{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:UL4DW2LJEVNCQAVQBOFALDHYWD","short_pith_number":"pith:UL4DW2LJ","canonical_record":{"source":{"id":"1105.5882","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2011-05-30T07:12:25Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"a3b3a0bafcfb64ee5579a86d784646b263804f18c0839d4a5c37e4b615dee01c","abstract_canon_sha256":"87053bc64e0cccef9871e6addc4d3ec56065dae44ce67559ae6f5062163fcefc"},"schema_version":"1.0"},"canonical_sha256":"a2f83b6969255a2802b00b8a058cf8b0fa3025f3da54e6a188c91a7eaa342504","source":{"kind":"arxiv","id":"1105.5882","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1105.5882","created_at":"2026-05-18T04:21:01Z"},{"alias_kind":"arxiv_version","alias_value":"1105.5882v1","created_at":"2026-05-18T04:21:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.5882","created_at":"2026-05-18T04:21:01Z"},{"alias_kind":"pith_short_12","alias_value":"UL4DW2LJEVNC","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"UL4DW2LJEVNCQAVQ","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"UL4DW2LJ","created_at":"2026-05-18T12:26:42Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:UL4DW2LJEVNCQAVQBOFALDHYWD","target":"record","payload":{"canonical_record":{"source":{"id":"1105.5882","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2011-05-30T07:12:25Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"a3b3a0bafcfb64ee5579a86d784646b263804f18c0839d4a5c37e4b615dee01c","abstract_canon_sha256":"87053bc64e0cccef9871e6addc4d3ec56065dae44ce67559ae6f5062163fcefc"},"schema_version":"1.0"},"canonical_sha256":"a2f83b6969255a2802b00b8a058cf8b0fa3025f3da54e6a188c91a7eaa342504","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:21:01.325477Z","signature_b64":"2cNwHep1iQf4ycZ6aTr1KZDbmErgkCVHTj9P6IrbbObjBoauuF0sR0Y2zuQXvUhrNpNaOx6xpbX9YbZMwAHwBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a2f83b6969255a2802b00b8a058cf8b0fa3025f3da54e6a188c91a7eaa342504","last_reissued_at":"2026-05-18T04:21:01.324853Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:21:01.324853Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1105.5882","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":"2026-05-18T04:21:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fEqLH6LdvCeDueMwzEzvmoibGtGPNrlVviQvMF3a8LTmnT05mwjbZpRdq+FCUAn7Uh8Gw5q2A2CDNXT6oRO6Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T14:36:26.796166Z"},"content_sha256":"6655bcc9dc9b0c6bcc407aceb8cf53d5b4c9d7133c4317c433d66f4404a50983","schema_version":"1.0","event_id":"sha256:6655bcc9dc9b0c6bcc407aceb8cf53d5b4c9d7133c4317c433d66f4404a50983"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:UL4DW2LJEVNCQAVQBOFALDHYWD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Reevaluation of the $^{14}$O($\\alpha$,p)$^{17}$F Resonant Reaction Rate","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"astro-ph.SR","authors_text":"H.W. Wang, J. Hu, J.J. He, S.W. Xu","submitted_at":"2011-05-30T07:12:25Z","abstract_excerpt":"The reaction rates of the key stellar reaction of $^{14}$O($\\alpha$,p)$^{17}$F have been reevaluated. It is thought that the previous 1$^-$ assignment for the 6.15-MeV state is incorrect by a careful reanalysis of the previous experimental data [J. G\\'{o}mez del Campo {\\it et al.}, Phys. Rev. Lett. {\\bf 86}, 43 (2001)]. Most probably, the 6.286-MeV state is the key 1$^-$ state and the 6.15-MeV state is a 2$^-$ one, and hence the resonance at $E_x$=6.286 MeV ($J^{\\pi}$=1$^-$) actually dominates the reaction rates in the temperature region of astrophysical interests. The newly calculated reactio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.5882","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":"2026-05-18T04:21:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bzziCibywZ/sN7dRhLhwFGq+bkBXeKvM03f1F4tdr6cvwH7++VXL6Sjy3sg3+g7vQPVtsjLJbovRSJK1d1V9Bw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T14:36:26.796817Z"},"content_sha256":"8600e0a0f8d685b9680fb8cf70312e7a745960250091efd4c85e1b7562d9d118","schema_version":"1.0","event_id":"sha256:8600e0a0f8d685b9680fb8cf70312e7a745960250091efd4c85e1b7562d9d118"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UL4DW2LJEVNCQAVQBOFALDHYWD/bundle.json","state_url":"https://pith.science/pith/UL4DW2LJEVNCQAVQBOFALDHYWD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UL4DW2LJEVNCQAVQBOFALDHYWD/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":"2026-05-29T14:36:26Z","links":{"resolver":"https://pith.science/pith/UL4DW2LJEVNCQAVQBOFALDHYWD","bundle":"https://pith.science/pith/UL4DW2LJEVNCQAVQBOFALDHYWD/bundle.json","state":"https://pith.science/pith/UL4DW2LJEVNCQAVQBOFALDHYWD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UL4DW2LJEVNCQAVQBOFALDHYWD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:UL4DW2LJEVNCQAVQBOFALDHYWD","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":"87053bc64e0cccef9871e6addc4d3ec56065dae44ce67559ae6f5062163fcefc","cross_cats_sorted":["nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2011-05-30T07:12:25Z","title_canon_sha256":"a3b3a0bafcfb64ee5579a86d784646b263804f18c0839d4a5c37e4b615dee01c"},"schema_version":"1.0","source":{"id":"1105.5882","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1105.5882","created_at":"2026-05-18T04:21:01Z"},{"alias_kind":"arxiv_version","alias_value":"1105.5882v1","created_at":"2026-05-18T04:21:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.5882","created_at":"2026-05-18T04:21:01Z"},{"alias_kind":"pith_short_12","alias_value":"UL4DW2LJEVNC","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"UL4DW2LJEVNCQAVQ","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"UL4DW2LJ","created_at":"2026-05-18T12:26:42Z"}],"graph_snapshots":[{"event_id":"sha256:8600e0a0f8d685b9680fb8cf70312e7a745960250091efd4c85e1b7562d9d118","target":"graph","created_at":"2026-05-18T04:21:01Z","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":"The reaction rates of the key stellar reaction of $^{14}$O($\\alpha$,p)$^{17}$F have been reevaluated. It is thought that the previous 1$^-$ assignment for the 6.15-MeV state is incorrect by a careful reanalysis of the previous experimental data [J. G\\'{o}mez del Campo {\\it et al.}, Phys. Rev. Lett. {\\bf 86}, 43 (2001)]. Most probably, the 6.286-MeV state is the key 1$^-$ state and the 6.15-MeV state is a 2$^-$ one, and hence the resonance at $E_x$=6.286 MeV ($J^{\\pi}$=1$^-$) actually dominates the reaction rates in the temperature region of astrophysical interests. The newly calculated reactio","authors_text":"H.W. Wang, J. Hu, J.J. He, S.W. Xu","cross_cats":["nucl-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2011-05-30T07:12:25Z","title":"Reevaluation of the $^{14}$O($\\alpha$,p)$^{17}$F Resonant Reaction Rate"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.5882","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":"sha256:6655bcc9dc9b0c6bcc407aceb8cf53d5b4c9d7133c4317c433d66f4404a50983","target":"record","created_at":"2026-05-18T04:21:01Z","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":"87053bc64e0cccef9871e6addc4d3ec56065dae44ce67559ae6f5062163fcefc","cross_cats_sorted":["nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2011-05-30T07:12:25Z","title_canon_sha256":"a3b3a0bafcfb64ee5579a86d784646b263804f18c0839d4a5c37e4b615dee01c"},"schema_version":"1.0","source":{"id":"1105.5882","kind":"arxiv","version":1}},"canonical_sha256":"a2f83b6969255a2802b00b8a058cf8b0fa3025f3da54e6a188c91a7eaa342504","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a2f83b6969255a2802b00b8a058cf8b0fa3025f3da54e6a188c91a7eaa342504","first_computed_at":"2026-05-18T04:21:01.324853Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:21:01.324853Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2cNwHep1iQf4ycZ6aTr1KZDbmErgkCVHTj9P6IrbbObjBoauuF0sR0Y2zuQXvUhrNpNaOx6xpbX9YbZMwAHwBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T04:21:01.325477Z","signed_message":"canonical_sha256_bytes"},"source_id":"1105.5882","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6655bcc9dc9b0c6bcc407aceb8cf53d5b4c9d7133c4317c433d66f4404a50983","sha256:8600e0a0f8d685b9680fb8cf70312e7a745960250091efd4c85e1b7562d9d118"],"state_sha256":"df2977f2763f664b1058a19f834b1a83adedc126363f26e813cf765b95dd1cfb"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xvS//cGV0F12//5SkdiPQQdwtl/lvRWxMk8cj/mUTTX548rWO04TRFmHOtzNmVDcXj+XQRn6hv8aLvYIJxAmDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T14:36:26.799892Z","bundle_sha256":"3a09b9c747c3479da62ff40c762d8bdefdf12ba0e1f2ecf78cee50b0383f32e7"}}