{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1997:PNQENYMT66NAU2DSEEKKKWOKVU","short_pith_number":"pith:PNQENYMT","canonical_record":{"source":{"id":"hep-ph/9701350","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1997-01-22T18:20:37Z","cross_cats_sorted":[],"title_canon_sha256":"19295540903d7d301933cb01efcdae98b451868db07b20f19f63665344442168","abstract_canon_sha256":"5c6cf142a547b22deb2fc5cbcdfa2c867f050d2c7ab9573c473dc5853c3ebe2b"},"schema_version":"1.0"},"canonical_sha256":"7b6046e193f79a0a68722114a559caad0d510aa1166faae52159ab3b4d57b830","source":{"kind":"arxiv","id":"hep-ph/9701350","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9701350","created_at":"2026-05-18T01:38:56Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9701350v2","created_at":"2026-05-18T01:38:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9701350","created_at":"2026-05-18T01:38:56Z"},{"alias_kind":"pith_short_12","alias_value":"PNQENYMT66NA","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_16","alias_value":"PNQENYMT66NAU2DS","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_8","alias_value":"PNQENYMT","created_at":"2026-05-18T12:25:48Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1997:PNQENYMT66NAU2DSEEKKKWOKVU","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9701350","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1997-01-22T18:20:37Z","cross_cats_sorted":[],"title_canon_sha256":"19295540903d7d301933cb01efcdae98b451868db07b20f19f63665344442168","abstract_canon_sha256":"5c6cf142a547b22deb2fc5cbcdfa2c867f050d2c7ab9573c473dc5853c3ebe2b"},"schema_version":"1.0"},"canonical_sha256":"7b6046e193f79a0a68722114a559caad0d510aa1166faae52159ab3b4d57b830","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:38:56.891462Z","signature_b64":"M8XoZh1Q4YGuE4Mil9VWntAF4xWOP/fk96gCHr7MMM5wXL7AZor/UZRVQV++xlrGoQfmhXvck0TR8MBiJ37mCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7b6046e193f79a0a68722114a559caad0d510aa1166faae52159ab3b4d57b830","last_reissued_at":"2026-05-18T01:38:56.890815Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:38:56.890815Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9701350","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":"2026-05-18T01:38:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QKd2Cw8OijH/TXTscNNbtF9fgHbmYkTIqIzC37akuoMShtrKyD16dxBXs/MqAq9FDhb9+qFNhp6nb5hUSuOdBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-28T11:12:45.929797Z"},"content_sha256":"741912359546f62b1321401b16c622ab0335a7151cb0245514275e9e86b32ef5","schema_version":"1.0","event_id":"sha256:741912359546f62b1321401b16c622ab0335a7151cb0245514275e9e86b32ef5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1997:PNQENYMT66NAU2DSEEKKKWOKVU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Supersymmetric Electroweak Parity Nonconservation in Top Quark Pair Production at the Fermilab Tevatron","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Chong Sheng Li, C.-P. Yuan, Jin Min Yang, Robert J. Oakes","submitted_at":"1997-01-22T18:20:37Z","abstract_excerpt":"We evaluate the supersymmetric (SUSY) electroweak corrections to the effect of parity nonconservation in $q {\\bar q} \\to t {\\bar t}$ production at the Fermilab Tevatron predicted by the Minimal Supersymmetric Model (MSSM). We find that the parity nonconserving asymmetry from the SUSY electroweak and SUSY Yukawa loop corrections predicted by the minimal supergravity (mSUGRA) model and the MSSM models with scenarios motivated by current data is about one percent. It will be challenging to observe such a small asymmetry at the Tevatron with 10 fb^{-1} of luminosity. It could however be observable"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9701350","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":"2026-05-18T01:38:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ESsoqjevPavehQhNCdL5nX4JcwyTtv/xWiB9zw6UcEeaSQEniyKbH26CEQ9jz4QxvJ5TVbSYAkaRnaXwoxHPAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-28T11:12:45.930133Z"},"content_sha256":"d89f9e62baba8d9c06535fd4ae8a252646f04196784ca76e6be0f941dd19099f","schema_version":"1.0","event_id":"sha256:d89f9e62baba8d9c06535fd4ae8a252646f04196784ca76e6be0f941dd19099f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PNQENYMT66NAU2DSEEKKKWOKVU/bundle.json","state_url":"https://pith.science/pith/PNQENYMT66NAU2DSEEKKKWOKVU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PNQENYMT66NAU2DSEEKKKWOKVU/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":"2026-06-28T11:12:45Z","links":{"resolver":"https://pith.science/pith/PNQENYMT66NAU2DSEEKKKWOKVU","bundle":"https://pith.science/pith/PNQENYMT66NAU2DSEEKKKWOKVU/bundle.json","state":"https://pith.science/pith/PNQENYMT66NAU2DSEEKKKWOKVU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PNQENYMT66NAU2DSEEKKKWOKVU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1997:PNQENYMT66NAU2DSEEKKKWOKVU","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":"5c6cf142a547b22deb2fc5cbcdfa2c867f050d2c7ab9573c473dc5853c3ebe2b","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1997-01-22T18:20:37Z","title_canon_sha256":"19295540903d7d301933cb01efcdae98b451868db07b20f19f63665344442168"},"schema_version":"1.0","source":{"id":"hep-ph/9701350","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9701350","created_at":"2026-05-18T01:38:56Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9701350v2","created_at":"2026-05-18T01:38:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9701350","created_at":"2026-05-18T01:38:56Z"},{"alias_kind":"pith_short_12","alias_value":"PNQENYMT66NA","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_16","alias_value":"PNQENYMT66NAU2DS","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_8","alias_value":"PNQENYMT","created_at":"2026-05-18T12:25:48Z"}],"graph_snapshots":[{"event_id":"sha256:d89f9e62baba8d9c06535fd4ae8a252646f04196784ca76e6be0f941dd19099f","target":"graph","created_at":"2026-05-18T01:38:56Z","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 evaluate the supersymmetric (SUSY) electroweak corrections to the effect of parity nonconservation in $q {\\bar q} \\to t {\\bar t}$ production at the Fermilab Tevatron predicted by the Minimal Supersymmetric Model (MSSM). We find that the parity nonconserving asymmetry from the SUSY electroweak and SUSY Yukawa loop corrections predicted by the minimal supergravity (mSUGRA) model and the MSSM models with scenarios motivated by current data is about one percent. It will be challenging to observe such a small asymmetry at the Tevatron with 10 fb^{-1} of luminosity. It could however be observable","authors_text":"Chong Sheng Li, C.-P. Yuan, Jin Min Yang, Robert J. Oakes","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1997-01-22T18:20:37Z","title":"Supersymmetric Electroweak Parity Nonconservation in Top Quark Pair Production at the Fermilab Tevatron"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9701350","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":"sha256:741912359546f62b1321401b16c622ab0335a7151cb0245514275e9e86b32ef5","target":"record","created_at":"2026-05-18T01:38:56Z","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":"5c6cf142a547b22deb2fc5cbcdfa2c867f050d2c7ab9573c473dc5853c3ebe2b","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1997-01-22T18:20:37Z","title_canon_sha256":"19295540903d7d301933cb01efcdae98b451868db07b20f19f63665344442168"},"schema_version":"1.0","source":{"id":"hep-ph/9701350","kind":"arxiv","version":2}},"canonical_sha256":"7b6046e193f79a0a68722114a559caad0d510aa1166faae52159ab3b4d57b830","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7b6046e193f79a0a68722114a559caad0d510aa1166faae52159ab3b4d57b830","first_computed_at":"2026-05-18T01:38:56.890815Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:38:56.890815Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"M8XoZh1Q4YGuE4Mil9VWntAF4xWOP/fk96gCHr7MMM5wXL7AZor/UZRVQV++xlrGoQfmhXvck0TR8MBiJ37mCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:38:56.891462Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9701350","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:741912359546f62b1321401b16c622ab0335a7151cb0245514275e9e86b32ef5","sha256:d89f9e62baba8d9c06535fd4ae8a252646f04196784ca76e6be0f941dd19099f"],"state_sha256":"aac01220b7a8eec88f1edcfd931d41e47caecc5624c475d8cf3faf58ab8e46a0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9SQQWJFOt0OyILTcuyF58ndT6zCU8wZQ98SVBUNtoPYuqI5p3TPa9kLm8de3myBxczVVqNko61aOPeRXShdBBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-28T11:12:45.932009Z","bundle_sha256":"863549c3833c016f3bd7f314ac7d7ea3a69b6e42029f76b4fe5a65536be5ce5e"}}