{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:T3SGYRSEZ4Y5HB3ZXJSXBV3MB3","short_pith_number":"pith:T3SGYRSE","schema_version":"1.0","canonical_sha256":"9ee46c4644cf31d38779ba6570d76c0ed4f7839bd969101a17c4830968d71a5f","source":{"kind":"arxiv","id":"1502.03333","version":2},"attestation_state":"computed","paper":{"title":"Radiation reaction induced non-monotonic features in runaway electron distributions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"A. Stahl, E. Hirvijoki, I. Pusztai, J. Decker, O. Embr\\'eus, T. F\\\"ul\\\"op","submitted_at":"2015-02-11T15:20:40Z","abstract_excerpt":"Runaway electrons, which are generated in a plasma where the induced electric field exceeds a certain critical value, can reach very high energies in the MeV range. For such energetic electrons, radiative losses will contribute significantly to the momentum space dynamics. Under certain conditions, due to radiative momentum losses, a non-monotonic feature - a \"bump\" - can form in the runaway electron tail, creating a potential for bump-on-tail-type instabilities to arise. Here we study the conditions for the existence of the bump. We derive an analytical threshold condition for bump appearance"},"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":"1502.03333","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2015-02-11T15:20:40Z","cross_cats_sorted":[],"title_canon_sha256":"054186ed98e78c2107073b2b2008377cbe3a4e5269d5f4c34ff6aca7f585e982","abstract_canon_sha256":"ede2c7b2c6db2a625765d082464582d692568de8d402d1f08508845ded0528d5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:49:04.928616Z","signature_b64":"lembyrVdwFJjbQtJ4M8d3hEAZr9y5AmtrqWay16cZEmOr/MrlEj28ndtSqA4zS7uXn45NQ430MWbNTNayuHlBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9ee46c4644cf31d38779ba6570d76c0ed4f7839bd969101a17c4830968d71a5f","last_reissued_at":"2026-05-18T00:49:04.928035Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:49:04.928035Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Radiation reaction induced non-monotonic features in runaway electron distributions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"A. Stahl, E. Hirvijoki, I. Pusztai, J. Decker, O. Embr\\'eus, T. F\\\"ul\\\"op","submitted_at":"2015-02-11T15:20:40Z","abstract_excerpt":"Runaway electrons, which are generated in a plasma where the induced electric field exceeds a certain critical value, can reach very high energies in the MeV range. For such energetic electrons, radiative losses will contribute significantly to the momentum space dynamics. Under certain conditions, due to radiative momentum losses, a non-monotonic feature - a \"bump\" - can form in the runaway electron tail, creating a potential for bump-on-tail-type instabilities to arise. Here we study the conditions for the existence of the bump. We derive an analytical threshold condition for bump appearance"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.03333","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1502.03333","created_at":"2026-05-18T00:49:04.928112+00:00"},{"alias_kind":"arxiv_version","alias_value":"1502.03333v2","created_at":"2026-05-18T00:49:04.928112+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1502.03333","created_at":"2026-05-18T00:49:04.928112+00:00"},{"alias_kind":"pith_short_12","alias_value":"T3SGYRSEZ4Y5","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_16","alias_value":"T3SGYRSEZ4Y5HB3Z","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_8","alias_value":"T3SGYRSE","created_at":"2026-05-18T12:29:42.218222+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/T3SGYRSEZ4Y5HB3ZXJSXBV3MB3","json":"https://pith.science/pith/T3SGYRSEZ4Y5HB3ZXJSXBV3MB3.json","graph_json":"https://pith.science/api/pith-number/T3SGYRSEZ4Y5HB3ZXJSXBV3MB3/graph.json","events_json":"https://pith.science/api/pith-number/T3SGYRSEZ4Y5HB3ZXJSXBV3MB3/events.json","paper":"https://pith.science/paper/T3SGYRSE"},"agent_actions":{"view_html":"https://pith.science/pith/T3SGYRSEZ4Y5HB3ZXJSXBV3MB3","download_json":"https://pith.science/pith/T3SGYRSEZ4Y5HB3ZXJSXBV3MB3.json","view_paper":"https://pith.science/paper/T3SGYRSE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1502.03333&json=true","fetch_graph":"https://pith.science/api/pith-number/T3SGYRSEZ4Y5HB3ZXJSXBV3MB3/graph.json","fetch_events":"https://pith.science/api/pith-number/T3SGYRSEZ4Y5HB3ZXJSXBV3MB3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/T3SGYRSEZ4Y5HB3ZXJSXBV3MB3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/T3SGYRSEZ4Y5HB3ZXJSXBV3MB3/action/storage_attestation","attest_author":"https://pith.science/pith/T3SGYRSEZ4Y5HB3ZXJSXBV3MB3/action/author_attestation","sign_citation":"https://pith.science/pith/T3SGYRSEZ4Y5HB3ZXJSXBV3MB3/action/citation_signature","submit_replication":"https://pith.science/pith/T3SGYRSEZ4Y5HB3ZXJSXBV3MB3/action/replication_record"}},"created_at":"2026-05-18T00:49:04.928112+00:00","updated_at":"2026-05-18T00:49:04.928112+00:00"}