{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:LXDWMASGYBIZAJ2JEWCF7UTMRO","short_pith_number":"pith:LXDWMASG","canonical_record":{"source":{"id":"1512.00833","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-12-02T20:33:14Z","cross_cats_sorted":["hep-ex","nucl-th"],"title_canon_sha256":"5d03ae17999c2fa5c19d3a252dd9133618d01d78fd70220605afa02d9a6e5060","abstract_canon_sha256":"99160056cb4a03af93c525ae602813b9b95e1ddf6d46f51c0a33b15d643afe73"},"schema_version":"1.0"},"canonical_sha256":"5dc7660246c05190274925845fd26c8baa2f362dd6701b3eff631a690c4668f1","source":{"kind":"arxiv","id":"1512.00833","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1512.00833","created_at":"2026-05-18T01:19:43Z"},{"alias_kind":"arxiv_version","alias_value":"1512.00833v3","created_at":"2026-05-18T01:19:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.00833","created_at":"2026-05-18T01:19:43Z"},{"alias_kind":"pith_short_12","alias_value":"LXDWMASGYBIZ","created_at":"2026-05-18T12:29:29Z"},{"alias_kind":"pith_short_16","alias_value":"LXDWMASGYBIZAJ2J","created_at":"2026-05-18T12:29:29Z"},{"alias_kind":"pith_short_8","alias_value":"LXDWMASG","created_at":"2026-05-18T12:29:29Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:LXDWMASGYBIZAJ2JEWCF7UTMRO","target":"record","payload":{"canonical_record":{"source":{"id":"1512.00833","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-12-02T20:33:14Z","cross_cats_sorted":["hep-ex","nucl-th"],"title_canon_sha256":"5d03ae17999c2fa5c19d3a252dd9133618d01d78fd70220605afa02d9a6e5060","abstract_canon_sha256":"99160056cb4a03af93c525ae602813b9b95e1ddf6d46f51c0a33b15d643afe73"},"schema_version":"1.0"},"canonical_sha256":"5dc7660246c05190274925845fd26c8baa2f362dd6701b3eff631a690c4668f1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:19:43.964737Z","signature_b64":"yNgMU1wa01TqR1MdG78myBog4EU7QL4eYhgS3PvmnhEDP/6aY4Xml4bhW6H0tdy7dp1WLFA0zBidaNFTYDpaBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5dc7660246c05190274925845fd26c8baa2f362dd6701b3eff631a690c4668f1","last_reissued_at":"2026-05-18T01:19:43.964276Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:19:43.964276Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1512.00833","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:19:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"s5JjPXgzM9RFc/80rB0Wx7mFjuWxqxpoIiN3qQui7gJJNq6VnVTTvp/cQhfzJ7LPH+XVzWlXmEr5aM6/Qlu5Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T13:25:19.223984Z"},"content_sha256":"4bd9b2c7a540be2ec8118aaef4e4f3c2d9224271fe0bf6f1db0bcb823e21a8a0","schema_version":"1.0","event_id":"sha256:4bd9b2c7a540be2ec8118aaef4e4f3c2d9224271fe0bf6f1db0bcb823e21a8a0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:LXDWMASGYBIZAJ2JEWCF7UTMRO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Hyperon elastic electromagnetic form factors in the space-like momentum region","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Christian S. Fischer, Helios Sanchis-Alepuz","submitted_at":"2015-12-02T20:33:14Z","abstract_excerpt":"We present a calculation of the electric and magnetic form factors of ground-state octet and decuplet baryons including strange quarks. We work with a combination of Dyson-Schwinger equations for the quark propagator and covariant Bethe-Salpeter equations describing baryons as bound states of three (non-perturbative) quarks. Our form factors for the octet baryons are in good agreement with corresponding lattice data at finite $Q^2$; deviations in some isospin channels for the magnetic moments can be explained by missing meson cloud effects. At larger $Q^2$ our quark core calculation has predic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.00833","kind":"arxiv","version":3},"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":"2026-05-18T01:19:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EnlTqnKe6eD6hLMoonCCUmOcZG/v5sIbHsp5MEsmshTN4aX/LGUNhD9u/qkJMw4b7TfCVVntb/6XzN9NbF47CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T13:25:19.224372Z"},"content_sha256":"0915ca24d24943e5a4d4432c4c5dfccd0c871fe43c17627126dc41d9fcb468dd","schema_version":"1.0","event_id":"sha256:0915ca24d24943e5a4d4432c4c5dfccd0c871fe43c17627126dc41d9fcb468dd"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LXDWMASGYBIZAJ2JEWCF7UTMRO/bundle.json","state_url":"https://pith.science/pith/LXDWMASGYBIZAJ2JEWCF7UTMRO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LXDWMASGYBIZAJ2JEWCF7UTMRO/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":"2026-06-01T13:25:19Z","links":{"resolver":"https://pith.science/pith/LXDWMASGYBIZAJ2JEWCF7UTMRO","bundle":"https://pith.science/pith/LXDWMASGYBIZAJ2JEWCF7UTMRO/bundle.json","state":"https://pith.science/pith/LXDWMASGYBIZAJ2JEWCF7UTMRO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LXDWMASGYBIZAJ2JEWCF7UTMRO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:LXDWMASGYBIZAJ2JEWCF7UTMRO","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":"99160056cb4a03af93c525ae602813b9b95e1ddf6d46f51c0a33b15d643afe73","cross_cats_sorted":["hep-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-12-02T20:33:14Z","title_canon_sha256":"5d03ae17999c2fa5c19d3a252dd9133618d01d78fd70220605afa02d9a6e5060"},"schema_version":"1.0","source":{"id":"1512.00833","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1512.00833","created_at":"2026-05-18T01:19:43Z"},{"alias_kind":"arxiv_version","alias_value":"1512.00833v3","created_at":"2026-05-18T01:19:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.00833","created_at":"2026-05-18T01:19:43Z"},{"alias_kind":"pith_short_12","alias_value":"LXDWMASGYBIZ","created_at":"2026-05-18T12:29:29Z"},{"alias_kind":"pith_short_16","alias_value":"LXDWMASGYBIZAJ2J","created_at":"2026-05-18T12:29:29Z"},{"alias_kind":"pith_short_8","alias_value":"LXDWMASG","created_at":"2026-05-18T12:29:29Z"}],"graph_snapshots":[{"event_id":"sha256:0915ca24d24943e5a4d4432c4c5dfccd0c871fe43c17627126dc41d9fcb468dd","target":"graph","created_at":"2026-05-18T01:19:43Z","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"},"paper":{"abstract_excerpt":"We present a calculation of the electric and magnetic form factors of ground-state octet and decuplet baryons including strange quarks. We work with a combination of Dyson-Schwinger equations for the quark propagator and covariant Bethe-Salpeter equations describing baryons as bound states of three (non-perturbative) quarks. Our form factors for the octet baryons are in good agreement with corresponding lattice data at finite $Q^2$; deviations in some isospin channels for the magnetic moments can be explained by missing meson cloud effects. At larger $Q^2$ our quark core calculation has predic","authors_text":"Christian S. Fischer, Helios Sanchis-Alepuz","cross_cats":["hep-ex","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-12-02T20:33:14Z","title":"Hyperon elastic electromagnetic form factors in the space-like momentum region"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.00833","kind":"arxiv","version":3},"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":"sha256:4bd9b2c7a540be2ec8118aaef4e4f3c2d9224271fe0bf6f1db0bcb823e21a8a0","target":"record","created_at":"2026-05-18T01:19:43Z","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":"99160056cb4a03af93c525ae602813b9b95e1ddf6d46f51c0a33b15d643afe73","cross_cats_sorted":["hep-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-12-02T20:33:14Z","title_canon_sha256":"5d03ae17999c2fa5c19d3a252dd9133618d01d78fd70220605afa02d9a6e5060"},"schema_version":"1.0","source":{"id":"1512.00833","kind":"arxiv","version":3}},"canonical_sha256":"5dc7660246c05190274925845fd26c8baa2f362dd6701b3eff631a690c4668f1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5dc7660246c05190274925845fd26c8baa2f362dd6701b3eff631a690c4668f1","first_computed_at":"2026-05-18T01:19:43.964276Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:19:43.964276Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"yNgMU1wa01TqR1MdG78myBog4EU7QL4eYhgS3PvmnhEDP/6aY4Xml4bhW6H0tdy7dp1WLFA0zBidaNFTYDpaBw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:19:43.964737Z","signed_message":"canonical_sha256_bytes"},"source_id":"1512.00833","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4bd9b2c7a540be2ec8118aaef4e4f3c2d9224271fe0bf6f1db0bcb823e21a8a0","sha256:0915ca24d24943e5a4d4432c4c5dfccd0c871fe43c17627126dc41d9fcb468dd"],"state_sha256":"40b3c2de8dd05842be1edf96931136e72286e0e0cc3191ce270650dcd90f504d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WutTacPDNBmqWUs8KsjCPyksiyfVvi1NWA9WRj1LtfwQ8KSF0sT5Z8Q5uEWRFJqdYp+YnWoOuG3GGFcr11TfCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T13:25:19.226709Z","bundle_sha256":"df9dc5ebd4afffa77368b96e5c3024821a4a8c9c7a9983dc6dbef4eb7d3e0a7d"}}