{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:ZBYUMGYSRRQ4GNRASNAMHFJPNH","short_pith_number":"pith:ZBYUMGYS","schema_version":"1.0","canonical_sha256":"c871461b128c61c336209340c3952f69d5d7ed0da38e46ce1e621f2953bbfa62","source":{"kind":"arxiv","id":"1608.02215","version":1},"attestation_state":"computed","paper":{"title":"Properties of an ultrarelativistic charged particle radiation in a constant homogeneous crossed electromagnetic field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"G.Yu. Lazarenko, O.V. Bogdanov, P.O. Kazinski","submitted_at":"2016-08-07T13:31:19Z","abstract_excerpt":"The properties of radiation created by a classical ultrarelativistic scalar charged particle in a constant homogeneous crossed electromagnetic field are described both analytically and numerically with radiation reaction taken into account in the form of the Landau-Lifshitz equation. The total radiation naturally falls into two parts: the radiation formed at the entrance point of a particle into the crossed field (the synchrotron entrance radiation), and the radiation coming from the late-time asymptotics of a particle motion (the de-excited radiation). The synchrotron entrance radiation resem"},"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":"1608.02215","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-08-07T13:31:19Z","cross_cats_sorted":[],"title_canon_sha256":"18c1b4059eecbecedf362478ebe066c8ed68f38057324dd1aaf598e878a969cd","abstract_canon_sha256":"3856942b42d719ed5b48b8e65ea6c52dd84c80fcd87bd1317779caed2d5ad8f2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:45:15.751819Z","signature_b64":"CLwwyHINkhGmMhxGjJEfEKvFWrdIlOpVJx9vPN/qGxtFKtCVoFD1CFvTmvu34NTaqxACv+WFdZZcA3XoytrWBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c871461b128c61c336209340c3952f69d5d7ed0da38e46ce1e621f2953bbfa62","last_reissued_at":"2026-05-18T00:45:15.751156Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:45:15.751156Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Properties of an ultrarelativistic charged particle radiation in a constant homogeneous crossed electromagnetic field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"G.Yu. Lazarenko, O.V. Bogdanov, P.O. Kazinski","submitted_at":"2016-08-07T13:31:19Z","abstract_excerpt":"The properties of radiation created by a classical ultrarelativistic scalar charged particle in a constant homogeneous crossed electromagnetic field are described both analytically and numerically with radiation reaction taken into account in the form of the Landau-Lifshitz equation. The total radiation naturally falls into two parts: the radiation formed at the entrance point of a particle into the crossed field (the synchrotron entrance radiation), and the radiation coming from the late-time asymptotics of a particle motion (the de-excited radiation). The synchrotron entrance radiation resem"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.02215","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":"1608.02215","created_at":"2026-05-18T00:45:15.751230+00:00"},{"alias_kind":"arxiv_version","alias_value":"1608.02215v1","created_at":"2026-05-18T00:45:15.751230+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.02215","created_at":"2026-05-18T00:45:15.751230+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZBYUMGYSRRQ4","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZBYUMGYSRRQ4GNRA","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZBYUMGYS","created_at":"2026-05-18T12:30:53.716459+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/ZBYUMGYSRRQ4GNRASNAMHFJPNH","json":"https://pith.science/pith/ZBYUMGYSRRQ4GNRASNAMHFJPNH.json","graph_json":"https://pith.science/api/pith-number/ZBYUMGYSRRQ4GNRASNAMHFJPNH/graph.json","events_json":"https://pith.science/api/pith-number/ZBYUMGYSRRQ4GNRASNAMHFJPNH/events.json","paper":"https://pith.science/paper/ZBYUMGYS"},"agent_actions":{"view_html":"https://pith.science/pith/ZBYUMGYSRRQ4GNRASNAMHFJPNH","download_json":"https://pith.science/pith/ZBYUMGYSRRQ4GNRASNAMHFJPNH.json","view_paper":"https://pith.science/paper/ZBYUMGYS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1608.02215&json=true","fetch_graph":"https://pith.science/api/pith-number/ZBYUMGYSRRQ4GNRASNAMHFJPNH/graph.json","fetch_events":"https://pith.science/api/pith-number/ZBYUMGYSRRQ4GNRASNAMHFJPNH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZBYUMGYSRRQ4GNRASNAMHFJPNH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZBYUMGYSRRQ4GNRASNAMHFJPNH/action/storage_attestation","attest_author":"https://pith.science/pith/ZBYUMGYSRRQ4GNRASNAMHFJPNH/action/author_attestation","sign_citation":"https://pith.science/pith/ZBYUMGYSRRQ4GNRASNAMHFJPNH/action/citation_signature","submit_replication":"https://pith.science/pith/ZBYUMGYSRRQ4GNRASNAMHFJPNH/action/replication_record"}},"created_at":"2026-05-18T00:45:15.751230+00:00","updated_at":"2026-05-18T00:45:15.751230+00:00"}