{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:WDPCQGPDYE5AFI42AHYQFICE2Y","short_pith_number":"pith:WDPCQGPD","schema_version":"1.0","canonical_sha256":"b0de2819e3c13a02a39a01f102a044d608e560d8427b295a2381d07c7f5e032a","source":{"kind":"arxiv","id":"1402.6375","version":1},"attestation_state":"computed","paper":{"title":"Effects of Reagent Rotation and Vibration on H + OH (v,j) $\\to$ O + H2","license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","headline":"","cross_cats":[],"primary_cat":"astro-ph.SR","authors_text":"Carina Arasa, Ewine F. van Dishoeck, Marc C. van Hemert, Xiaohu Li","submitted_at":"2014-02-25T23:53:30Z","abstract_excerpt":"The dynamics of the reaction H + OH $\\to$ O (3P) + H2 have been studied in a series of quasi-classical trajectory (QCT) calculations and transition state theory (TST) methods using high quality 3A' and 3A'' potential energy surfaces (PESs). Accurate OH (v, j) state resolved cross sections and rate constants on both potential energy surfaces are presented and fitted for OH at (v = 0, j = 0-16) and (v = 1, j = 0-6). The cross sections were calculated for different collisional energies (Ec), ranging from the threshold energy at each specific rovibrational state up to 1.0 eV with step sizes of 0.1"},"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":"1402.6375","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"astro-ph.SR","submitted_at":"2014-02-25T23:53:30Z","cross_cats_sorted":[],"title_canon_sha256":"4c040668dafbdef04f4bee456bf6e65a5930953dcb0fcd3b8f905748c2aa079c","abstract_canon_sha256":"47b354796645dfa3a55930d2b53f1bb86575b1bff493ca222b79279f07ae9100"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:57:44.659624Z","signature_b64":"/hhvKzjeIG2yyq/S+TBgy45dGIK6sGlbGYphrsqLSwEa2Nesf54BiTXkc25eYn/LWgNt8v25ApgxUZDwB3sSBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b0de2819e3c13a02a39a01f102a044d608e560d8427b295a2381d07c7f5e032a","last_reissued_at":"2026-05-18T02:57:44.659184Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:57:44.659184Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effects of Reagent Rotation and Vibration on H + OH (v,j) $\\to$ O + H2","license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","headline":"","cross_cats":[],"primary_cat":"astro-ph.SR","authors_text":"Carina Arasa, Ewine F. van Dishoeck, Marc C. van Hemert, Xiaohu Li","submitted_at":"2014-02-25T23:53:30Z","abstract_excerpt":"The dynamics of the reaction H + OH $\\to$ O (3P) + H2 have been studied in a series of quasi-classical trajectory (QCT) calculations and transition state theory (TST) methods using high quality 3A' and 3A'' potential energy surfaces (PESs). Accurate OH (v, j) state resolved cross sections and rate constants on both potential energy surfaces are presented and fitted for OH at (v = 0, j = 0-16) and (v = 1, j = 0-6). The cross sections were calculated for different collisional energies (Ec), ranging from the threshold energy at each specific rovibrational state up to 1.0 eV with step sizes of 0.1"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.6375","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":"1402.6375","created_at":"2026-05-18T02:57:44.659248+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.6375v1","created_at":"2026-05-18T02:57:44.659248+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.6375","created_at":"2026-05-18T02:57:44.659248+00:00"},{"alias_kind":"pith_short_12","alias_value":"WDPCQGPDYE5A","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_16","alias_value":"WDPCQGPDYE5AFI42","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_8","alias_value":"WDPCQGPD","created_at":"2026-05-18T12:28:54.890064+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/WDPCQGPDYE5AFI42AHYQFICE2Y","json":"https://pith.science/pith/WDPCQGPDYE5AFI42AHYQFICE2Y.json","graph_json":"https://pith.science/api/pith-number/WDPCQGPDYE5AFI42AHYQFICE2Y/graph.json","events_json":"https://pith.science/api/pith-number/WDPCQGPDYE5AFI42AHYQFICE2Y/events.json","paper":"https://pith.science/paper/WDPCQGPD"},"agent_actions":{"view_html":"https://pith.science/pith/WDPCQGPDYE5AFI42AHYQFICE2Y","download_json":"https://pith.science/pith/WDPCQGPDYE5AFI42AHYQFICE2Y.json","view_paper":"https://pith.science/paper/WDPCQGPD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.6375&json=true","fetch_graph":"https://pith.science/api/pith-number/WDPCQGPDYE5AFI42AHYQFICE2Y/graph.json","fetch_events":"https://pith.science/api/pith-number/WDPCQGPDYE5AFI42AHYQFICE2Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WDPCQGPDYE5AFI42AHYQFICE2Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WDPCQGPDYE5AFI42AHYQFICE2Y/action/storage_attestation","attest_author":"https://pith.science/pith/WDPCQGPDYE5AFI42AHYQFICE2Y/action/author_attestation","sign_citation":"https://pith.science/pith/WDPCQGPDYE5AFI42AHYQFICE2Y/action/citation_signature","submit_replication":"https://pith.science/pith/WDPCQGPDYE5AFI42AHYQFICE2Y/action/replication_record"}},"created_at":"2026-05-18T02:57:44.659248+00:00","updated_at":"2026-05-18T02:57:44.659248+00:00"}