{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:2JTNCMOIAC2UWBHO5RGGLASWEV","short_pith_number":"pith:2JTNCMOI","schema_version":"1.0","canonical_sha256":"d266d131c800b54b04eeec4c658256255764b22dadd59e4930a18e712c42c83e","source":{"kind":"arxiv","id":"2401.10127","version":2},"attestation_state":"computed","paper":{"title":"Heavy Quarks in Polarised Deep-Inelastic Scattering at the Electron-Ion Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Adrianne Schaus, Emanuele R. Nocera, Felix Hekhorn, Giacomo Magni, Juan Rojo, Roy Stegeman, Tanjona R. Rabemananjara","submitted_at":"2024-01-18T16:57:58Z","abstract_excerpt":"We extend the FONLL general-mass variable-flavour-number scheme to the case of longitudinally polarised DIS structure functions, accounting for perturbative corrections up to $\\mathcal{O}(\\alpha_s^2)$. We quantify the impact of charm quark mass and higher-order perturbative corrections on projected measurements of inclusive and charm-tagged longitudinal asymmetries at the Electron-Ion Collider (EIC) and at the Electron-ion collider in China (EicC). We demonstrate how the inclusion of these corrections is essential to compute predictions with an accuracy that matches the projected precision of "},"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":"2401.10127","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-01-18T16:57:58Z","cross_cats_sorted":["hep-ex","nucl-ex","nucl-th"],"title_canon_sha256":"b34b8620bd2decee82488b21de7cf826d1bc084e178dbc21c9470b2c7d634e1c","abstract_canon_sha256":"4f34e823b1ba0eab4ebcabde6414a8fe2a1ee98711bd2771d8d7fa014cadcd08"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:49:36.061845Z","signature_b64":"a0DatKBJ1JDytp+dPXCKdnVq5LOTKDBG4SRbvoZKvnLMvWH4LTv5RATacG9ghPvkxjV9u5WgiHLTG81wErD+CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d266d131c800b54b04eeec4c658256255764b22dadd59e4930a18e712c42c83e","last_reissued_at":"2026-07-05T07:49:36.061320Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:49:36.061320Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Heavy Quarks in Polarised Deep-Inelastic Scattering at the Electron-Ion Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Adrianne Schaus, Emanuele R. Nocera, Felix Hekhorn, Giacomo Magni, Juan Rojo, Roy Stegeman, Tanjona R. Rabemananjara","submitted_at":"2024-01-18T16:57:58Z","abstract_excerpt":"We extend the FONLL general-mass variable-flavour-number scheme to the case of longitudinally polarised DIS structure functions, accounting for perturbative corrections up to $\\mathcal{O}(\\alpha_s^2)$. We quantify the impact of charm quark mass and higher-order perturbative corrections on projected measurements of inclusive and charm-tagged longitudinal asymmetries at the Electron-Ion Collider (EIC) and at the Electron-ion collider in China (EicC). We demonstrate how the inclusion of these corrections is essential to compute predictions with an accuracy that matches the projected precision of "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2401.10127","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2401.10127/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2401.10127","created_at":"2026-07-05T07:49:36.061391+00:00"},{"alias_kind":"arxiv_version","alias_value":"2401.10127v2","created_at":"2026-07-05T07:49:36.061391+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2401.10127","created_at":"2026-07-05T07:49:36.061391+00:00"},{"alias_kind":"pith_short_12","alias_value":"2JTNCMOIAC2U","created_at":"2026-07-05T07:49:36.061391+00:00"},{"alias_kind":"pith_short_16","alias_value":"2JTNCMOIAC2UWBHO","created_at":"2026-07-05T07:49:36.061391+00:00"},{"alias_kind":"pith_short_8","alias_value":"2JTNCMOI","created_at":"2026-07-05T07:49:36.061391+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.17134","citing_title":"PineAPPLv1: fast and flexible theory predictions for present and future colliders","ref_index":17,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2JTNCMOIAC2UWBHO5RGGLASWEV","json":"https://pith.science/pith/2JTNCMOIAC2UWBHO5RGGLASWEV.json","graph_json":"https://pith.science/api/pith-number/2JTNCMOIAC2UWBHO5RGGLASWEV/graph.json","events_json":"https://pith.science/api/pith-number/2JTNCMOIAC2UWBHO5RGGLASWEV/events.json","paper":"https://pith.science/paper/2JTNCMOI"},"agent_actions":{"view_html":"https://pith.science/pith/2JTNCMOIAC2UWBHO5RGGLASWEV","download_json":"https://pith.science/pith/2JTNCMOIAC2UWBHO5RGGLASWEV.json","view_paper":"https://pith.science/paper/2JTNCMOI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2401.10127&json=true","fetch_graph":"https://pith.science/api/pith-number/2JTNCMOIAC2UWBHO5RGGLASWEV/graph.json","fetch_events":"https://pith.science/api/pith-number/2JTNCMOIAC2UWBHO5RGGLASWEV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2JTNCMOIAC2UWBHO5RGGLASWEV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2JTNCMOIAC2UWBHO5RGGLASWEV/action/storage_attestation","attest_author":"https://pith.science/pith/2JTNCMOIAC2UWBHO5RGGLASWEV/action/author_attestation","sign_citation":"https://pith.science/pith/2JTNCMOIAC2UWBHO5RGGLASWEV/action/citation_signature","submit_replication":"https://pith.science/pith/2JTNCMOIAC2UWBHO5RGGLASWEV/action/replication_record"}},"created_at":"2026-07-05T07:49:36.061391+00:00","updated_at":"2026-07-05T07:49:36.061391+00:00"}