equation of motion for a propagating fermionic particle, we examine previous claims for a preferred axis at $n_{\\mu}$($\\equiv(1,0,0,1)$), $n^{2}=0$ embedded in the framework of very special relativity (VSR). We show that, in a relatively high energy scale, the corresponding equation of motion is reduced to a conserving lepton number chiral equation previously predicted in the literature. Otherwise, in a relatively low energy scale, the equation is reduced to the usual Dirac equation for a free propagating fermionic par"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0701092","kind":"arxiv","version":2},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:34:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ILrtJzSmQkdcMCFkDY+9qvebHURoIyNFRioRzLmg9kkcOZ2VBqpi5mV00uTyBoIRPTBU50wzf8gzSsmHT6xaBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T20:49:44.119249Z"},"content_sha256":"c4738d53cfd34ac04c72def03dfc99b417af95f0585048e25bdbce5caa047825","schema_version":"1.0","event_id":"sha256:c4738d53cfd34ac04c72def03dfc99b417af95f0585048e25bdbce5caa047825"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2MVO2ZP7KKSFO2IMWTYJJWJD7G/bundle.json","state_url":"https://pith.science/pith/2MVO2ZP7KKSFO2IMWTYJJWJD7G/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2MVO2ZP7KKSFO2IMWTYJJWJD7G/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-28T20:49:44Z","links":{"resolver":"https://pith.science/pith/2MVO2ZP7KKSFO2IMWTYJJWJD7G","bundle":"https://pith.science/pith/2MVO2ZP7KKSFO2IMWTYJJWJD7G/bundle.json","state":"https://pith.science/pith/2MVO2ZP7KKSFO2IMWTYJJWJD7G/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2MVO2ZP7KKSFO2IMWTYJJWJD7G/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2007:2MVO2ZP7KKSFO2IMWTYJJWJD7G","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":"b8299ab155acbc796481b6b9e6059a997e89578bc560ff61fa151b2e32c1bc8e","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"2007-01-10T16:47:46Z","title_canon_sha256":"a3f966fb64e10942b89c72e8bd68ab583d0ac397daaf0d66d5f3b2990400dc42"},"schema_version":"1.0","source":{"id":"hep-th/0701092","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0701092","created_at":"2026-05-18T04:34:28Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0701092v2","created_at":"2026-05-18T04:34:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0701092","created_at":"2026-05-18T04:34:28Z"},{"alias_kind":"pith_short_12","alias_value":"2MVO2ZP7KKSF","created_at":"2026-05-18T12:25:54Z"},{"alias_kind":"pith_short_16","alias_value":"2MVO2ZP7KKSFO2IM","created_at":"2026-05-18T12:25:54Z"},{"alias_kind":"pith_short_8","alias_value":"2MVO2ZP7","created_at":"2026-05-18T12:25:54Z"}],"graph_snapshots":[{"event_id":"sha256:c4738d53cfd34ac04c72def03dfc99b417af95f0585048e25bdbce5caa047825","target":"graph","created_at":"2026-05-18T04:34:28Z","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"},"paper":{"abstract_excerpt":"Using a generalized procedure for obtaining the dispersion relation and the equation of motion for a propagating fermionic particle, we examine previous claims for a preferred axis at $n_{\\mu}$($\\equiv(1,0,0,1)$), $n^{2}=0$ embedded in the framework of very special relativity (VSR). We show that, in a relatively high energy scale, the corresponding equation of motion is reduced to a conserving lepton number chiral equation previously predicted in the literature. Otherwise, in a relatively low energy scale, the equation is reduced to the usual Dirac equation for a free propagating fermionic par","authors_text":"Alex E. Bernardini, Roldao da Rocha","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"2007-01-10T16:47:46Z","title":"Obtaining the equation of motion for a fermionic particle in a generalized Lorentz-violating system framework"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0701092","kind":"arxiv","version":2},"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":"sha256:675a702b0973d614a2a2a49cbc9b697a2a6981e51225e4d54aaa733f53fec811","target":"record","created_at":"2026-05-18T04:34:28Z","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":"b8299ab155acbc796481b6b9e6059a997e89578bc560ff61fa151b2e32c1bc8e","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"2007-01-10T16:47:46Z","title_canon_sha256":"a3f966fb64e10942b89c72e8bd68ab583d0ac397daaf0d66d5f3b2990400dc42"},"schema_version":"1.0","source":{"id":"hep-th/0701092","kind":"arxiv","version":2}},"canonical_sha256":"d32aed65ff52a457690cb4f094d923f9b31a5c11aded9898668319b6466ff67a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d32aed65ff52a457690cb4f094d923f9b31a5c11aded9898668319b6466ff67a","first_computed_at":"2026-05-18T04:34:28.249478Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:34:28.249478Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"VliolI6cF308tv1sQSvfHZa1rwK5gxx/2N70+JYNwLwqtLT9zOgM8blN3WFZzp2Yi/Jz0X7NzSjTLm3KuFwACw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:34:28.250127Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/0701092","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:675a702b0973d614a2a2a49cbc9b697a2a6981e51225e4d54aaa733f53fec811","sha256:c4738d53cfd34ac04c72def03dfc99b417af95f0585048e25bdbce5caa047825"],"state_sha256":"4373f03275d2ff982c9161eaec554b09f266766cdbe8e6a6c9b3e426d1a12ebd"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"feC8rimDXt4cUUA/+BCS7xBmUuGDmJZX1oBZdZcswCnDiiqFAwDcB8hrk6mADft2000Bx1EH3bNqSom4SQlTAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T20:49:44.122982Z","bundle_sha256":"438152b773c4b579a211fe9e870e4b79af2f7b9330fa28e6ab155f264b78f97e"}}