{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1997:JJLAD3UNWPYB3F5RJ3RH52NNJF","short_pith_number":"pith:JJLAD3UN","canonical_record":{"source":{"id":"nucl-th/9709053","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1997-09-25T03:51:38Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"4fff02138cdc092f94b7488ab1c3785041e31aa3da68a17c9129326006cbd880","abstract_canon_sha256":"fc2bb79f68f54b211ec1ed0380dfd1c8c689ed4e9e71a8fa03a7ebee05b966ec"},"schema_version":"1.0"},"canonical_sha256":"4a5601ee8db3f01d97b14ee27ee9ad496026443fa2bcb3bb5fcb5bd75f8ebd6b","source":{"kind":"arxiv","id":"nucl-th/9709053","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/9709053","created_at":"2026-05-18T04:25:39Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9709053v2","created_at":"2026-05-18T04:25:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9709053","created_at":"2026-05-18T04:25:39Z"},{"alias_kind":"pith_short_12","alias_value":"JJLAD3UNWPYB","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_16","alias_value":"JJLAD3UNWPYB3F5R","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_8","alias_value":"JJLAD3UN","created_at":"2026-05-18T12:25:48Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1997:JJLAD3UNWPYB3F5RJ3RH52NNJF","target":"record","payload":{"canonical_record":{"source":{"id":"nucl-th/9709053","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1997-09-25T03:51:38Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"4fff02138cdc092f94b7488ab1c3785041e31aa3da68a17c9129326006cbd880","abstract_canon_sha256":"fc2bb79f68f54b211ec1ed0380dfd1c8c689ed4e9e71a8fa03a7ebee05b966ec"},"schema_version":"1.0"},"canonical_sha256":"4a5601ee8db3f01d97b14ee27ee9ad496026443fa2bcb3bb5fcb5bd75f8ebd6b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:25:39.437225Z","signature_b64":"Nrs5axqcVlZOtsX1AAIs1FxtFuIYwcCOt9FyCcRt4nqw+JOWXWBZu6GV9gz9dP85WZujLzZbw6sxUFhG3wpWBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4a5601ee8db3f01d97b14ee27ee9ad496026443fa2bcb3bb5fcb5bd75f8ebd6b","last_reissued_at":"2026-05-18T04:25:39.436792Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:25:39.436792Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"nucl-th/9709053","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":"2026-05-18T04:25:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"V154wM01BnlXeHiqHPtD/dWljmeI8NIzGN2oaZKUF9JEURtRHSaRXYDHtU9A0jpwYCms07X/0gYxitTyJ0SICw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T13:46:46.607476Z"},"content_sha256":"6e2d0c0bea42f11a1486ba3be63a3871194d75071001a124c2466acd0b46f1d2","schema_version":"1.0","event_id":"sha256:6e2d0c0bea42f11a1486ba3be63a3871194d75071001a124c2466acd0b46f1d2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1997:JJLAD3UNWPYB3F5RJ3RH52NNJF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Strange Mesonic Transition Form Factor in the Chiral Constituent Quark Model","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Hiroshi Ito, M. J. Ramsey-Musolf","submitted_at":"1997-09-25T03:51:38Z","abstract_excerpt":"The form factor $g_{\\rho \\pi}^{(S)}(Q^{2})$ of the strange vector current transition matrix element $<\\rho| \\bar{s}\\gamma_\\mus|\\pi>$ is calculated within the chiral quark model. A strange vector current of the constituent $U$- and D-quarks is induced by kaon radiative corrections and this mechanism yields the nonvanishing values of $g_{\\rho\\pi}^{(S)}(0)$. The numerical result at the photon point is consistent with the one given by the $\\phi $-meson dominance model, but the fall-off in the $Q^{2}$-dependence is faster than the monopole form factor. Mesonic radiative corrections are also examine"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9709053","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":"2026-05-18T04:25:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ugcJ5aWHMCkepfiE6jC4VoQRjITT6y003A7fwU5E+N4pZeSi6OXw47YOot/SBztofzuFQSHAF031LCmLcTzxBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T13:46:46.608089Z"},"content_sha256":"4319ba041f5984a019982122b080908003a9f12fd033bf37dff3850294c1ceed","schema_version":"1.0","event_id":"sha256:4319ba041f5984a019982122b080908003a9f12fd033bf37dff3850294c1ceed"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JJLAD3UNWPYB3F5RJ3RH52NNJF/bundle.json","state_url":"https://pith.science/pith/JJLAD3UNWPYB3F5RJ3RH52NNJF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JJLAD3UNWPYB3F5RJ3RH52NNJF/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":"2026-05-26T13:46:46Z","links":{"resolver":"https://pith.science/pith/JJLAD3UNWPYB3F5RJ3RH52NNJF","bundle":"https://pith.science/pith/JJLAD3UNWPYB3F5RJ3RH52NNJF/bundle.json","state":"https://pith.science/pith/JJLAD3UNWPYB3F5RJ3RH52NNJF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JJLAD3UNWPYB3F5RJ3RH52NNJF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1997:JJLAD3UNWPYB3F5RJ3RH52NNJF","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":"fc2bb79f68f54b211ec1ed0380dfd1c8c689ed4e9e71a8fa03a7ebee05b966ec","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"nucl-th","submitted_at":"1997-09-25T03:51:38Z","title_canon_sha256":"4fff02138cdc092f94b7488ab1c3785041e31aa3da68a17c9129326006cbd880"},"schema_version":"1.0","source":{"id":"nucl-th/9709053","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/9709053","created_at":"2026-05-18T04:25:39Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9709053v2","created_at":"2026-05-18T04:25:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9709053","created_at":"2026-05-18T04:25:39Z"},{"alias_kind":"pith_short_12","alias_value":"JJLAD3UNWPYB","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_16","alias_value":"JJLAD3UNWPYB3F5R","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_8","alias_value":"JJLAD3UN","created_at":"2026-05-18T12:25:48Z"}],"graph_snapshots":[{"event_id":"sha256:4319ba041f5984a019982122b080908003a9f12fd033bf37dff3850294c1ceed","target":"graph","created_at":"2026-05-18T04:25:39Z","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":"The form factor $g_{\\rho \\pi}^{(S)}(Q^{2})$ of the strange vector current transition matrix element $<\\rho| \\bar{s}\\gamma_\\mus|\\pi>$ is calculated within the chiral quark model. A strange vector current of the constituent $U$- and D-quarks is induced by kaon radiative corrections and this mechanism yields the nonvanishing values of $g_{\\rho\\pi}^{(S)}(0)$. The numerical result at the photon point is consistent with the one given by the $\\phi $-meson dominance model, but the fall-off in the $Q^{2}$-dependence is faster than the monopole form factor. Mesonic radiative corrections are also examine","authors_text":"Hiroshi Ito, M. J. Ramsey-Musolf","cross_cats":["hep-ph"],"headline":"","license":"","primary_cat":"nucl-th","submitted_at":"1997-09-25T03:51:38Z","title":"Strange Mesonic Transition Form Factor in the Chiral Constituent Quark Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9709053","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":"sha256:6e2d0c0bea42f11a1486ba3be63a3871194d75071001a124c2466acd0b46f1d2","target":"record","created_at":"2026-05-18T04:25:39Z","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":"fc2bb79f68f54b211ec1ed0380dfd1c8c689ed4e9e71a8fa03a7ebee05b966ec","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"nucl-th","submitted_at":"1997-09-25T03:51:38Z","title_canon_sha256":"4fff02138cdc092f94b7488ab1c3785041e31aa3da68a17c9129326006cbd880"},"schema_version":"1.0","source":{"id":"nucl-th/9709053","kind":"arxiv","version":2}},"canonical_sha256":"4a5601ee8db3f01d97b14ee27ee9ad496026443fa2bcb3bb5fcb5bd75f8ebd6b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4a5601ee8db3f01d97b14ee27ee9ad496026443fa2bcb3bb5fcb5bd75f8ebd6b","first_computed_at":"2026-05-18T04:25:39.436792Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:25:39.436792Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Nrs5axqcVlZOtsX1AAIs1FxtFuIYwcCOt9FyCcRt4nqw+JOWXWBZu6GV9gz9dP85WZujLzZbw6sxUFhG3wpWBA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:25:39.437225Z","signed_message":"canonical_sha256_bytes"},"source_id":"nucl-th/9709053","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6e2d0c0bea42f11a1486ba3be63a3871194d75071001a124c2466acd0b46f1d2","sha256:4319ba041f5984a019982122b080908003a9f12fd033bf37dff3850294c1ceed"],"state_sha256":"f7c4b17fb883fe42c07ba981c836f6fb457ebd37aaa0de5da0953d0376dbb2f7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TpF9iPS4ROZg6gA0GbUg0AMFpevxkREEfttW8/z8e5oZXlHqF4vgSnPesGMVTx77/u/qSgKlMAXoS9mU7Q/nAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T13:46:46.610885Z","bundle_sha256":"b8b17b2fb8714f8cfbfc535143daafcde1c8693ead334c5b50101a45bdee0f09"}}