{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:4BQEUHZDCNNLBJOPTXG774BK4D","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":"9bc9c293feabc998783b45167066ca38ab052094393b147059c1623b91503e23","cross_cats_sorted":["physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2015-06-26T16:12:52Z","title_canon_sha256":"cd97bb753a8235f70ee33d62215253b13846f4769836ffb784b19ffd70c598bd"},"schema_version":"1.0","source":{"id":"1506.08136","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1506.08136","created_at":"2026-05-18T01:37:47Z"},{"alias_kind":"arxiv_version","alias_value":"1506.08136v1","created_at":"2026-05-18T01:37:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1506.08136","created_at":"2026-05-18T01:37:47Z"},{"alias_kind":"pith_short_12","alias_value":"4BQEUHZDCNNL","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_16","alias_value":"4BQEUHZDCNNLBJOP","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_8","alias_value":"4BQEUHZD","created_at":"2026-05-18T12:29:05Z"}],"graph_snapshots":[{"event_id":"sha256:7a860e37d800939e91c0578f543fbef47fc26604611f556618506e63643f2704","target":"graph","created_at":"2026-05-18T01:37:47Z","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":"Electron-impact cross sections for the dissociation process of vibrationally excited He2+ molecular ion, as a function of the incident electron energy are calculated for the dissociative transition X2\\Sigma+u \\to A2\\Sigma+g by using the R-matrix method in the adiabatic-nuclei approximation. The potential energy curves for the involved electronic states and target properties, also calculated with the R-matrix method, were found to be in good agreement with the results reported in literature.","authors_text":"K.L. Baluja, R. Celiberto, R.K. Janev, V. Laporta","cross_cats":["physics.atom-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2015-06-26T16:12:52Z","title":"Electron-impact dissociation cross sections of vibrationally excited He2+ molecular ion"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1506.08136","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":"sha256:210d8cfe39eda57102ba5a5bfc911d4b0b62ea5db6154e47e199dba3f0511647","target":"record","created_at":"2026-05-18T01:37:47Z","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":"9bc9c293feabc998783b45167066ca38ab052094393b147059c1623b91503e23","cross_cats_sorted":["physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2015-06-26T16:12:52Z","title_canon_sha256":"cd97bb753a8235f70ee33d62215253b13846f4769836ffb784b19ffd70c598bd"},"schema_version":"1.0","source":{"id":"1506.08136","kind":"arxiv","version":1}},"canonical_sha256":"e0604a1f23135ab0a5cf9dcdfff02ae0dabfbe7faef96b4eda7edeeae8b6ad25","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e0604a1f23135ab0a5cf9dcdfff02ae0dabfbe7faef96b4eda7edeeae8b6ad25","first_computed_at":"2026-05-18T01:37:47.968193Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:37:47.968193Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"rmpKar9PcmFNUnmX6XkpLYOrhcXFInDRC4zzEYDRS7oA+p6Pl0myM15uH1CIR4/4cNHjQyR1egkQInRow98xAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:37:47.968635Z","signed_message":"canonical_sha256_bytes"},"source_id":"1506.08136","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:210d8cfe39eda57102ba5a5bfc911d4b0b62ea5db6154e47e199dba3f0511647","sha256:7a860e37d800939e91c0578f543fbef47fc26604611f556618506e63643f2704"],"state_sha256":"2d7997fd0601a570b7f0cd7de76f26f8ac2bca581d184acd403bccf8c77278b2"}