{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:3GPOYAEUWAXF4AFLJ5B3JMQUIT","short_pith_number":"pith:3GPOYAEU","canonical_record":{"source":{"id":"1606.09385","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2016-06-30T08:17:46Z","cross_cats_sorted":[],"title_canon_sha256":"0ebdbadf78f68816871d32b5e96888d7de086bfa70e8fa5c848f2e0a03bdedbd","abstract_canon_sha256":"60ee842153114eeee820c9da4f4e3d36870aba4260876445844e6bab51d38447"},"schema_version":"1.0"},"canonical_sha256":"d99eec0094b02e5e00ab4f43b4b21444f39e0c7afa6b6277b2146b97bed70131","source":{"kind":"arxiv","id":"1606.09385","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1606.09385","created_at":"2026-05-18T01:04:10Z"},{"alias_kind":"arxiv_version","alias_value":"1606.09385v3","created_at":"2026-05-18T01:04:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.09385","created_at":"2026-05-18T01:04:10Z"},{"alias_kind":"pith_short_12","alias_value":"3GPOYAEUWAXF","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_16","alias_value":"3GPOYAEUWAXF4AFL","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_8","alias_value":"3GPOYAEU","created_at":"2026-05-18T12:29:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:3GPOYAEUWAXF4AFLJ5B3JMQUIT","target":"record","payload":{"canonical_record":{"source":{"id":"1606.09385","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2016-06-30T08:17:46Z","cross_cats_sorted":[],"title_canon_sha256":"0ebdbadf78f68816871d32b5e96888d7de086bfa70e8fa5c848f2e0a03bdedbd","abstract_canon_sha256":"60ee842153114eeee820c9da4f4e3d36870aba4260876445844e6bab51d38447"},"schema_version":"1.0"},"canonical_sha256":"d99eec0094b02e5e00ab4f43b4b21444f39e0c7afa6b6277b2146b97bed70131","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:04:10.675241Z","signature_b64":"WIs5WA+raZj7APeChluRo0OefO/wyxm5W5/X+T41b/lkSbZ5gdPyC08//Klm8LM9sBsl3CerdsyrDHxPh65jBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d99eec0094b02e5e00ab4f43b4b21444f39e0c7afa6b6277b2146b97bed70131","last_reissued_at":"2026-05-18T01:04:10.674710Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:04:10.674710Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1606.09385","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":"2026-05-18T01:04:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kEff7vP7i2lI05zYDBi3WAsp8YVTGIwZr84sWomi+44fpFIa2QeYC903gvHD5JVXLjFwkmjI+ruCEBKfRCHuAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T06:51:22.066263Z"},"content_sha256":"9dbdbb68c30eb47fbcf7de0a08d1bcbff31d8967ec412dbafa6cb843e4ee9a6b","schema_version":"1.0","event_id":"sha256:9dbdbb68c30eb47fbcf7de0a08d1bcbff31d8967ec412dbafa6cb843e4ee9a6b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:3GPOYAEUWAXF4AFLJ5B3JMQUIT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Nucleon-pion-state contribution in lattice calculations of the nucleon charges $g_A,g_T$ and $g_S$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Oliver Bar","submitted_at":"2016-06-30T08:17:46Z","abstract_excerpt":"We employ leading order covariant chiral perturbation theory to compute the nucleon-pion-state contribution to the 3-point correlation functions one typically measures in lattice QCD to extract the isovector nucleon charges $g_A,g_T$ and $g_S$. We estimate the impact of the nucleon-pion-state contribution on both the plateau and the summation method for lattice simulations with physical pion masses. The nucleon-pion-state contribution results in an overestimation of all charges with both methods. The overestimation is roughly equal for the axial and the tensor charge, and about fifty percent l"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.09385","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":"2026-05-18T01:04:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"paGyB+M0qFKyGm61CojPhhqMFshwtqQJkYYnY6ycyyjVL6uhgBsGW68fENk3ObeyXY2sXlGgDk1ByP4eDxeMBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T06:51:22.066946Z"},"content_sha256":"e3f1d5e5fea5df8c79579da27594c9542c8e0f7b8184452b4ff8518d54bcd342","schema_version":"1.0","event_id":"sha256:e3f1d5e5fea5df8c79579da27594c9542c8e0f7b8184452b4ff8518d54bcd342"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3GPOYAEUWAXF4AFLJ5B3JMQUIT/bundle.json","state_url":"https://pith.science/pith/3GPOYAEUWAXF4AFLJ5B3JMQUIT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3GPOYAEUWAXF4AFLJ5B3JMQUIT/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":"2026-05-31T06:51:22Z","links":{"resolver":"https://pith.science/pith/3GPOYAEUWAXF4AFLJ5B3JMQUIT","bundle":"https://pith.science/pith/3GPOYAEUWAXF4AFLJ5B3JMQUIT/bundle.json","state":"https://pith.science/pith/3GPOYAEUWAXF4AFLJ5B3JMQUIT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3GPOYAEUWAXF4AFLJ5B3JMQUIT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:3GPOYAEUWAXF4AFLJ5B3JMQUIT","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":"60ee842153114eeee820c9da4f4e3d36870aba4260876445844e6bab51d38447","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2016-06-30T08:17:46Z","title_canon_sha256":"0ebdbadf78f68816871d32b5e96888d7de086bfa70e8fa5c848f2e0a03bdedbd"},"schema_version":"1.0","source":{"id":"1606.09385","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1606.09385","created_at":"2026-05-18T01:04:10Z"},{"alias_kind":"arxiv_version","alias_value":"1606.09385v3","created_at":"2026-05-18T01:04:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.09385","created_at":"2026-05-18T01:04:10Z"},{"alias_kind":"pith_short_12","alias_value":"3GPOYAEUWAXF","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_16","alias_value":"3GPOYAEUWAXF4AFL","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_8","alias_value":"3GPOYAEU","created_at":"2026-05-18T12:29:55Z"}],"graph_snapshots":[{"event_id":"sha256:e3f1d5e5fea5df8c79579da27594c9542c8e0f7b8184452b4ff8518d54bcd342","target":"graph","created_at":"2026-05-18T01:04:10Z","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 employ leading order covariant chiral perturbation theory to compute the nucleon-pion-state contribution to the 3-point correlation functions one typically measures in lattice QCD to extract the isovector nucleon charges $g_A,g_T$ and $g_S$. We estimate the impact of the nucleon-pion-state contribution on both the plateau and the summation method for lattice simulations with physical pion masses. The nucleon-pion-state contribution results in an overestimation of all charges with both methods. The overestimation is roughly equal for the axial and the tensor charge, and about fifty percent l","authors_text":"Oliver Bar","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2016-06-30T08:17:46Z","title":"Nucleon-pion-state contribution in lattice calculations of the nucleon charges $g_A,g_T$ and $g_S$"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.09385","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":"sha256:9dbdbb68c30eb47fbcf7de0a08d1bcbff31d8967ec412dbafa6cb843e4ee9a6b","target":"record","created_at":"2026-05-18T01:04:10Z","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":"60ee842153114eeee820c9da4f4e3d36870aba4260876445844e6bab51d38447","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2016-06-30T08:17:46Z","title_canon_sha256":"0ebdbadf78f68816871d32b5e96888d7de086bfa70e8fa5c848f2e0a03bdedbd"},"schema_version":"1.0","source":{"id":"1606.09385","kind":"arxiv","version":3}},"canonical_sha256":"d99eec0094b02e5e00ab4f43b4b21444f39e0c7afa6b6277b2146b97bed70131","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d99eec0094b02e5e00ab4f43b4b21444f39e0c7afa6b6277b2146b97bed70131","first_computed_at":"2026-05-18T01:04:10.674710Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:04:10.674710Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"WIs5WA+raZj7APeChluRo0OefO/wyxm5W5/X+T41b/lkSbZ5gdPyC08//Klm8LM9sBsl3CerdsyrDHxPh65jBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:04:10.675241Z","signed_message":"canonical_sha256_bytes"},"source_id":"1606.09385","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9dbdbb68c30eb47fbcf7de0a08d1bcbff31d8967ec412dbafa6cb843e4ee9a6b","sha256:e3f1d5e5fea5df8c79579da27594c9542c8e0f7b8184452b4ff8518d54bcd342"],"state_sha256":"d6f05dd305eee83e58d12e7a65655f13d01651a4bc2a230a8b0a2604b87f70b4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qVUo/rbQ+FYF6nERhMR2NvJXIEQEmAXSja6DxRHHidgey1oEn378Scsv3k0gxDW6mXsufEEhmeVbEs1WbfEABw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T06:51:22.070623Z","bundle_sha256":"ee255db686f15a6bdd80a42358bdcf4be822e5d714c51b022ac196f7651f7010"}}