{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:Y5JILKYAZNM3CH6SYDPGYYUZSF","short_pith_number":"pith:Y5JILKYA","schema_version":"1.0","canonical_sha256":"c75285ab00cb59b11fd2c0de6c62999155ec76e84df69671ab20f11dbbd91696","source":{"kind":"arxiv","id":"1706.02000","version":2},"attestation_state":"computed","paper":{"title":"Accessing the nucleon transverse structure in inclusive deep inelastic scattering","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Alberto Accardi, Alessandro Bacchetta","submitted_at":"2017-06-06T22:53:55Z","abstract_excerpt":"We revisit the standard analysis of inclusive Deep Inelastic Scattering off nucleons taking into account the fact that on-shell quarks cannot be present in the final state, but they rather decay into hadrons - a process that can be described in terms of suitable \"jet\" correlators. As a consequence, a spin-flip term associated with the invariant mass of the produced hadrons is generated non perturbatively and couples to the target's transversity distribution function. In inclusive cross sections, this provides an hitherto neglected and large contribution to the twist-3 part of the g2 structure "},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1706.02000","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-06-06T22:53:55Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"2ea715395c1fe5352669053edb340ec6d30acdfbc634ca98f54198e789a486ca","abstract_canon_sha256":"459d83afd5e460676d7a88b35de6886acdc216a7ce951045953b1b0b91a1b082"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:33:17.641955Z","signature_b64":"XkONfyTdq3GqNBRiZ9khxXb5tFG4WFKjrgtKwpgxA/UwIm+H/qhCnEZ37p+9janQcCp6wX9yqoe+6Ahw/HmKAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c75285ab00cb59b11fd2c0de6c62999155ec76e84df69671ab20f11dbbd91696","last_reissued_at":"2026-05-18T00:33:17.641234Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:33:17.641234Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Accessing the nucleon transverse structure in inclusive deep inelastic scattering","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Alberto Accardi, Alessandro Bacchetta","submitted_at":"2017-06-06T22:53:55Z","abstract_excerpt":"We revisit the standard analysis of inclusive Deep Inelastic Scattering off nucleons taking into account the fact that on-shell quarks cannot be present in the final state, but they rather decay into hadrons - a process that can be described in terms of suitable \"jet\" correlators. As a consequence, a spin-flip term associated with the invariant mass of the produced hadrons is generated non perturbatively and couples to the target's transversity distribution function. In inclusive cross sections, this provides an hitherto neglected and large contribution to the twist-3 part of the g2 structure "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.02000","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1706.02000","created_at":"2026-05-18T00:33:17.641366+00:00"},{"alias_kind":"arxiv_version","alias_value":"1706.02000v2","created_at":"2026-05-18T00:33:17.641366+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.02000","created_at":"2026-05-18T00:33:17.641366+00:00"},{"alias_kind":"pith_short_12","alias_value":"Y5JILKYAZNM3","created_at":"2026-05-18T12:31:56.362134+00:00"},{"alias_kind":"pith_short_16","alias_value":"Y5JILKYAZNM3CH6S","created_at":"2026-05-18T12:31:56.362134+00:00"},{"alias_kind":"pith_short_8","alias_value":"Y5JILKYA","created_at":"2026-05-18T12:31:56.362134+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.19997","citing_title":"Introduction to transverse momentum imaging","ref_index":44,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/Y5JILKYAZNM3CH6SYDPGYYUZSF","json":"https://pith.science/pith/Y5JILKYAZNM3CH6SYDPGYYUZSF.json","graph_json":"https://pith.science/api/pith-number/Y5JILKYAZNM3CH6SYDPGYYUZSF/graph.json","events_json":"https://pith.science/api/pith-number/Y5JILKYAZNM3CH6SYDPGYYUZSF/events.json","paper":"https://pith.science/paper/Y5JILKYA"},"agent_actions":{"view_html":"https://pith.science/pith/Y5JILKYAZNM3CH6SYDPGYYUZSF","download_json":"https://pith.science/pith/Y5JILKYAZNM3CH6SYDPGYYUZSF.json","view_paper":"https://pith.science/paper/Y5JILKYA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1706.02000&json=true","fetch_graph":"https://pith.science/api/pith-number/Y5JILKYAZNM3CH6SYDPGYYUZSF/graph.json","fetch_events":"https://pith.science/api/pith-number/Y5JILKYAZNM3CH6SYDPGYYUZSF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Y5JILKYAZNM3CH6SYDPGYYUZSF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Y5JILKYAZNM3CH6SYDPGYYUZSF/action/storage_attestation","attest_author":"https://pith.science/pith/Y5JILKYAZNM3CH6SYDPGYYUZSF/action/author_attestation","sign_citation":"https://pith.science/pith/Y5JILKYAZNM3CH6SYDPGYYUZSF/action/citation_signature","submit_replication":"https://pith.science/pith/Y5JILKYAZNM3CH6SYDPGYYUZSF/action/replication_record"}},"created_at":"2026-05-18T00:33:17.641366+00:00","updated_at":"2026-05-18T00:33:17.641366+00:00"}