{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:HTLJL5ZVMDONXXIC72BN7SIDUS","short_pith_number":"pith:HTLJL5ZV","canonical_record":{"source":{"id":"1507.02724","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-07-09T22:08:41Z","cross_cats_sorted":[],"title_canon_sha256":"d4127c516cc9ebb81fcfae37fe07a8a19be694aa5e9380ba923305f7b8db6291","abstract_canon_sha256":"c5c071982752df499a5e5c660416bfa3da53a03905763062fedcefe5ba344f14"},"schema_version":"1.0"},"canonical_sha256":"3cd695f73560dcdbdd02fe82dfc903a4b5636365ff68ca1f6ce4c84022e19c6d","source":{"kind":"arxiv","id":"1507.02724","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1507.02724","created_at":"2026-05-18T01:11:46Z"},{"alias_kind":"arxiv_version","alias_value":"1507.02724v2","created_at":"2026-05-18T01:11:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.02724","created_at":"2026-05-18T01:11:46Z"},{"alias_kind":"pith_short_12","alias_value":"HTLJL5ZVMDON","created_at":"2026-05-18T12:29:25Z"},{"alias_kind":"pith_short_16","alias_value":"HTLJL5ZVMDONXXIC","created_at":"2026-05-18T12:29:25Z"},{"alias_kind":"pith_short_8","alias_value":"HTLJL5ZV","created_at":"2026-05-18T12:29:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:HTLJL5ZVMDONXXIC72BN7SIDUS","target":"record","payload":{"canonical_record":{"source":{"id":"1507.02724","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-07-09T22:08:41Z","cross_cats_sorted":[],"title_canon_sha256":"d4127c516cc9ebb81fcfae37fe07a8a19be694aa5e9380ba923305f7b8db6291","abstract_canon_sha256":"c5c071982752df499a5e5c660416bfa3da53a03905763062fedcefe5ba344f14"},"schema_version":"1.0"},"canonical_sha256":"3cd695f73560dcdbdd02fe82dfc903a4b5636365ff68ca1f6ce4c84022e19c6d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:11:46.824420Z","signature_b64":"2Vd5pU5hunVAgzr7eu8QHy0OI3HtjY3iQG9LItHo8o1Nu9rq/ImwAy0nbN2ezDRMLZv1hn1fYKPOGbKCUFwXBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3cd695f73560dcdbdd02fe82dfc903a4b5636365ff68ca1f6ce4c84022e19c6d","last_reissued_at":"2026-05-18T01:11:46.823984Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:11:46.823984Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1507.02724","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:11:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/rFezK+vS4PXJesGI2yRfQznojOcxydCcBw5moNSbyonz8+DRxWa/avUxz0Idh/8V/nLFROLEhykDJhvAyjgDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T16:33:09.170347Z"},"content_sha256":"9d736ae29f20a27ecf602fcf9dda3a5b43bb5b1773d1ae9c2b801832fa29e032","schema_version":"1.0","event_id":"sha256:9d736ae29f20a27ecf602fcf9dda3a5b43bb5b1773d1ae9c2b801832fa29e032"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:HTLJL5ZVMDONXXIC72BN7SIDUS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Study of decuplet baryon resonances from lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Andrew V. Pochinsky, Constantia Alexandrou, John W. Negele, Marcus Petschlies, Sergey N. Syritsyn","submitted_at":"2015-07-09T22:08:41Z","abstract_excerpt":"A lattice QCD study of the strong decay width and coupling constant of decuplet baryons to an octet baryon - pion state is presented. The transfer matrix method is used to obtain the overlap of lattice states with decuplet baryon quantum numbers on the one hand and octet baryon-pion quantum numbers on the other as an approximation to the matrix element of the corresponding transition. By making use of leading order effective field theory, the coupling constants, as well as the widths for the various decay channels are determined. The transitions studied are $ \\Delta \\to \\pi \\,N$, $\\Sigma^* \\to"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.02724","kind":"arxiv","version":2},"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":"2026-05-18T01:11:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9m1XV/S5nA5Bbz0Q8EkN4J3eDyG+bT9kKsUdYugb4Zn410tznKwdDmCpTjc0kNmqUBZw1QrU0x5w1FAXNzsnDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T16:33:09.170776Z"},"content_sha256":"3026430462a39fdf78ac8d52a3626a4052483fd1b84a0432553ce504aea96d69","schema_version":"1.0","event_id":"sha256:3026430462a39fdf78ac8d52a3626a4052483fd1b84a0432553ce504aea96d69"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HTLJL5ZVMDONXXIC72BN7SIDUS/bundle.json","state_url":"https://pith.science/pith/HTLJL5ZVMDONXXIC72BN7SIDUS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HTLJL5ZVMDONXXIC72BN7SIDUS/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":"2026-05-26T16:33:09Z","links":{"resolver":"https://pith.science/pith/HTLJL5ZVMDONXXIC72BN7SIDUS","bundle":"https://pith.science/pith/HTLJL5ZVMDONXXIC72BN7SIDUS/bundle.json","state":"https://pith.science/pith/HTLJL5ZVMDONXXIC72BN7SIDUS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HTLJL5ZVMDONXXIC72BN7SIDUS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:HTLJL5ZVMDONXXIC72BN7SIDUS","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":"c5c071982752df499a5e5c660416bfa3da53a03905763062fedcefe5ba344f14","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-07-09T22:08:41Z","title_canon_sha256":"d4127c516cc9ebb81fcfae37fe07a8a19be694aa5e9380ba923305f7b8db6291"},"schema_version":"1.0","source":{"id":"1507.02724","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1507.02724","created_at":"2026-05-18T01:11:46Z"},{"alias_kind":"arxiv_version","alias_value":"1507.02724v2","created_at":"2026-05-18T01:11:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.02724","created_at":"2026-05-18T01:11:46Z"},{"alias_kind":"pith_short_12","alias_value":"HTLJL5ZVMDON","created_at":"2026-05-18T12:29:25Z"},{"alias_kind":"pith_short_16","alias_value":"HTLJL5ZVMDONXXIC","created_at":"2026-05-18T12:29:25Z"},{"alias_kind":"pith_short_8","alias_value":"HTLJL5ZV","created_at":"2026-05-18T12:29:25Z"}],"graph_snapshots":[{"event_id":"sha256:3026430462a39fdf78ac8d52a3626a4052483fd1b84a0432553ce504aea96d69","target":"graph","created_at":"2026-05-18T01:11:46Z","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":"A lattice QCD study of the strong decay width and coupling constant of decuplet baryons to an octet baryon - pion state is presented. The transfer matrix method is used to obtain the overlap of lattice states with decuplet baryon quantum numbers on the one hand and octet baryon-pion quantum numbers on the other as an approximation to the matrix element of the corresponding transition. By making use of leading order effective field theory, the coupling constants, as well as the widths for the various decay channels are determined. The transitions studied are $ \\Delta \\to \\pi \\,N$, $\\Sigma^* \\to","authors_text":"Andrew V. Pochinsky, Constantia Alexandrou, John W. Negele, Marcus Petschlies, Sergey N. Syritsyn","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-07-09T22:08:41Z","title":"Study of decuplet baryon resonances from lattice QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.02724","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":"sha256:9d736ae29f20a27ecf602fcf9dda3a5b43bb5b1773d1ae9c2b801832fa29e032","target":"record","created_at":"2026-05-18T01:11:46Z","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":"c5c071982752df499a5e5c660416bfa3da53a03905763062fedcefe5ba344f14","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-07-09T22:08:41Z","title_canon_sha256":"d4127c516cc9ebb81fcfae37fe07a8a19be694aa5e9380ba923305f7b8db6291"},"schema_version":"1.0","source":{"id":"1507.02724","kind":"arxiv","version":2}},"canonical_sha256":"3cd695f73560dcdbdd02fe82dfc903a4b5636365ff68ca1f6ce4c84022e19c6d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3cd695f73560dcdbdd02fe82dfc903a4b5636365ff68ca1f6ce4c84022e19c6d","first_computed_at":"2026-05-18T01:11:46.823984Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:11:46.823984Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2Vd5pU5hunVAgzr7eu8QHy0OI3HtjY3iQG9LItHo8o1Nu9rq/ImwAy0nbN2ezDRMLZv1hn1fYKPOGbKCUFwXBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:11:46.824420Z","signed_message":"canonical_sha256_bytes"},"source_id":"1507.02724","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9d736ae29f20a27ecf602fcf9dda3a5b43bb5b1773d1ae9c2b801832fa29e032","sha256:3026430462a39fdf78ac8d52a3626a4052483fd1b84a0432553ce504aea96d69"],"state_sha256":"4120ee9972b34bda75ffcd042bff892e62190c865c13b12f19f41f7c52968eac"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"q8Mkg1AIhU3PsPxqjGxq5AIfou5H3QNgPv7dSaNM4vJgQ5uNZ1SXKAqhezf5cdluDqTGCy12dLxVmfsRDeiYBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T16:33:09.173896Z","bundle_sha256":"eaa98281c4b6ee8cbb6dbf05e9e08fa115df8e362f10a486aa6dd49bfbe5bb1a"}}