{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:ZROAQTMSDGX3L3Z2YWCW6VDZKK","short_pith_number":"pith:ZROAQTMS","canonical_record":{"source":{"id":"1412.8413","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-12-29T18:29:25Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"bc8b9ae46500aacd367a8c029164495c8433b57cec4458577c91c5d1ab57fc62","abstract_canon_sha256":"5e852c89856d1b9e9c5293429b8258c7d1390a658be5cb71d6e52fc62702189d"},"schema_version":"1.0"},"canonical_sha256":"cc5c084d9219afb5ef3ac5856f5479528a1f15420e1c74bf8280b22c99da229b","source":{"kind":"arxiv","id":"1412.8413","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.8413","created_at":"2026-05-18T01:41:15Z"},{"alias_kind":"arxiv_version","alias_value":"1412.8413v1","created_at":"2026-05-18T01:41:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.8413","created_at":"2026-05-18T01:41:15Z"},{"alias_kind":"pith_short_12","alias_value":"ZROAQTMSDGX3","created_at":"2026-05-18T12:28:59Z"},{"alias_kind":"pith_short_16","alias_value":"ZROAQTMSDGX3L3Z2","created_at":"2026-05-18T12:28:59Z"},{"alias_kind":"pith_short_8","alias_value":"ZROAQTMS","created_at":"2026-05-18T12:28:59Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:ZROAQTMSDGX3L3Z2YWCW6VDZKK","target":"record","payload":{"canonical_record":{"source":{"id":"1412.8413","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-12-29T18:29:25Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"bc8b9ae46500aacd367a8c029164495c8433b57cec4458577c91c5d1ab57fc62","abstract_canon_sha256":"5e852c89856d1b9e9c5293429b8258c7d1390a658be5cb71d6e52fc62702189d"},"schema_version":"1.0"},"canonical_sha256":"cc5c084d9219afb5ef3ac5856f5479528a1f15420e1c74bf8280b22c99da229b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:15.326918Z","signature_b64":"xuh8VNkRGjROw0/cLZsEjIp1TewXYASTsKvqTed1OAr8udO0EUhNrILSimL8Jmuj5dsNDqbewBDRjvmJJXXgDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cc5c084d9219afb5ef3ac5856f5479528a1f15420e1c74bf8280b22c99da229b","last_reissued_at":"2026-05-18T01:41:15.326292Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:15.326292Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1412.8413","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":"2026-05-18T01:41:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"F6dASFRat8+6NsgJJ89bT16T5YYFNwepyGkN/TsZh+YVsh0wZTVPK9fDbD9MfU91Ij3p829TiD41FUJdwRSsDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T00:56:28.306110Z"},"content_sha256":"ef053d15f7c383501e29f6f59c561858b6885d2cce7c1ee250fa3ec4d90b2fd4","schema_version":"1.0","event_id":"sha256:ef053d15f7c383501e29f6f59c561858b6885d2cce7c1ee250fa3ec4d90b2fd4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:ZROAQTMSDGX3L3Z2YWCW6VDZKK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Electromagnetic baryon form factors in the Poincare-covariant Faddeev approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Gernot Eichmann, Helios Sanchis-Alepuz, Reinhard Alkofer, Richard Williams","submitted_at":"2014-12-29T18:29:25Z","abstract_excerpt":"Baryons are treated as three-quark systems using QCD degrees of freedom in Poincare-covariant bound-state equations. The quark self-energy as well as the interaction between quarks are approximated by a vector-vector interaction via a single dressed-gluon exchange (rainbow-ladder truncation), thereby allowing a unified study of quark, meson and baryon properties. Here we will focus on the calculation of electromagnetic properties of spin-1/2 and spin-3/2 ground state baryons."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.8413","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":"2026-05-18T01:41:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Y01Vx3flNfQgl6Ncb7qe0Lav8ycKi6VENNhmBW/MRNGlF1Z0KXH2wyz7kdx49EFiyHEP5fb+St64fV5p27chDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T00:56:28.306593Z"},"content_sha256":"b8e7095dc7b3f13ecfc470e495497fe7c6e130b88bcfe25a5c95825ce724b267","schema_version":"1.0","event_id":"sha256:b8e7095dc7b3f13ecfc470e495497fe7c6e130b88bcfe25a5c95825ce724b267"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZROAQTMSDGX3L3Z2YWCW6VDZKK/bundle.json","state_url":"https://pith.science/pith/ZROAQTMSDGX3L3Z2YWCW6VDZKK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZROAQTMSDGX3L3Z2YWCW6VDZKK/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":"2026-06-01T00:56:28Z","links":{"resolver":"https://pith.science/pith/ZROAQTMSDGX3L3Z2YWCW6VDZKK","bundle":"https://pith.science/pith/ZROAQTMSDGX3L3Z2YWCW6VDZKK/bundle.json","state":"https://pith.science/pith/ZROAQTMSDGX3L3Z2YWCW6VDZKK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZROAQTMSDGX3L3Z2YWCW6VDZKK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:ZROAQTMSDGX3L3Z2YWCW6VDZKK","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":"5e852c89856d1b9e9c5293429b8258c7d1390a658be5cb71d6e52fc62702189d","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-12-29T18:29:25Z","title_canon_sha256":"bc8b9ae46500aacd367a8c029164495c8433b57cec4458577c91c5d1ab57fc62"},"schema_version":"1.0","source":{"id":"1412.8413","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.8413","created_at":"2026-05-18T01:41:15Z"},{"alias_kind":"arxiv_version","alias_value":"1412.8413v1","created_at":"2026-05-18T01:41:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.8413","created_at":"2026-05-18T01:41:15Z"},{"alias_kind":"pith_short_12","alias_value":"ZROAQTMSDGX3","created_at":"2026-05-18T12:28:59Z"},{"alias_kind":"pith_short_16","alias_value":"ZROAQTMSDGX3L3Z2","created_at":"2026-05-18T12:28:59Z"},{"alias_kind":"pith_short_8","alias_value":"ZROAQTMS","created_at":"2026-05-18T12:28:59Z"}],"graph_snapshots":[{"event_id":"sha256:b8e7095dc7b3f13ecfc470e495497fe7c6e130b88bcfe25a5c95825ce724b267","target":"graph","created_at":"2026-05-18T01:41:15Z","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":"Baryons are treated as three-quark systems using QCD degrees of freedom in Poincare-covariant bound-state equations. The quark self-energy as well as the interaction between quarks are approximated by a vector-vector interaction via a single dressed-gluon exchange (rainbow-ladder truncation), thereby allowing a unified study of quark, meson and baryon properties. Here we will focus on the calculation of electromagnetic properties of spin-1/2 and spin-3/2 ground state baryons.","authors_text":"Gernot Eichmann, Helios Sanchis-Alepuz, Reinhard Alkofer, Richard Williams","cross_cats":["nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-12-29T18:29:25Z","title":"Electromagnetic baryon form factors in the Poincare-covariant Faddeev approach"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.8413","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:ef053d15f7c383501e29f6f59c561858b6885d2cce7c1ee250fa3ec4d90b2fd4","target":"record","created_at":"2026-05-18T01:41:15Z","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":"5e852c89856d1b9e9c5293429b8258c7d1390a658be5cb71d6e52fc62702189d","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-12-29T18:29:25Z","title_canon_sha256":"bc8b9ae46500aacd367a8c029164495c8433b57cec4458577c91c5d1ab57fc62"},"schema_version":"1.0","source":{"id":"1412.8413","kind":"arxiv","version":1}},"canonical_sha256":"cc5c084d9219afb5ef3ac5856f5479528a1f15420e1c74bf8280b22c99da229b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cc5c084d9219afb5ef3ac5856f5479528a1f15420e1c74bf8280b22c99da229b","first_computed_at":"2026-05-18T01:41:15.326292Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:41:15.326292Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xuh8VNkRGjROw0/cLZsEjIp1TewXYASTsKvqTed1OAr8udO0EUhNrILSimL8Jmuj5dsNDqbewBDRjvmJJXXgDA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:41:15.326918Z","signed_message":"canonical_sha256_bytes"},"source_id":"1412.8413","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ef053d15f7c383501e29f6f59c561858b6885d2cce7c1ee250fa3ec4d90b2fd4","sha256:b8e7095dc7b3f13ecfc470e495497fe7c6e130b88bcfe25a5c95825ce724b267"],"state_sha256":"ac99b94d32cc2c1be9625692ffe6df40afef430e8c5a48b3068c5f422201df6f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"f4Ty/iTHLGinL0baUlbiaFBaXt9DJf6LVnra5ELmzUkry7xs/31Cw7rk/Uw2S866GGHKnyrj9K6gYdQgKqs7DA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T00:56:28.309969Z","bundle_sha256":"7b613654387fb2319a021f164981b56815221229a24db44a5fb170858ed12753"}}