{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1994:GVTNTLIF3KW6QBDUVTQM2XLVSU","short_pith_number":"pith:GVTNTLIF","canonical_record":{"source":{"id":"hep-lat/9406007","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1994-06-10T20:43:49Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"1798ca1c2ff41b7ca17c498d135b17fd86fa11ad696a20c751b780ca9247b077","abstract_canon_sha256":"764f6c301c315018abbf0709449c82d69f01475f5b63f59f51d9c4fd13695455"},"schema_version":"1.0"},"canonical_sha256":"3566d9ad05daade80474ace0cd5d759504cc9156f193ffd381e92469117bd20d","source":{"kind":"arxiv","id":"hep-lat/9406007","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/9406007","created_at":"2026-07-04T15:50:44Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9406007v1","created_at":"2026-07-04T15:50:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9406007","created_at":"2026-07-04T15:50:44Z"},{"alias_kind":"pith_short_12","alias_value":"GVTNTLIF3KW6","created_at":"2026-07-04T15:50:44Z"},{"alias_kind":"pith_short_16","alias_value":"GVTNTLIF3KW6QBDU","created_at":"2026-07-04T15:50:44Z"},{"alias_kind":"pith_short_8","alias_value":"GVTNTLIF","created_at":"2026-07-04T15:50:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1994:GVTNTLIF3KW6QBDUVTQM2XLVSU","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/9406007","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1994-06-10T20:43:49Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"1798ca1c2ff41b7ca17c498d135b17fd86fa11ad696a20c751b780ca9247b077","abstract_canon_sha256":"764f6c301c315018abbf0709449c82d69f01475f5b63f59f51d9c4fd13695455"},"schema_version":"1.0"},"canonical_sha256":"3566d9ad05daade80474ace0cd5d759504cc9156f193ffd381e92469117bd20d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:50:44.597821Z","signature_b64":"4DOC461qqwzQqsnrC4/jr1OIDa7R5zAcyWlIvd8U67jVEx9fJTokp2Qad/OCCieMdNdwwdHDn4hsZYiEdoL6DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3566d9ad05daade80474ace0cd5d759504cc9156f193ffd381e92469117bd20d","last_reissued_at":"2026-07-04T15:50:44.597414Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:50:44.597414Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/9406007","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":"2026-07-04T15:50:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mNV7l/5OiCelAWWFkgT2p5C+G4r0t3RwgaiSpqFe44y5azkF6dkYnL6puWFDTb9rzMp2smJ7Yd4rC/CMHlxxBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-10T05:16:41.108319Z"},"content_sha256":"6105a40b0984ad7e828068bff033ffd11e5af71fba81412e1538e36906fc2016","schema_version":"1.0","event_id":"sha256:6105a40b0984ad7e828068bff033ffd11e5af71fba81412e1538e36906fc2016"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1994:GVTNTLIF3KW6QBDUVTQM2XLVSU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"$\\pi NN$ and Pseudoscalar Form Factors from Lattice QCD","license":"","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"K.F. Liu, S.J. Dong, Terrence Draper, Walter Wilcox","submitted_at":"1994-06-10T20:43:49Z","abstract_excerpt":"The $\\pi NN$ form factor $g_{\\pi NN}(q^2)$ is obtained from a quenched lattice QCD calculation of the pseudoscalar form factor $g_P(q^2)$ of the proton with pion pole dominance. We find that $g_{\\pi NN}(q^2)$ fitted with the monopole form agrees well with the Goldberger-Treiman relation and is much preferred over the dipole form. The monopole mass is determined to be $0.75 \\pm 0.14 {\\rm GeV}$ which shows that $g_{\\pi NN}(q^2)$ is rather soft. The extrapolated $\\pi N$ coupling constant $g_{\\pi NN} = 12.7 \\pm 2.4$ is quite consistent with the phenomenological values. We also compare $g_{\\pi NN}("},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9406007","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-lat/9406007/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-04T15:50:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2EFfXM39HUybhbMKtR/tMFeyc1sFCIV9LTQUsdbT5Z23ZlkB+wR9QLWjihMp/Y+Otdg8vRkM3I99E2ATBxblAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-10T05:16:41.108930Z"},"content_sha256":"ced0ba90d341d83052fba66c6ee865faee62090298986afe4e5fa55cf1fcdcd4","schema_version":"1.0","event_id":"sha256:ced0ba90d341d83052fba66c6ee865faee62090298986afe4e5fa55cf1fcdcd4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GVTNTLIF3KW6QBDUVTQM2XLVSU/bundle.json","state_url":"https://pith.science/pith/GVTNTLIF3KW6QBDUVTQM2XLVSU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GVTNTLIF3KW6QBDUVTQM2XLVSU/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":"2026-08-10T05:16:41Z","links":{"resolver":"https://pith.science/pith/GVTNTLIF3KW6QBDUVTQM2XLVSU","bundle":"https://pith.science/pith/GVTNTLIF3KW6QBDUVTQM2XLVSU/bundle.json","state":"https://pith.science/pith/GVTNTLIF3KW6QBDUVTQM2XLVSU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GVTNTLIF3KW6QBDUVTQM2XLVSU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1994:GVTNTLIF3KW6QBDUVTQM2XLVSU","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":"764f6c301c315018abbf0709449c82d69f01475f5b63f59f51d9c4fd13695455","cross_cats_sorted":["hep-ph","nucl-th"],"license":"","primary_cat":"hep-lat","submitted_at":"1994-06-10T20:43:49Z","title_canon_sha256":"1798ca1c2ff41b7ca17c498d135b17fd86fa11ad696a20c751b780ca9247b077"},"schema_version":"1.0","source":{"id":"hep-lat/9406007","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/9406007","created_at":"2026-07-04T15:50:44Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9406007v1","created_at":"2026-07-04T15:50:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9406007","created_at":"2026-07-04T15:50:44Z"},{"alias_kind":"pith_short_12","alias_value":"GVTNTLIF3KW6","created_at":"2026-07-04T15:50:44Z"},{"alias_kind":"pith_short_16","alias_value":"GVTNTLIF3KW6QBDU","created_at":"2026-07-04T15:50:44Z"},{"alias_kind":"pith_short_8","alias_value":"GVTNTLIF","created_at":"2026-07-04T15:50:44Z"}],"graph_snapshots":[{"event_id":"sha256:ced0ba90d341d83052fba66c6ee865faee62090298986afe4e5fa55cf1fcdcd4","target":"graph","created_at":"2026-07-04T15:50:44Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-lat/9406007/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The $\\pi NN$ form factor $g_{\\pi NN}(q^2)$ is obtained from a quenched lattice QCD calculation of the pseudoscalar form factor $g_P(q^2)$ of the proton with pion pole dominance. We find that $g_{\\pi NN}(q^2)$ fitted with the monopole form agrees well with the Goldberger-Treiman relation and is much preferred over the dipole form. The monopole mass is determined to be $0.75 \\pm 0.14 {\\rm GeV}$ which shows that $g_{\\pi NN}(q^2)$ is rather soft. The extrapolated $\\pi N$ coupling constant $g_{\\pi NN} = 12.7 \\pm 2.4$ is quite consistent with the phenomenological values. We also compare $g_{\\pi NN}(","authors_text":"K.F. Liu, S.J. Dong, Terrence Draper, Walter Wilcox","cross_cats":["hep-ph","nucl-th"],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"1994-06-10T20:43:49Z","title":"$\\pi NN$ and Pseudoscalar Form Factors from Lattice QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9406007","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":"sha256:6105a40b0984ad7e828068bff033ffd11e5af71fba81412e1538e36906fc2016","target":"record","created_at":"2026-07-04T15:50:44Z","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":"764f6c301c315018abbf0709449c82d69f01475f5b63f59f51d9c4fd13695455","cross_cats_sorted":["hep-ph","nucl-th"],"license":"","primary_cat":"hep-lat","submitted_at":"1994-06-10T20:43:49Z","title_canon_sha256":"1798ca1c2ff41b7ca17c498d135b17fd86fa11ad696a20c751b780ca9247b077"},"schema_version":"1.0","source":{"id":"hep-lat/9406007","kind":"arxiv","version":1}},"canonical_sha256":"3566d9ad05daade80474ace0cd5d759504cc9156f193ffd381e92469117bd20d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3566d9ad05daade80474ace0cd5d759504cc9156f193ffd381e92469117bd20d","first_computed_at":"2026-07-04T15:50:44.597414Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:50:44.597414Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4DOC461qqwzQqsnrC4/jr1OIDa7R5zAcyWlIvd8U67jVEx9fJTokp2Qad/OCCieMdNdwwdHDn4hsZYiEdoL6DQ==","signature_status":"signed_v1","signed_at":"2026-07-04T15:50:44.597821Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/9406007","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6105a40b0984ad7e828068bff033ffd11e5af71fba81412e1538e36906fc2016","sha256:ced0ba90d341d83052fba66c6ee865faee62090298986afe4e5fa55cf1fcdcd4"],"state_sha256":"dfbe5ef7968c6c8a52fdac1a285e3e3663d16a98bd4e7090303197f705f624c0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NTUOG860XsNqixnuk7fki7LCZe5EK5ayZXfvlDAp4mmPpN0H/mhsHzD6Qm6Safmfzg9wYUBADW7t7CKJYv4TDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-10T05:16:41.113305Z","bundle_sha256":"100aeca2a813e23785e5a522d1a287ecd8bd812a8abed6530ab963c9e4478091"}}