{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2019:WR5L7GPAURANMJIM5O3OUEYAHF","short_pith_number":"pith:WR5L7GPA","canonical_record":{"source":{"id":"1902.10553","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-02-27T14:30:09Z","cross_cats_sorted":["nucl-ex","physics.comp-ph"],"title_canon_sha256":"d18ee52426f9f0c5bb6c457c2b03beda7bf5a66076998f2dfc409a73259a4f99","abstract_canon_sha256":"fa368060546b3db22d9a19a8cbe7aaefdbb024e1175438feec8fc4ad11ba22fa"},"schema_version":"1.0"},"canonical_sha256":"b47abf99e0a440d6250cebb6ea130039613af2549079282372433cbb8e13e6c1","source":{"kind":"arxiv","id":"1902.10553","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1902.10553","created_at":"2026-05-17T23:47:25Z"},{"alias_kind":"arxiv_version","alias_value":"1902.10553v1","created_at":"2026-05-17T23:47:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1902.10553","created_at":"2026-05-17T23:47:25Z"},{"alias_kind":"pith_short_12","alias_value":"WR5L7GPAURAN","created_at":"2026-05-18T12:33:30Z"},{"alias_kind":"pith_short_16","alias_value":"WR5L7GPAURANMJIM","created_at":"2026-05-18T12:33:30Z"},{"alias_kind":"pith_short_8","alias_value":"WR5L7GPA","created_at":"2026-05-18T12:33:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2019:WR5L7GPAURANMJIM5O3OUEYAHF","target":"record","payload":{"canonical_record":{"source":{"id":"1902.10553","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-02-27T14:30:09Z","cross_cats_sorted":["nucl-ex","physics.comp-ph"],"title_canon_sha256":"d18ee52426f9f0c5bb6c457c2b03beda7bf5a66076998f2dfc409a73259a4f99","abstract_canon_sha256":"fa368060546b3db22d9a19a8cbe7aaefdbb024e1175438feec8fc4ad11ba22fa"},"schema_version":"1.0"},"canonical_sha256":"b47abf99e0a440d6250cebb6ea130039613af2549079282372433cbb8e13e6c1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:47:25.898370Z","signature_b64":"l4S+BQPHpVgw/Licq9DRZpmI5DwqJfiTs6ddNuHmAZ5OrXkPiY6oIsA1QFZmdZqLsdC2/9e+3bPnUPtvjlcqBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b47abf99e0a440d6250cebb6ea130039613af2549079282372433cbb8e13e6c1","last_reissued_at":"2026-05-17T23:47:25.897685Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:47:25.897685Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1902.10553","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":"2026-05-17T23:47:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"z5oMQOez5mHaHhhPQJlVFjtOzXIl5Zw9Hh+s+gf43VR/w/iYqus+RKvH9Ug7ia/EJ+cY/yYSzhsQ8nU3v8QSAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T19:19:05.971932Z"},"content_sha256":"d66009189df05c8ba16f2bead8ed71bb654bbcdaf63478827d56b3c1285d58d6","schema_version":"1.0","event_id":"sha256:d66009189df05c8ba16f2bead8ed71bb654bbcdaf63478827d56b3c1285d58d6"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2019:WR5L7GPAURANMJIM5O3OUEYAHF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Ab initio calculations of 5H resonant states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex","physics.comp-ph"],"primary_cat":"nucl-th","authors_text":"E. Hiyama, J. Carbonell, R. Lazauskas","submitted_at":"2019-02-27T14:30:09Z","abstract_excerpt":"By solving the 5-body Faddeev-Yakubovsky equations in configuration space with realistic nuclear Hamiltonians we have studied the resonant states of $^5$H isotope. Two different methods, allowing to bypass the exponentially diverging boundary conditions, have been employed providing consistent results. The existence of $^5$H broad J$^{\\pi}$=1/2$^+$,3/2$^+$,5/2$^+$ states as S-matrix poles has been confirmed and compared with the, also calculated, resonant states in $^4$H isotope. We have established that the positions of these resonances only mildly depend on the nuclear interaction model."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1902.10553","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":"2026-05-17T23:47:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"on2AVtaMoy7X5LikIRU8qu8eb3rNSndUxNJg46CbWOEA8j1enGPUwYqssbqjpx2Y0o+/iO/IBa9DvzNsdC3JCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T19:19:05.972277Z"},"content_sha256":"10d425630d8519387cf0e1df2cac193d692205e35a338459e7ac76a30aec4d93","schema_version":"1.0","event_id":"sha256:10d425630d8519387cf0e1df2cac193d692205e35a338459e7ac76a30aec4d93"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WR5L7GPAURANMJIM5O3OUEYAHF/bundle.json","state_url":"https://pith.science/pith/WR5L7GPAURANMJIM5O3OUEYAHF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WR5L7GPAURANMJIM5O3OUEYAHF/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":"2026-06-04T19:19:05Z","links":{"resolver":"https://pith.science/pith/WR5L7GPAURANMJIM5O3OUEYAHF","bundle":"https://pith.science/pith/WR5L7GPAURANMJIM5O3OUEYAHF/bundle.json","state":"https://pith.science/pith/WR5L7GPAURANMJIM5O3OUEYAHF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WR5L7GPAURANMJIM5O3OUEYAHF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:WR5L7GPAURANMJIM5O3OUEYAHF","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":"fa368060546b3db22d9a19a8cbe7aaefdbb024e1175438feec8fc4ad11ba22fa","cross_cats_sorted":["nucl-ex","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-02-27T14:30:09Z","title_canon_sha256":"d18ee52426f9f0c5bb6c457c2b03beda7bf5a66076998f2dfc409a73259a4f99"},"schema_version":"1.0","source":{"id":"1902.10553","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1902.10553","created_at":"2026-05-17T23:47:25Z"},{"alias_kind":"arxiv_version","alias_value":"1902.10553v1","created_at":"2026-05-17T23:47:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1902.10553","created_at":"2026-05-17T23:47:25Z"},{"alias_kind":"pith_short_12","alias_value":"WR5L7GPAURAN","created_at":"2026-05-18T12:33:30Z"},{"alias_kind":"pith_short_16","alias_value":"WR5L7GPAURANMJIM","created_at":"2026-05-18T12:33:30Z"},{"alias_kind":"pith_short_8","alias_value":"WR5L7GPA","created_at":"2026-05-18T12:33:30Z"}],"graph_snapshots":[{"event_id":"sha256:10d425630d8519387cf0e1df2cac193d692205e35a338459e7ac76a30aec4d93","target":"graph","created_at":"2026-05-17T23:47:25Z","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":"By solving the 5-body Faddeev-Yakubovsky equations in configuration space with realistic nuclear Hamiltonians we have studied the resonant states of $^5$H isotope. Two different methods, allowing to bypass the exponentially diverging boundary conditions, have been employed providing consistent results. The existence of $^5$H broad J$^{\\pi}$=1/2$^+$,3/2$^+$,5/2$^+$ states as S-matrix poles has been confirmed and compared with the, also calculated, resonant states in $^4$H isotope. We have established that the positions of these resonances only mildly depend on the nuclear interaction model.","authors_text":"E. Hiyama, J. Carbonell, R. Lazauskas","cross_cats":["nucl-ex","physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-02-27T14:30:09Z","title":"Ab initio calculations of 5H resonant states"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1902.10553","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:d66009189df05c8ba16f2bead8ed71bb654bbcdaf63478827d56b3c1285d58d6","target":"record","created_at":"2026-05-17T23:47:25Z","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":"fa368060546b3db22d9a19a8cbe7aaefdbb024e1175438feec8fc4ad11ba22fa","cross_cats_sorted":["nucl-ex","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-02-27T14:30:09Z","title_canon_sha256":"d18ee52426f9f0c5bb6c457c2b03beda7bf5a66076998f2dfc409a73259a4f99"},"schema_version":"1.0","source":{"id":"1902.10553","kind":"arxiv","version":1}},"canonical_sha256":"b47abf99e0a440d6250cebb6ea130039613af2549079282372433cbb8e13e6c1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b47abf99e0a440d6250cebb6ea130039613af2549079282372433cbb8e13e6c1","first_computed_at":"2026-05-17T23:47:25.897685Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:47:25.897685Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"l4S+BQPHpVgw/Licq9DRZpmI5DwqJfiTs6ddNuHmAZ5OrXkPiY6oIsA1QFZmdZqLsdC2/9e+3bPnUPtvjlcqBg==","signature_status":"signed_v1","signed_at":"2026-05-17T23:47:25.898370Z","signed_message":"canonical_sha256_bytes"},"source_id":"1902.10553","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d66009189df05c8ba16f2bead8ed71bb654bbcdaf63478827d56b3c1285d58d6","sha256:10d425630d8519387cf0e1df2cac193d692205e35a338459e7ac76a30aec4d93"],"state_sha256":"23d513f549770967b536e51ebe99787780ebd9be9f7c0e23bfd110282566f16a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ys2GhKiNHZ0MXzfYPGchPGfpvRPibroTdEbU/Dt83Cd/2cgbGLGL81aUb/KxNgCU0XWFQ5tpj3o+F/hlNDp8Dw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-04T19:19:05.974297Z","bundle_sha256":"a38d0a07947f264f57d5861fd21693ba6b53138a9706dfc591dd55d713ece5c0"}}