{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:AVO4ADBBW4N24WGTV7TFPRLNEO","short_pith_number":"pith:AVO4ADBB","canonical_record":{"source":{"id":"1201.6114","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-01-30T06:54:46Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"ab101d62fe08566cf6fc256adc2d965ae17e693df972976e29263241ecacc748","abstract_canon_sha256":"23db78b2d71c6f91cf4380c33353356ba2a4ca5dec6114bb582c47deff690c75"},"schema_version":"1.0"},"canonical_sha256":"055dc00c21b71bae58d3afe657c56d238dd36e54edb220d95286ff759273c927","source":{"kind":"arxiv","id":"1201.6114","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.6114","created_at":"2026-05-18T03:22:52Z"},{"alias_kind":"arxiv_version","alias_value":"1201.6114v2","created_at":"2026-05-18T03:22:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.6114","created_at":"2026-05-18T03:22:52Z"},{"alias_kind":"pith_short_12","alias_value":"AVO4ADBBW4N2","created_at":"2026-05-18T12:26:58Z"},{"alias_kind":"pith_short_16","alias_value":"AVO4ADBBW4N24WGT","created_at":"2026-05-18T12:26:58Z"},{"alias_kind":"pith_short_8","alias_value":"AVO4ADBB","created_at":"2026-05-18T12:26:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:AVO4ADBBW4N24WGTV7TFPRLNEO","target":"record","payload":{"canonical_record":{"source":{"id":"1201.6114","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-01-30T06:54:46Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"ab101d62fe08566cf6fc256adc2d965ae17e693df972976e29263241ecacc748","abstract_canon_sha256":"23db78b2d71c6f91cf4380c33353356ba2a4ca5dec6114bb582c47deff690c75"},"schema_version":"1.0"},"canonical_sha256":"055dc00c21b71bae58d3afe657c56d238dd36e54edb220d95286ff759273c927","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:22:52.799666Z","signature_b64":"EvggrMxf3lbSZxEnVYuYxrBnbCNZh5etcwiLvLdOp16X/smOzM7JKjOXCoMFfR1CO5rRB1dNoYirmzgMLZN2AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"055dc00c21b71bae58d3afe657c56d238dd36e54edb220d95286ff759273c927","last_reissued_at":"2026-05-18T03:22:52.799179Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:22:52.799179Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1201.6114","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":"2026-05-18T03:22:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qUHg/oA3hk0in2Vz/YuFMzHgvMeCmPi19EbYZPUB2pOEUqEAT049ubdGC7Wa83KpKoT7mqFx+ocThKlC0CckCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T11:06:24.091696Z"},"content_sha256":"92293f12d871bee2f06a1d7d6dad93947070091ad253fe603b5848434500e63f","schema_version":"1.0","event_id":"sha256:92293f12d871bee2f06a1d7d6dad93947070091ad253fe603b5848434500e63f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:AVO4ADBBW4N24WGTV7TFPRLNEO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Chiral extrapolations for nucleon magnetic moments","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-lat","authors_text":"D. B. Leinweber, J. M. M. Hall, R. D. Young","submitted_at":"2012-01-30T06:54:46Z","abstract_excerpt":"Lattice QCD simulations have made significant progress in the calculation of nucleon electromagnetic form factors in the chiral regime in recent years. With simulation results achieving pion masses of order ~180 MeV, there is an apparent challenge as to how the physical regime is approached. By using contemporary methods in chiral effective field theory, both the quark-mass and finite-volume dependence of the isovector nucleon magnetic moment are carefully examined. The extrapolation to the physical point yields a result that is compatible with experiment, albeit with a combined statistical an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.6114","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":"2026-05-18T03:22:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GVeApOz6vb4gE0bEI+O6cvLXd8WwLl0JJbsMs77HDrfauO8j0q3zOw20rUVwWw0h8oMkGnMkdl4TMNFQGAirCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T11:06:24.092050Z"},"content_sha256":"a7dc862922b1cb3a9ba5b40702dee454f1202e4c0f007b6716c38bf3ec98fc1a","schema_version":"1.0","event_id":"sha256:a7dc862922b1cb3a9ba5b40702dee454f1202e4c0f007b6716c38bf3ec98fc1a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AVO4ADBBW4N24WGTV7TFPRLNEO/bundle.json","state_url":"https://pith.science/pith/AVO4ADBBW4N24WGTV7TFPRLNEO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AVO4ADBBW4N24WGTV7TFPRLNEO/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":"2026-05-28T11:06:24Z","links":{"resolver":"https://pith.science/pith/AVO4ADBBW4N24WGTV7TFPRLNEO","bundle":"https://pith.science/pith/AVO4ADBBW4N24WGTV7TFPRLNEO/bundle.json","state":"https://pith.science/pith/AVO4ADBBW4N24WGTV7TFPRLNEO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AVO4ADBBW4N24WGTV7TFPRLNEO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:AVO4ADBBW4N24WGTV7TFPRLNEO","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":"23db78b2d71c6f91cf4380c33353356ba2a4ca5dec6114bb582c47deff690c75","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-01-30T06:54:46Z","title_canon_sha256":"ab101d62fe08566cf6fc256adc2d965ae17e693df972976e29263241ecacc748"},"schema_version":"1.0","source":{"id":"1201.6114","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.6114","created_at":"2026-05-18T03:22:52Z"},{"alias_kind":"arxiv_version","alias_value":"1201.6114v2","created_at":"2026-05-18T03:22:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.6114","created_at":"2026-05-18T03:22:52Z"},{"alias_kind":"pith_short_12","alias_value":"AVO4ADBBW4N2","created_at":"2026-05-18T12:26:58Z"},{"alias_kind":"pith_short_16","alias_value":"AVO4ADBBW4N24WGT","created_at":"2026-05-18T12:26:58Z"},{"alias_kind":"pith_short_8","alias_value":"AVO4ADBB","created_at":"2026-05-18T12:26:58Z"}],"graph_snapshots":[{"event_id":"sha256:a7dc862922b1cb3a9ba5b40702dee454f1202e4c0f007b6716c38bf3ec98fc1a","target":"graph","created_at":"2026-05-18T03:22:52Z","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":"Lattice QCD simulations have made significant progress in the calculation of nucleon electromagnetic form factors in the chiral regime in recent years. With simulation results achieving pion masses of order ~180 MeV, there is an apparent challenge as to how the physical regime is approached. By using contemporary methods in chiral effective field theory, both the quark-mass and finite-volume dependence of the isovector nucleon magnetic moment are carefully examined. The extrapolation to the physical point yields a result that is compatible with experiment, albeit with a combined statistical an","authors_text":"D. B. Leinweber, J. M. M. Hall, R. D. Young","cross_cats":["nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-01-30T06:54:46Z","title":"Chiral extrapolations for nucleon magnetic moments"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.6114","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":"sha256:92293f12d871bee2f06a1d7d6dad93947070091ad253fe603b5848434500e63f","target":"record","created_at":"2026-05-18T03:22:52Z","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":"23db78b2d71c6f91cf4380c33353356ba2a4ca5dec6114bb582c47deff690c75","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-01-30T06:54:46Z","title_canon_sha256":"ab101d62fe08566cf6fc256adc2d965ae17e693df972976e29263241ecacc748"},"schema_version":"1.0","source":{"id":"1201.6114","kind":"arxiv","version":2}},"canonical_sha256":"055dc00c21b71bae58d3afe657c56d238dd36e54edb220d95286ff759273c927","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"055dc00c21b71bae58d3afe657c56d238dd36e54edb220d95286ff759273c927","first_computed_at":"2026-05-18T03:22:52.799179Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:22:52.799179Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"EvggrMxf3lbSZxEnVYuYxrBnbCNZh5etcwiLvLdOp16X/smOzM7JKjOXCoMFfR1CO5rRB1dNoYirmzgMLZN2AA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:22:52.799666Z","signed_message":"canonical_sha256_bytes"},"source_id":"1201.6114","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:92293f12d871bee2f06a1d7d6dad93947070091ad253fe603b5848434500e63f","sha256:a7dc862922b1cb3a9ba5b40702dee454f1202e4c0f007b6716c38bf3ec98fc1a"],"state_sha256":"1f1c39dad1859c7b89a4beec9f1180af3e94fe47b9b5f144917b1792fd1623e4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OJo0JHXNpH9rgN4MZwdPeUKxpAVdJBmxAcPTyRENiW425uGCIV/uwIQfZFjDebG6Q8WkFGaQWQxsBuoRZSwhAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T11:06:24.094420Z","bundle_sha256":"b77ba8df3f164248330189946ea135c200a8dc3fec570b98a688f62e66556431"}}