{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2007:HKKDEZL5WZ5STPUPB34K6WHYHD","short_pith_number":"pith:HKKDEZL5","canonical_record":{"source":{"id":"0708.2715","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"physics.atom-ph","submitted_at":"2007-08-20T23:42:03Z","cross_cats_sorted":[],"title_canon_sha256":"1aa24a3f19397291a6081559e5949a48a847cea0ca69f2aae60862c657610994","abstract_canon_sha256":"33cd33cff570b95d9503613dba07b25ed2c0b06b55ffd72293832d607303ab0a"},"schema_version":"1.0"},"canonical_sha256":"3a9432657db67b29be8f0ef8af58f838daaad35396497e9b8d0707dfeb6c92ae","source":{"kind":"arxiv","id":"0708.2715","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0708.2715","created_at":"2026-07-04T15:03:43Z"},{"alias_kind":"arxiv_version","alias_value":"0708.2715v1","created_at":"2026-07-04T15:03:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0708.2715","created_at":"2026-07-04T15:03:43Z"},{"alias_kind":"pith_short_12","alias_value":"HKKDEZL5WZ5S","created_at":"2026-07-04T15:03:43Z"},{"alias_kind":"pith_short_16","alias_value":"HKKDEZL5WZ5STPUP","created_at":"2026-07-04T15:03:43Z"},{"alias_kind":"pith_short_8","alias_value":"HKKDEZL5","created_at":"2026-07-04T15:03:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2007:HKKDEZL5WZ5STPUPB34K6WHYHD","target":"record","payload":{"canonical_record":{"source":{"id":"0708.2715","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"physics.atom-ph","submitted_at":"2007-08-20T23:42:03Z","cross_cats_sorted":[],"title_canon_sha256":"1aa24a3f19397291a6081559e5949a48a847cea0ca69f2aae60862c657610994","abstract_canon_sha256":"33cd33cff570b95d9503613dba07b25ed2c0b06b55ffd72293832d607303ab0a"},"schema_version":"1.0"},"canonical_sha256":"3a9432657db67b29be8f0ef8af58f838daaad35396497e9b8d0707dfeb6c92ae","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:03:43.948335Z","signature_b64":"K/MDdmZphC210Y5UylLOchRP69ZULw6kmJFNoz4BTsX7oafcvm7JBP+bReNmdeHeM3QU13XnfssM9jfjUNdsDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3a9432657db67b29be8f0ef8af58f838daaad35396497e9b8d0707dfeb6c92ae","last_reissued_at":"2026-07-04T15:03:43.947998Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:03:43.947998Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0708.2715","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":"2026-07-04T15:03:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fR+THnRbKJGNU1OHGMATK4XIy0sQddKv5CRbBwdvVidSoi0odRHihTN91uZ0984aqyK/uLd4X6lfxv5mKOwtDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-01T06:09:37.193550Z"},"content_sha256":"8972c269aabd4e531cf45a13f625b38b480dfb898f787f9c9fd6807d541fa73a","schema_version":"1.0","event_id":"sha256:8972c269aabd4e531cf45a13f625b38b480dfb898f787f9c9fd6807d541fa73a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2007:HKKDEZL5WZ5STPUPB34K6WHYHD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dissociative recombination of H3+ in the ground and excited vibrational states","license":"","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Chris H. Greene, Samantha Fonseca dos Santos, Viatcheslav Kokoouline","submitted_at":"2007-08-20T23:42:03Z","abstract_excerpt":"The article presents calculated dissociative recombination (DR) rate coefficients for H+3 . The previous theoretical work on H+3 was performed using the adiabatic hyperspherical approximation to calculate the target ion vibrational states and it considered just a limited number of ionic rotational states. In this study, we use accurate vibrational wave functions and a larger number of possible rotational states of the H3+ ground vibrational level. The DR rate coefficient obtained is found to agree better with the experimental data from storage-ring experiments than the previous theoretical cal"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0708.2715","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/0708.2715/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-04T15:03:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ceFnCu3XYhKK+C9/5nmHvg7J/8xWflHxzyxeHBNnQV2CaMoz3p1o1kUVtyQdKJ5xLN5QBhEP5vYUq6JqYv0ZCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-01T06:09:37.193949Z"},"content_sha256":"4eab83973f91d18d5592ae56b425294bd1868ecff56424796bbe26134a85d96e","schema_version":"1.0","event_id":"sha256:4eab83973f91d18d5592ae56b425294bd1868ecff56424796bbe26134a85d96e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HKKDEZL5WZ5STPUPB34K6WHYHD/bundle.json","state_url":"https://pith.science/pith/HKKDEZL5WZ5STPUPB34K6WHYHD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HKKDEZL5WZ5STPUPB34K6WHYHD/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":"2026-08-01T06:09:37Z","links":{"resolver":"https://pith.science/pith/HKKDEZL5WZ5STPUPB34K6WHYHD","bundle":"https://pith.science/pith/HKKDEZL5WZ5STPUPB34K6WHYHD/bundle.json","state":"https://pith.science/pith/HKKDEZL5WZ5STPUPB34K6WHYHD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HKKDEZL5WZ5STPUPB34K6WHYHD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2007:HKKDEZL5WZ5STPUPB34K6WHYHD","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":"33cd33cff570b95d9503613dba07b25ed2c0b06b55ffd72293832d607303ab0a","cross_cats_sorted":[],"license":"","primary_cat":"physics.atom-ph","submitted_at":"2007-08-20T23:42:03Z","title_canon_sha256":"1aa24a3f19397291a6081559e5949a48a847cea0ca69f2aae60862c657610994"},"schema_version":"1.0","source":{"id":"0708.2715","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0708.2715","created_at":"2026-07-04T15:03:43Z"},{"alias_kind":"arxiv_version","alias_value":"0708.2715v1","created_at":"2026-07-04T15:03:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0708.2715","created_at":"2026-07-04T15:03:43Z"},{"alias_kind":"pith_short_12","alias_value":"HKKDEZL5WZ5S","created_at":"2026-07-04T15:03:43Z"},{"alias_kind":"pith_short_16","alias_value":"HKKDEZL5WZ5STPUP","created_at":"2026-07-04T15:03:43Z"},{"alias_kind":"pith_short_8","alias_value":"HKKDEZL5","created_at":"2026-07-04T15:03:43Z"}],"graph_snapshots":[{"event_id":"sha256:4eab83973f91d18d5592ae56b425294bd1868ecff56424796bbe26134a85d96e","target":"graph","created_at":"2026-07-04T15:03:43Z","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/0708.2715/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The article presents calculated dissociative recombination (DR) rate coefficients for H+3 . The previous theoretical work on H+3 was performed using the adiabatic hyperspherical approximation to calculate the target ion vibrational states and it considered just a limited number of ionic rotational states. In this study, we use accurate vibrational wave functions and a larger number of possible rotational states of the H3+ ground vibrational level. The DR rate coefficient obtained is found to agree better with the experimental data from storage-ring experiments than the previous theoretical cal","authors_text":"Chris H. Greene, Samantha Fonseca dos Santos, Viatcheslav Kokoouline","cross_cats":[],"headline":"","license":"","primary_cat":"physics.atom-ph","submitted_at":"2007-08-20T23:42:03Z","title":"Dissociative recombination of H3+ in the ground and excited vibrational states"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0708.2715","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":"sha256:8972c269aabd4e531cf45a13f625b38b480dfb898f787f9c9fd6807d541fa73a","target":"record","created_at":"2026-07-04T15:03:43Z","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":"33cd33cff570b95d9503613dba07b25ed2c0b06b55ffd72293832d607303ab0a","cross_cats_sorted":[],"license":"","primary_cat":"physics.atom-ph","submitted_at":"2007-08-20T23:42:03Z","title_canon_sha256":"1aa24a3f19397291a6081559e5949a48a847cea0ca69f2aae60862c657610994"},"schema_version":"1.0","source":{"id":"0708.2715","kind":"arxiv","version":1}},"canonical_sha256":"3a9432657db67b29be8f0ef8af58f838daaad35396497e9b8d0707dfeb6c92ae","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3a9432657db67b29be8f0ef8af58f838daaad35396497e9b8d0707dfeb6c92ae","first_computed_at":"2026-07-04T15:03:43.947998Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:03:43.947998Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"K/MDdmZphC210Y5UylLOchRP69ZULw6kmJFNoz4BTsX7oafcvm7JBP+bReNmdeHeM3QU13XnfssM9jfjUNdsDw==","signature_status":"signed_v1","signed_at":"2026-07-04T15:03:43.948335Z","signed_message":"canonical_sha256_bytes"},"source_id":"0708.2715","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8972c269aabd4e531cf45a13f625b38b480dfb898f787f9c9fd6807d541fa73a","sha256:4eab83973f91d18d5592ae56b425294bd1868ecff56424796bbe26134a85d96e"],"state_sha256":"b6f588f5a9ba5173cee164d7e5e672b1aeb24a3e3c7b84fc84f18b476a73183e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"REo+LvB4oG2mKTYJMdVmBCv542yvCmfWRQ6LVCBRwXHuMbYfVhCUL0mbPeKbAsscJETBSiujDk0HdxmP0xuaCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-01T06:09:37.197876Z","bundle_sha256":"c4cdd899ad1676c01130243717a55b013ed824211e5565910564fa789a71b80f"}}