{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:J3JTEK57ZBTBNBBNHW3BTPLW4W","short_pith_number":"pith:J3JTEK57","schema_version":"1.0","canonical_sha256":"4ed3322bbfc86616842d3db619bd76e5b971026eb0149eb3ec3e77f219d89bed","source":{"kind":"arxiv","id":"1702.03171","version":3},"attestation_state":"computed","paper":{"title":"Vacuum Cherenkov radiation for Lorentz-violating fermions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"M. Schreck","submitted_at":"2017-02-10T13:52:06Z","abstract_excerpt":"The current work focuses on the process of vacuum Cherenkov radiation for Lorentz-violating fermions that are described by the minimal Standard-Model Extension (SME). To date, most considerations of this important hypothetical process have been restricted to Lorentz-violating photons, as the necessary theoretical tools for the SME fermion sector have not been available. With their development in a very recent paper, we are now in a position to compute the decay rates based on a modified Dirac theory. Two realizations of the Cherenkov process are studied. In the first scenario, the spin project"},"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":"1702.03171","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-02-10T13:52:06Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"a2aad2a36db06636604ff90733e1a39227b9427f7b790ad09da289f263b3ece7","abstract_canon_sha256":"642fa25a6e1338985583722de427ee950148361e3dd14c96ad6f30367bacd771"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:29:01.669119Z","signature_b64":"uPuckuEzD0Wo9vMDP4/ggIniVrfeN2RJMTXpii57bxYVyi8igCiAbPHNYMWbe8ErvO9C/mamF+/gLy7xZK4GCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4ed3322bbfc86616842d3db619bd76e5b971026eb0149eb3ec3e77f219d89bed","last_reissued_at":"2026-05-18T00:29:01.668699Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:29:01.668699Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Vacuum Cherenkov radiation for Lorentz-violating fermions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"M. Schreck","submitted_at":"2017-02-10T13:52:06Z","abstract_excerpt":"The current work focuses on the process of vacuum Cherenkov radiation for Lorentz-violating fermions that are described by the minimal Standard-Model Extension (SME). To date, most considerations of this important hypothetical process have been restricted to Lorentz-violating photons, as the necessary theoretical tools for the SME fermion sector have not been available. With their development in a very recent paper, we are now in a position to compute the decay rates based on a modified Dirac theory. Two realizations of the Cherenkov process are studied. In the first scenario, the spin project"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.03171","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":""},"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":"1702.03171","created_at":"2026-05-18T00:29:01.668764+00:00"},{"alias_kind":"arxiv_version","alias_value":"1702.03171v3","created_at":"2026-05-18T00:29:01.668764+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.03171","created_at":"2026-05-18T00:29:01.668764+00:00"},{"alias_kind":"pith_short_12","alias_value":"J3JTEK57ZBTB","created_at":"2026-05-18T12:31:21.493067+00:00"},{"alias_kind":"pith_short_16","alias_value":"J3JTEK57ZBTBNBBN","created_at":"2026-05-18T12:31:21.493067+00:00"},{"alias_kind":"pith_short_8","alias_value":"J3JTEK57","created_at":"2026-05-18T12:31:21.493067+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.17646","citing_title":"Crystallography, Lorentz violation, and the Standard-Model Extension","ref_index":57,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/J3JTEK57ZBTBNBBNHW3BTPLW4W","json":"https://pith.science/pith/J3JTEK57ZBTBNBBNHW3BTPLW4W.json","graph_json":"https://pith.science/api/pith-number/J3JTEK57ZBTBNBBNHW3BTPLW4W/graph.json","events_json":"https://pith.science/api/pith-number/J3JTEK57ZBTBNBBNHW3BTPLW4W/events.json","paper":"https://pith.science/paper/J3JTEK57"},"agent_actions":{"view_html":"https://pith.science/pith/J3JTEK57ZBTBNBBNHW3BTPLW4W","download_json":"https://pith.science/pith/J3JTEK57ZBTBNBBNHW3BTPLW4W.json","view_paper":"https://pith.science/paper/J3JTEK57","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1702.03171&json=true","fetch_graph":"https://pith.science/api/pith-number/J3JTEK57ZBTBNBBNHW3BTPLW4W/graph.json","fetch_events":"https://pith.science/api/pith-number/J3JTEK57ZBTBNBBNHW3BTPLW4W/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J3JTEK57ZBTBNBBNHW3BTPLW4W/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J3JTEK57ZBTBNBBNHW3BTPLW4W/action/storage_attestation","attest_author":"https://pith.science/pith/J3JTEK57ZBTBNBBNHW3BTPLW4W/action/author_attestation","sign_citation":"https://pith.science/pith/J3JTEK57ZBTBNBBNHW3BTPLW4W/action/citation_signature","submit_replication":"https://pith.science/pith/J3JTEK57ZBTBNBBNHW3BTPLW4W/action/replication_record"}},"created_at":"2026-05-18T00:29:01.668764+00:00","updated_at":"2026-05-18T00:29:01.668764+00:00"}