{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1994:HITOE5Z4A2H2NL2OB5PX57TMXL","short_pith_number":"pith:HITOE5Z4","canonical_record":{"source":{"id":"hep-ph/9409212","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1994-09-02T12:51:38Z","cross_cats_sorted":[],"title_canon_sha256":"b2ae5e125ca58398c347bf8fdb2d898139a7e215060e8003384d6aed2294eb36","abstract_canon_sha256":"002e87092be41e46d97c7da32f8c8fe235fb1aa2672ba09cb7121b51ebbd2395"},"schema_version":"1.0"},"canonical_sha256":"3a26e2773c068fa6af4e0f5f7efe6cbac611f33dca2cc80b0422167febaf85a7","source":{"kind":"arxiv","id":"hep-ph/9409212","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9409212","created_at":"2026-05-18T04:15:48Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9409212v2","created_at":"2026-05-18T04:15:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9409212","created_at":"2026-05-18T04:15:48Z"},{"alias_kind":"pith_short_12","alias_value":"HITOE5Z4A2H2","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"HITOE5Z4A2H2NL2O","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"HITOE5Z4","created_at":"2026-05-18T12:25:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1994:HITOE5Z4A2H2NL2OB5PX57TMXL","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9409212","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1994-09-02T12:51:38Z","cross_cats_sorted":[],"title_canon_sha256":"b2ae5e125ca58398c347bf8fdb2d898139a7e215060e8003384d6aed2294eb36","abstract_canon_sha256":"002e87092be41e46d97c7da32f8c8fe235fb1aa2672ba09cb7121b51ebbd2395"},"schema_version":"1.0"},"canonical_sha256":"3a26e2773c068fa6af4e0f5f7efe6cbac611f33dca2cc80b0422167febaf85a7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:15:48.671372Z","signature_b64":"gw3t7p0cZnRceHuXyYR5rFIM5PfbPxGm8b/EOzQVQ+O2DBUaTey1JD2PGhGJNXiLFGy97tyS3w3DyxbIW3IqDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3a26e2773c068fa6af4e0f5f7efe6cbac611f33dca2cc80b0422167febaf85a7","last_reissued_at":"2026-05-18T04:15:48.670902Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:15:48.670902Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9409212","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":"2026-05-18T04:15:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vcs85pER/Vwsvfci6tIJcyJu6/3nRbjB20rF2rMOq94KbgspZyWEkZHmSU4/juxzNKGoyXbJFV76OOg+Gf5QAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T21:48:23.402852Z"},"content_sha256":"a1652eb9957119fa9a4310eb5675bbd76d8babfdd1cddb0319b1de7fa14e3ff2","schema_version":"1.0","event_id":"sha256:a1652eb9957119fa9a4310eb5675bbd76d8babfdd1cddb0319b1de7fa14e3ff2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1994:HITOE5Z4A2H2NL2OB5PX57TMXL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"QCD Sum Rule Calculation of Twist-3 Contributions to Polarized Nucleon Structure Functions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Schaefer, E. Stein, L. Mankiewicz, P. Gornicki, W. Greiner","submitted_at":"1994-09-02T12:51:38Z","abstract_excerpt":"Using the framework of QCD sum rules we predict the twist-3 contribution to the second moment of the polarized nucleon structure function $g_2(x)$. As the relevant local operator depends explicitely on the gluon field, we employ a recently studied interpolating nucleon current which contains three quark field and one gluon field operator. Despite the fact that our calculation is based on the analysis of a completely different correlation function, our estimates are consitent with those of Balitsky, Braun and Kolesnichenko who used a three-quark current."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9409212","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":"2026-05-18T04:15:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1Tal/s7WYMAOBI85ZhXYn7qLrk3woRRSNd4aq7wWUQxQDluvJGgcS3NNmLftFXYx0QVedWPYjpMf58doLm8hBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T21:48:23.403530Z"},"content_sha256":"150fbb2af5c870900ffdcf40975bb7f920945dba09918680e383e7b2e8e299f9","schema_version":"1.0","event_id":"sha256:150fbb2af5c870900ffdcf40975bb7f920945dba09918680e383e7b2e8e299f9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HITOE5Z4A2H2NL2OB5PX57TMXL/bundle.json","state_url":"https://pith.science/pith/HITOE5Z4A2H2NL2OB5PX57TMXL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HITOE5Z4A2H2NL2OB5PX57TMXL/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":"2026-05-25T21:48:23Z","links":{"resolver":"https://pith.science/pith/HITOE5Z4A2H2NL2OB5PX57TMXL","bundle":"https://pith.science/pith/HITOE5Z4A2H2NL2OB5PX57TMXL/bundle.json","state":"https://pith.science/pith/HITOE5Z4A2H2NL2OB5PX57TMXL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HITOE5Z4A2H2NL2OB5PX57TMXL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1994:HITOE5Z4A2H2NL2OB5PX57TMXL","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":"002e87092be41e46d97c7da32f8c8fe235fb1aa2672ba09cb7121b51ebbd2395","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1994-09-02T12:51:38Z","title_canon_sha256":"b2ae5e125ca58398c347bf8fdb2d898139a7e215060e8003384d6aed2294eb36"},"schema_version":"1.0","source":{"id":"hep-ph/9409212","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9409212","created_at":"2026-05-18T04:15:48Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9409212v2","created_at":"2026-05-18T04:15:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9409212","created_at":"2026-05-18T04:15:48Z"},{"alias_kind":"pith_short_12","alias_value":"HITOE5Z4A2H2","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"HITOE5Z4A2H2NL2O","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"HITOE5Z4","created_at":"2026-05-18T12:25:47Z"}],"graph_snapshots":[{"event_id":"sha256:150fbb2af5c870900ffdcf40975bb7f920945dba09918680e383e7b2e8e299f9","target":"graph","created_at":"2026-05-18T04:15:48Z","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":"Using the framework of QCD sum rules we predict the twist-3 contribution to the second moment of the polarized nucleon structure function $g_2(x)$. As the relevant local operator depends explicitely on the gluon field, we employ a recently studied interpolating nucleon current which contains three quark field and one gluon field operator. Despite the fact that our calculation is based on the analysis of a completely different correlation function, our estimates are consitent with those of Balitsky, Braun and Kolesnichenko who used a three-quark current.","authors_text":"A. Schaefer, E. Stein, L. Mankiewicz, P. Gornicki, W. Greiner","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1994-09-02T12:51:38Z","title":"QCD Sum Rule Calculation of Twist-3 Contributions to Polarized Nucleon Structure Functions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9409212","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:a1652eb9957119fa9a4310eb5675bbd76d8babfdd1cddb0319b1de7fa14e3ff2","target":"record","created_at":"2026-05-18T04:15:48Z","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":"002e87092be41e46d97c7da32f8c8fe235fb1aa2672ba09cb7121b51ebbd2395","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1994-09-02T12:51:38Z","title_canon_sha256":"b2ae5e125ca58398c347bf8fdb2d898139a7e215060e8003384d6aed2294eb36"},"schema_version":"1.0","source":{"id":"hep-ph/9409212","kind":"arxiv","version":2}},"canonical_sha256":"3a26e2773c068fa6af4e0f5f7efe6cbac611f33dca2cc80b0422167febaf85a7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3a26e2773c068fa6af4e0f5f7efe6cbac611f33dca2cc80b0422167febaf85a7","first_computed_at":"2026-05-18T04:15:48.670902Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:15:48.670902Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"gw3t7p0cZnRceHuXyYR5rFIM5PfbPxGm8b/EOzQVQ+O2DBUaTey1JD2PGhGJNXiLFGy97tyS3w3DyxbIW3IqDg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:15:48.671372Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9409212","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a1652eb9957119fa9a4310eb5675bbd76d8babfdd1cddb0319b1de7fa14e3ff2","sha256:150fbb2af5c870900ffdcf40975bb7f920945dba09918680e383e7b2e8e299f9"],"state_sha256":"7687b64e6208667d1120624762d9182157bf8ab71279c6e95619da675dbdc60a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NmQ1WzfQLA5gb7OVyLCfm6nHasamxNWGSuN80lwCrRdnPdYocYQnFZiKDrmsZqo1XgRUnbPHvlmlmJWZpLBtDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T21:48:23.407039Z","bundle_sha256":"3eb6e2f9b51534b85122f4a4734e0fe064ab04476332c38ce8eaa03a3b791a13"}}