{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:SWARHF4ZJ6YDM6ASIMIRL3V6CQ","short_pith_number":"pith:SWARHF4Z","schema_version":"1.0","canonical_sha256":"95811397994fb0367812431115eebe1439067153c7255b6a7ab7395b4d8a57ce","source":{"kind":"arxiv","id":"1806.01177","version":2},"attestation_state":"computed","paper":{"title":"Transversity generalized parton distributions for the deuteron","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"B. Pire, W. Cosyn","submitted_at":"2018-06-04T16:17:08Z","abstract_excerpt":"Transversity generalized parton distributions (GPDs) appear as scalar functions in the decomposition of off-forward quark-quark and gluon-gluon correlators with a parton helicity flip. For a spin 1 hadron, we find 9 transversity GPDs for both quarks and gluons at leading twist 2. We study these twist-2 chiral odd quark transversity GPDs for the deuteron in a light cone convolution model, based on the impulse approximation, and using the lowest Fock-space state for the deuteron."},"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":"1806.01177","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-06-04T16:17:08Z","cross_cats_sorted":["nucl-ex","nucl-th"],"title_canon_sha256":"c1a0f31ed598cf6dce03eb3d97b35ee973e2545b3f538183783658ceb2741df5","abstract_canon_sha256":"9674e82155637a0ce84242839417e7c48dd805dc61d29e55e420fdbfac1d7542"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:02:34.439157Z","signature_b64":"ExClhOKuWIG0TZ+rxgARsvV/NJS4MbJN6Ccy4KP4x87JB6oBYNMm0T6hnF5a/t5MUYGJ3Ulz90Y3SbaWyNNtAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"95811397994fb0367812431115eebe1439067153c7255b6a7ab7395b4d8a57ce","last_reissued_at":"2026-05-18T00:02:34.438610Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:02:34.438610Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Transversity generalized parton distributions for the deuteron","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"B. Pire, W. Cosyn","submitted_at":"2018-06-04T16:17:08Z","abstract_excerpt":"Transversity generalized parton distributions (GPDs) appear as scalar functions in the decomposition of off-forward quark-quark and gluon-gluon correlators with a parton helicity flip. For a spin 1 hadron, we find 9 transversity GPDs for both quarks and gluons at leading twist 2. We study these twist-2 chiral odd quark transversity GPDs for the deuteron in a light cone convolution model, based on the impulse approximation, and using the lowest Fock-space state for the deuteron."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.01177","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":"1806.01177","created_at":"2026-05-18T00:02:34.438721+00:00"},{"alias_kind":"arxiv_version","alias_value":"1806.01177v2","created_at":"2026-05-18T00:02:34.438721+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.01177","created_at":"2026-05-18T00:02:34.438721+00:00"},{"alias_kind":"pith_short_12","alias_value":"SWARHF4ZJ6YD","created_at":"2026-05-18T12:32:53.628368+00:00"},{"alias_kind":"pith_short_16","alias_value":"SWARHF4ZJ6YDM6AS","created_at":"2026-05-18T12:32:53.628368+00:00"},{"alias_kind":"pith_short_8","alias_value":"SWARHF4Z","created_at":"2026-05-18T12:32:53.628368+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1907.08662","citing_title":"Probing quark transversity GPDs in diffractive photo- and electroproduction on the deuteron","ref_index":1,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SWARHF4ZJ6YDM6ASIMIRL3V6CQ","json":"https://pith.science/pith/SWARHF4ZJ6YDM6ASIMIRL3V6CQ.json","graph_json":"https://pith.science/api/pith-number/SWARHF4ZJ6YDM6ASIMIRL3V6CQ/graph.json","events_json":"https://pith.science/api/pith-number/SWARHF4ZJ6YDM6ASIMIRL3V6CQ/events.json","paper":"https://pith.science/paper/SWARHF4Z"},"agent_actions":{"view_html":"https://pith.science/pith/SWARHF4ZJ6YDM6ASIMIRL3V6CQ","download_json":"https://pith.science/pith/SWARHF4ZJ6YDM6ASIMIRL3V6CQ.json","view_paper":"https://pith.science/paper/SWARHF4Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1806.01177&json=true","fetch_graph":"https://pith.science/api/pith-number/SWARHF4ZJ6YDM6ASIMIRL3V6CQ/graph.json","fetch_events":"https://pith.science/api/pith-number/SWARHF4ZJ6YDM6ASIMIRL3V6CQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SWARHF4ZJ6YDM6ASIMIRL3V6CQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SWARHF4ZJ6YDM6ASIMIRL3V6CQ/action/storage_attestation","attest_author":"https://pith.science/pith/SWARHF4ZJ6YDM6ASIMIRL3V6CQ/action/author_attestation","sign_citation":"https://pith.science/pith/SWARHF4ZJ6YDM6ASIMIRL3V6CQ/action/citation_signature","submit_replication":"https://pith.science/pith/SWARHF4ZJ6YDM6ASIMIRL3V6CQ/action/replication_record"}},"created_at":"2026-05-18T00:02:34.438721+00:00","updated_at":"2026-05-18T00:02:34.438721+00:00"}