{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:KPZOWHDTRAT7CQYMBOUJ2OMVMY","short_pith_number":"pith:KPZOWHDT","canonical_record":{"source":{"id":"1206.2268","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2012-06-11T15:58:27Z","cross_cats_sorted":["physics.plasm-ph"],"title_canon_sha256":"b8f08bf0b38b88ef021faab7dc2bfcd2efcc5474535af53a8b803e9d7504700e","abstract_canon_sha256":"024f8bb63841403230a88cd82baa83021d6f9ecf6ba2256f08ae3e90f37669e4"},"schema_version":"1.0"},"canonical_sha256":"53f2eb1c738827f1430c0ba89d3995663f0b66773be7c71c00a44d8d2359218b","source":{"kind":"arxiv","id":"1206.2268","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1206.2268","created_at":"2026-05-18T03:48:58Z"},{"alias_kind":"arxiv_version","alias_value":"1206.2268v1","created_at":"2026-05-18T03:48:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.2268","created_at":"2026-05-18T03:48:58Z"},{"alias_kind":"pith_short_12","alias_value":"KPZOWHDTRAT7","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_16","alias_value":"KPZOWHDTRAT7CQYM","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_8","alias_value":"KPZOWHDT","created_at":"2026-05-18T12:27:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:KPZOWHDTRAT7CQYMBOUJ2OMVMY","target":"record","payload":{"canonical_record":{"source":{"id":"1206.2268","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2012-06-11T15:58:27Z","cross_cats_sorted":["physics.plasm-ph"],"title_canon_sha256":"b8f08bf0b38b88ef021faab7dc2bfcd2efcc5474535af53a8b803e9d7504700e","abstract_canon_sha256":"024f8bb63841403230a88cd82baa83021d6f9ecf6ba2256f08ae3e90f37669e4"},"schema_version":"1.0"},"canonical_sha256":"53f2eb1c738827f1430c0ba89d3995663f0b66773be7c71c00a44d8d2359218b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:48:58.648068Z","signature_b64":"KLu9CrBHQRjld/BDq/qwtVB9DIOSp3iS6fCY9SEXDgRprEsnq1ieoLeFDfn87UvPWYyBa7QRuJxCCyCP4uSFBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"53f2eb1c738827f1430c0ba89d3995663f0b66773be7c71c00a44d8d2359218b","last_reissued_at":"2026-05-18T03:48:58.647541Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:48:58.647541Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1206.2268","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:48:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0yMdEAmM6jjhuans2GcvoGM2IsYVn1rrkvJP7iunh7sHlfdIe6cpbJF87lEEYkdRyiV1ZV9sMU/YJ3G6Ne+hDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-19T16:55:53.065622Z"},"content_sha256":"b0e81524472c234666823ebb08ea786a75c6f46ece98cc4d1dae1cbf0e936f64","schema_version":"1.0","event_id":"sha256:b0e81524472c234666823ebb08ea786a75c6f46ece98cc4d1dae1cbf0e936f64"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:KPZOWHDTRAT7CQYMBOUJ2OMVMY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Electron--impact resonant vibration excitation cross sections and rate coefficients for carbon monoxide","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.plasm-ph"],"primary_cat":"physics.chem-ph","authors_text":"C. M. Cassidy, J. Tennyson, R. Celiberto, V. Laporta","submitted_at":"2012-06-11T15:58:27Z","abstract_excerpt":"Resonant vibrational and rotation-vibration excitation cross sections for electron-CO scattering are calculated in the 0-10 eV energy range for all 81 vibrational states of CO, assuming that the excitation occur via the 2{\\Pi} shape resonance. Static exchange plus polarization calculations performed using the R-matrix method are used to estimate resonance positions and widths as functions of internuclear separation. The effects of nuclear motion are considered using a local complex potential model. Good agreement is obtained with available experimental data on excitation from the vibrational g"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.2268","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:48:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Eb2E2TR7L6K4FMliEsCRSHIZMXgrjdbm68DQHNWFgwdIraxEyk3n8NEEYfA5R3DiElr2dzkUCl3TOjmhSZOAAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-19T16:55:53.065969Z"},"content_sha256":"931690b5e0b3848a85fc2285e3fd20298a97316d1144c33256eea82f8b3691a0","schema_version":"1.0","event_id":"sha256:931690b5e0b3848a85fc2285e3fd20298a97316d1144c33256eea82f8b3691a0"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KPZOWHDTRAT7CQYMBOUJ2OMVMY/bundle.json","state_url":"https://pith.science/pith/KPZOWHDTRAT7CQYMBOUJ2OMVMY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KPZOWHDTRAT7CQYMBOUJ2OMVMY/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-19T16:55:53Z","links":{"resolver":"https://pith.science/pith/KPZOWHDTRAT7CQYMBOUJ2OMVMY","bundle":"https://pith.science/pith/KPZOWHDTRAT7CQYMBOUJ2OMVMY/bundle.json","state":"https://pith.science/pith/KPZOWHDTRAT7CQYMBOUJ2OMVMY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KPZOWHDTRAT7CQYMBOUJ2OMVMY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:KPZOWHDTRAT7CQYMBOUJ2OMVMY","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"024f8bb63841403230a88cd82baa83021d6f9ecf6ba2256f08ae3e90f37669e4","cross_cats_sorted":["physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2012-06-11T15:58:27Z","title_canon_sha256":"b8f08bf0b38b88ef021faab7dc2bfcd2efcc5474535af53a8b803e9d7504700e"},"schema_version":"1.0","source":{"id":"1206.2268","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1206.2268","created_at":"2026-05-18T03:48:58Z"},{"alias_kind":"arxiv_version","alias_value":"1206.2268v1","created_at":"2026-05-18T03:48:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.2268","created_at":"2026-05-18T03:48:58Z"},{"alias_kind":"pith_short_12","alias_value":"KPZOWHDTRAT7","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_16","alias_value":"KPZOWHDTRAT7CQYM","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_8","alias_value":"KPZOWHDT","created_at":"2026-05-18T12:27:11Z"}],"graph_snapshots":[{"event_id":"sha256:931690b5e0b3848a85fc2285e3fd20298a97316d1144c33256eea82f8b3691a0","target":"graph","created_at":"2026-05-18T03:48:58Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"Resonant vibrational and rotation-vibration excitation cross sections for electron-CO scattering are calculated in the 0-10 eV energy range for all 81 vibrational states of CO, assuming that the excitation occur via the 2{\\Pi} shape resonance. Static exchange plus polarization calculations performed using the R-matrix method are used to estimate resonance positions and widths as functions of internuclear separation. The effects of nuclear motion are considered using a local complex potential model. Good agreement is obtained with available experimental data on excitation from the vibrational g","authors_text":"C. M. Cassidy, J. Tennyson, R. Celiberto, V. Laporta","cross_cats":["physics.plasm-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2012-06-11T15:58:27Z","title":"Electron--impact resonant vibration excitation cross sections and rate coefficients for carbon monoxide"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.2268","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:b0e81524472c234666823ebb08ea786a75c6f46ece98cc4d1dae1cbf0e936f64","target":"record","created_at":"2026-05-18T03:48:58Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"024f8bb63841403230a88cd82baa83021d6f9ecf6ba2256f08ae3e90f37669e4","cross_cats_sorted":["physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2012-06-11T15:58:27Z","title_canon_sha256":"b8f08bf0b38b88ef021faab7dc2bfcd2efcc5474535af53a8b803e9d7504700e"},"schema_version":"1.0","source":{"id":"1206.2268","kind":"arxiv","version":1}},"canonical_sha256":"53f2eb1c738827f1430c0ba89d3995663f0b66773be7c71c00a44d8d2359218b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"53f2eb1c738827f1430c0ba89d3995663f0b66773be7c71c00a44d8d2359218b","first_computed_at":"2026-05-18T03:48:58.647541Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:48:58.647541Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"KLu9CrBHQRjld/BDq/qwtVB9DIOSp3iS6fCY9SEXDgRprEsnq1ieoLeFDfn87UvPWYyBa7QRuJxCCyCP4uSFBA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:48:58.648068Z","signed_message":"canonical_sha256_bytes"},"source_id":"1206.2268","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b0e81524472c234666823ebb08ea786a75c6f46ece98cc4d1dae1cbf0e936f64","sha256:931690b5e0b3848a85fc2285e3fd20298a97316d1144c33256eea82f8b3691a0"],"state_sha256":"ea1f32496f8897f8828a096be80dad2dcf36a2d000c725799dd3e9a4b0b05b21"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vifmpDCsuRQh6hSMNtlUNDxwgv7TLyRUpdDHzha26e83ed/V4gIGtOxrw6HaS8gUrJGC2gAi6KUJ1O9s7WFJBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-19T16:55:53.067995Z","bundle_sha256":"95a5a1dd346a7fb7ccdb8a0bc82dfbac03694d88885ab1badd75538c426dc72d"}}