{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:LIUFCLF2I7IYN3SUXRPR4JRVTL","short_pith_number":"pith:LIUFCLF2","schema_version":"1.0","canonical_sha256":"5a28512cba47d186ee54bc5f1e26359ac50f1b33226a44801e6346cf3b09ed6f","source":{"kind":"arxiv","id":"1501.01771","version":1},"attestation_state":"computed","paper":{"title":"Dissociative electron attachment and electron-impact resonant dissociation of vibrationally excited O2 molecules","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph","physics.chem-ph"],"primary_cat":"physics.plasm-ph","authors_text":"J. Tennyson, R. Celiberto, V. Laporta","submitted_at":"2015-01-08T09:15:44Z","abstract_excerpt":"State-by-state cross sections for dissociative electron attachment and electron-impact dissociation for molecular oxygen are computed using ab initio resonance curves calculated with the R-matrix method. When O2 is in its vibrational ground state, the main contribution for both processes comes from the $^2\\Pi_u$ resonance state of $O_2^-$ but with a significant contribution from the $^4\\Sigma$ resonant state. Vibrational excitation leads to an increased contribution from the low-lying $^2\\Pi_{g}$ resonance, greatly increased cross sections for both processes, and the threshold moving to lower "},"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":"1501.01771","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2015-01-08T09:15:44Z","cross_cats_sorted":["physics.atom-ph","physics.chem-ph"],"title_canon_sha256":"e49e71c9973f2b2f89320ba3d0600691f765496f809aab588092fa77040d7174","abstract_canon_sha256":"e5a8e3a6621e0c3cd16c001984e4b8ed73cb30e43f37b02eb8bf66dc107e1524"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:29:46.412329Z","signature_b64":"slRkoFeBKiPIyOFg4bS6FQeUcE5kSIFNrGyKimHPBQY3HT5A7maVKl9tylPweJn/PSL0MxFlQtu9GW5NBYSpAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5a28512cba47d186ee54bc5f1e26359ac50f1b33226a44801e6346cf3b09ed6f","last_reissued_at":"2026-05-18T02:29:46.411949Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:29:46.411949Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dissociative electron attachment and electron-impact resonant dissociation of vibrationally excited O2 molecules","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph","physics.chem-ph"],"primary_cat":"physics.plasm-ph","authors_text":"J. Tennyson, R. Celiberto, V. Laporta","submitted_at":"2015-01-08T09:15:44Z","abstract_excerpt":"State-by-state cross sections for dissociative electron attachment and electron-impact dissociation for molecular oxygen are computed using ab initio resonance curves calculated with the R-matrix method. When O2 is in its vibrational ground state, the main contribution for both processes comes from the $^2\\Pi_u$ resonance state of $O_2^-$ but with a significant contribution from the $^4\\Sigma$ resonant state. Vibrational excitation leads to an increased contribution from the low-lying $^2\\Pi_{g}$ resonance, greatly increased cross sections for both processes, and the threshold moving to lower "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.01771","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":"1501.01771","created_at":"2026-05-18T02:29:46.412003+00:00"},{"alias_kind":"arxiv_version","alias_value":"1501.01771v1","created_at":"2026-05-18T02:29:46.412003+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.01771","created_at":"2026-05-18T02:29:46.412003+00:00"},{"alias_kind":"pith_short_12","alias_value":"LIUFCLF2I7IY","created_at":"2026-05-18T12:29:29.992203+00:00"},{"alias_kind":"pith_short_16","alias_value":"LIUFCLF2I7IYN3SU","created_at":"2026-05-18T12:29:29.992203+00:00"},{"alias_kind":"pith_short_8","alias_value":"LIUFCLF2","created_at":"2026-05-18T12:29:29.992203+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/LIUFCLF2I7IYN3SUXRPR4JRVTL","json":"https://pith.science/pith/LIUFCLF2I7IYN3SUXRPR4JRVTL.json","graph_json":"https://pith.science/api/pith-number/LIUFCLF2I7IYN3SUXRPR4JRVTL/graph.json","events_json":"https://pith.science/api/pith-number/LIUFCLF2I7IYN3SUXRPR4JRVTL/events.json","paper":"https://pith.science/paper/LIUFCLF2"},"agent_actions":{"view_html":"https://pith.science/pith/LIUFCLF2I7IYN3SUXRPR4JRVTL","download_json":"https://pith.science/pith/LIUFCLF2I7IYN3SUXRPR4JRVTL.json","view_paper":"https://pith.science/paper/LIUFCLF2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1501.01771&json=true","fetch_graph":"https://pith.science/api/pith-number/LIUFCLF2I7IYN3SUXRPR4JRVTL/graph.json","fetch_events":"https://pith.science/api/pith-number/LIUFCLF2I7IYN3SUXRPR4JRVTL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LIUFCLF2I7IYN3SUXRPR4JRVTL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LIUFCLF2I7IYN3SUXRPR4JRVTL/action/storage_attestation","attest_author":"https://pith.science/pith/LIUFCLF2I7IYN3SUXRPR4JRVTL/action/author_attestation","sign_citation":"https://pith.science/pith/LIUFCLF2I7IYN3SUXRPR4JRVTL/action/citation_signature","submit_replication":"https://pith.science/pith/LIUFCLF2I7IYN3SUXRPR4JRVTL/action/replication_record"}},"created_at":"2026-05-18T02:29:46.412003+00:00","updated_at":"2026-05-18T02:29:46.412003+00:00"}