{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:VKBUIDQUPAWD7ZR6SXJN7KEXQE","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":"52f79fae8608e47b60690f0d1f9a3e66adf75ffeeadf26bb6d1aa27968e0855a","cross_cats_sorted":["physics.comp-ph"],"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2023-07-18T12:51:40Z","title_canon_sha256":"2cff4aeef2436edc00376f8b892bcba9765e9c8e60193de889094adc5c041623"},"schema_version":"1.0","source":{"id":"2307.09217","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2307.09217","created_at":"2026-07-05T06:34:06Z"},{"alias_kind":"arxiv_version","alias_value":"2307.09217v2","created_at":"2026-07-05T06:34:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2307.09217","created_at":"2026-07-05T06:34:06Z"},{"alias_kind":"pith_short_12","alias_value":"VKBUIDQUPAWD","created_at":"2026-07-05T06:34:06Z"},{"alias_kind":"pith_short_16","alias_value":"VKBUIDQUPAWD7ZR6","created_at":"2026-07-05T06:34:06Z"},{"alias_kind":"pith_short_8","alias_value":"VKBUIDQU","created_at":"2026-07-05T06:34:06Z"}],"graph_snapshots":[{"event_id":"sha256:77eb6d103c3df66827c8e47f818d0a3d012701885e003012748136bf4b8272ba","target":"graph","created_at":"2026-07-05T06:34:06Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2307.09217/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The potential energy curves for molecular ions up to $N_2^{4+}$ are calculated in an ab initio manner using the multi configurational self-consistent field method. Specifically, we implement in an automatic way a previously used double loop optimisation scheme within the multi configurational self-consisted field method. We obtain the potential energy curves up to $N_2^{4+}$ ions with any combination of core, inner valence, and outer valence holes. Finally, we provide the code used to generate these potential energy curves.","authors_text":"Agapi Emmanouilidou, Antonis Hadjipittas","cross_cats":["physics.comp-ph"],"headline":"","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2023-07-18T12:51:40Z","title":"Potential energy curves of molecular nitrogen up to $N_2^{4+}$"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2307.09217","kind":"arxiv","version":2},"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:b35e7819f5f54a3be9bc23a652ed9774ee11b90ec8bbd926687801408be4ef48","target":"record","created_at":"2026-07-05T06:34:06Z","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":"52f79fae8608e47b60690f0d1f9a3e66adf75ffeeadf26bb6d1aa27968e0855a","cross_cats_sorted":["physics.comp-ph"],"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2023-07-18T12:51:40Z","title_canon_sha256":"2cff4aeef2436edc00376f8b892bcba9765e9c8e60193de889094adc5c041623"},"schema_version":"1.0","source":{"id":"2307.09217","kind":"arxiv","version":2}},"canonical_sha256":"aa83440e14782c3fe63e95d2dfa8978138865906eabf5c8fb8829a807cdd3d68","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"aa83440e14782c3fe63e95d2dfa8978138865906eabf5c8fb8829a807cdd3d68","first_computed_at":"2026-07-05T06:34:06.772078Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:34:06.772078Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"+FkxdbTSlKcJz75hJf53GTyjVRJKVXs7YGMQP6n0i52T16wf0yvH6HvLZ7JLFt+91b7T9uN5hO4+PATWXSbYDA==","signature_status":"signed_v1","signed_at":"2026-07-05T06:34:06.772464Z","signed_message":"canonical_sha256_bytes"},"source_id":"2307.09217","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b35e7819f5f54a3be9bc23a652ed9774ee11b90ec8bbd926687801408be4ef48","sha256:77eb6d103c3df66827c8e47f818d0a3d012701885e003012748136bf4b8272ba"],"state_sha256":"e7f6c1b973c6ce037a15aed6b6c4a01e4c0d0b62e2639d409e3677fbea1b356d"}