{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:DGUSLDNTRZKOGCCDNRROBFT6OP","short_pith_number":"pith:DGUSLDNT","canonical_record":{"source":{"id":"1302.6889","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-02-27T15:58:23Z","cross_cats_sorted":["hep-ex","hep-lat","nucl-ex","nucl-th"],"title_canon_sha256":"ebb5368385155dc4dffc38cadd8d2b4ecefb0f56ac8e7c072520f2e0cd6e839f","abstract_canon_sha256":"93b7aa5f554d941ddb12393d5d5281ee55a97c3e86df2cc600ca0478ac7cccdf"},"schema_version":"1.0"},"canonical_sha256":"19a9258db38e54e308436c62e0967e73eb8c110b93584eb703a0eee0be833256","source":{"kind":"arxiv","id":"1302.6889","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1302.6889","created_at":"2026-05-18T03:21:45Z"},{"alias_kind":"arxiv_version","alias_value":"1302.6889v2","created_at":"2026-05-18T03:21:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.6889","created_at":"2026-05-18T03:21:45Z"},{"alias_kind":"pith_short_12","alias_value":"DGUSLDNTRZKO","created_at":"2026-05-18T12:27:43Z"},{"alias_kind":"pith_short_16","alias_value":"DGUSLDNTRZKOGCCD","created_at":"2026-05-18T12:27:43Z"},{"alias_kind":"pith_short_8","alias_value":"DGUSLDNT","created_at":"2026-05-18T12:27:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:DGUSLDNTRZKOGCCDNRROBFT6OP","target":"record","payload":{"canonical_record":{"source":{"id":"1302.6889","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-02-27T15:58:23Z","cross_cats_sorted":["hep-ex","hep-lat","nucl-ex","nucl-th"],"title_canon_sha256":"ebb5368385155dc4dffc38cadd8d2b4ecefb0f56ac8e7c072520f2e0cd6e839f","abstract_canon_sha256":"93b7aa5f554d941ddb12393d5d5281ee55a97c3e86df2cc600ca0478ac7cccdf"},"schema_version":"1.0"},"canonical_sha256":"19a9258db38e54e308436c62e0967e73eb8c110b93584eb703a0eee0be833256","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:21:45.220184Z","signature_b64":"Prw6IMWp6IlSA/OskGDcAjD3WeLpo6qzqzXRHMXTFnAX7WHiwD/3It25sN50jpKtHaFKr/oZuGJ3sYYHwBtPAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"19a9258db38e54e308436c62e0967e73eb8c110b93584eb703a0eee0be833256","last_reissued_at":"2026-05-18T03:21:45.219361Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:21:45.219361Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1302.6889","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":"2026-05-18T03:21:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QMSoD6qAWoLcwt2Y+ahNAFCiyZyJzQbbcWgTYgqmrpx4FiQn89jbgtcCW0MqmjimS+tILVaSLd1niyf3uslQDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-18T22:38:28.001779Z"},"content_sha256":"e13c19522149eb9d6c75fda5f7e799e1af45ae82f24012653248c205b1b71222","schema_version":"1.0","event_id":"sha256:e13c19522149eb9d6c75fda5f7e799e1af45ae82f24012653248c205b1b71222"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:DGUSLDNTRZKOGCCDNRROBFT6OP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Octet to decuplet electromagnetic transition in a relativistic quark model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"G. Ramalho, K. Tsushima","submitted_at":"2013-02-27T15:58:23Z","abstract_excerpt":"We study the octet to decuplet baryon electromagnetic transitions using the covariant spectator quark model, and predict the transition magnetic dipole form factors for those involving the strange baryons. Utilizing SU(3) symmetry, the valence quark contributions are supplemented by the pion cloud dressing based on the one estimated in the $\\gamma^\\ast N \\to \\Delta$ reaction. Although the valence quark contributions are dominant in general, the pion cloud effects turn out to be very important to describe the experimental data. We also show that, other mesons besides the pion in particular the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.6889","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":"2026-05-18T03:21:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tiyHUVW39fuWcvt5Mu1F7FsByxaTI2/dN8XHnp4N8Ink+vUUYg//dmDDq0yf8u3bgNegemw4B7Rm3URFOrcaDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-18T22:38:28.002145Z"},"content_sha256":"f176519c294419effa64cd319475352ee103547bfe41bba2b84eba4e914c2f2b","schema_version":"1.0","event_id":"sha256:f176519c294419effa64cd319475352ee103547bfe41bba2b84eba4e914c2f2b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DGUSLDNTRZKOGCCDNRROBFT6OP/bundle.json","state_url":"https://pith.science/pith/DGUSLDNTRZKOGCCDNRROBFT6OP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DGUSLDNTRZKOGCCDNRROBFT6OP/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":"2026-05-18T22:38:28Z","links":{"resolver":"https://pith.science/pith/DGUSLDNTRZKOGCCDNRROBFT6OP","bundle":"https://pith.science/pith/DGUSLDNTRZKOGCCDNRROBFT6OP/bundle.json","state":"https://pith.science/pith/DGUSLDNTRZKOGCCDNRROBFT6OP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DGUSLDNTRZKOGCCDNRROBFT6OP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:DGUSLDNTRZKOGCCDNRROBFT6OP","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":"93b7aa5f554d941ddb12393d5d5281ee55a97c3e86df2cc600ca0478ac7cccdf","cross_cats_sorted":["hep-ex","hep-lat","nucl-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-02-27T15:58:23Z","title_canon_sha256":"ebb5368385155dc4dffc38cadd8d2b4ecefb0f56ac8e7c072520f2e0cd6e839f"},"schema_version":"1.0","source":{"id":"1302.6889","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1302.6889","created_at":"2026-05-18T03:21:45Z"},{"alias_kind":"arxiv_version","alias_value":"1302.6889v2","created_at":"2026-05-18T03:21:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.6889","created_at":"2026-05-18T03:21:45Z"},{"alias_kind":"pith_short_12","alias_value":"DGUSLDNTRZKO","created_at":"2026-05-18T12:27:43Z"},{"alias_kind":"pith_short_16","alias_value":"DGUSLDNTRZKOGCCD","created_at":"2026-05-18T12:27:43Z"},{"alias_kind":"pith_short_8","alias_value":"DGUSLDNT","created_at":"2026-05-18T12:27:43Z"}],"graph_snapshots":[{"event_id":"sha256:f176519c294419effa64cd319475352ee103547bfe41bba2b84eba4e914c2f2b","target":"graph","created_at":"2026-05-18T03:21:45Z","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":"We study the octet to decuplet baryon electromagnetic transitions using the covariant spectator quark model, and predict the transition magnetic dipole form factors for those involving the strange baryons. Utilizing SU(3) symmetry, the valence quark contributions are supplemented by the pion cloud dressing based on the one estimated in the $\\gamma^\\ast N \\to \\Delta$ reaction. Although the valence quark contributions are dominant in general, the pion cloud effects turn out to be very important to describe the experimental data. We also show that, other mesons besides the pion in particular the ","authors_text":"G. Ramalho, K. Tsushima","cross_cats":["hep-ex","hep-lat","nucl-ex","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-02-27T15:58:23Z","title":"Octet to decuplet electromagnetic transition in a relativistic quark model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.6889","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:e13c19522149eb9d6c75fda5f7e799e1af45ae82f24012653248c205b1b71222","target":"record","created_at":"2026-05-18T03:21:45Z","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":"93b7aa5f554d941ddb12393d5d5281ee55a97c3e86df2cc600ca0478ac7cccdf","cross_cats_sorted":["hep-ex","hep-lat","nucl-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-02-27T15:58:23Z","title_canon_sha256":"ebb5368385155dc4dffc38cadd8d2b4ecefb0f56ac8e7c072520f2e0cd6e839f"},"schema_version":"1.0","source":{"id":"1302.6889","kind":"arxiv","version":2}},"canonical_sha256":"19a9258db38e54e308436c62e0967e73eb8c110b93584eb703a0eee0be833256","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"19a9258db38e54e308436c62e0967e73eb8c110b93584eb703a0eee0be833256","first_computed_at":"2026-05-18T03:21:45.219361Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:21:45.219361Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Prw6IMWp6IlSA/OskGDcAjD3WeLpo6qzqzXRHMXTFnAX7WHiwD/3It25sN50jpKtHaFKr/oZuGJ3sYYHwBtPAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:21:45.220184Z","signed_message":"canonical_sha256_bytes"},"source_id":"1302.6889","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e13c19522149eb9d6c75fda5f7e799e1af45ae82f24012653248c205b1b71222","sha256:f176519c294419effa64cd319475352ee103547bfe41bba2b84eba4e914c2f2b"],"state_sha256":"2e9c1ddcba8ad68b05dffdaf5994a3d0aa00898f40cfe9e1e0fd31587c248cab"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yNjXymgZk5ngIdsp+BzXKPXhjUiH+Qg2b55YvXQOlOigZuhEHekPKSSOdkvWJqiYGQSphYgdjy1mSVSpHtXrCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-18T22:38:28.003540Z","bundle_sha256":"88f8f01ba680898caf5374136d32fdec8e174e51469e16d47cb8b3ed5bcd95c0"}}