{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:7RAJYXQXWYCGV6PD6IBDKGUOHL","short_pith_number":"pith:7RAJYXQX","schema_version":"1.0","canonical_sha256":"fc409c5e17b6046af9e3f202351a8e3af03f2f3914fd8b7603773c45cb1a01bd","source":{"kind":"arxiv","id":"2307.09869","version":2},"attestation_state":"computed","paper":{"title":"Spatial imaging of proton via leading-twist non-skewed GPDs with basis light-front quantization","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Chandan Mondal, James P. Vary, Satvir Kaur, Siqi Xu, Xingbo Zhao","submitted_at":"2023-07-19T09:58:03Z","abstract_excerpt":"The internal image of the proton is unveiled by examining the generalized parton distributions (GPDs) at zero skewness, within the basis light-front quantized environment. Several distributions emerge when a quark is sampled with different currents depending upon the helicity arrangements of the active quark and the proton target. We investigate six of the eight leading-twist proton GPDs of the valence quarks, the helicity conserving distributions $(H, E, \\tilde{H})$ and the helicity non-conserving $(H_T,E_T,\\tilde{H}_T)$ distributions at skewness set to zero ($\\zeta=0$). We consider purely tr"},"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":"2307.09869","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-07-19T09:58:03Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"66412e0c296e7b6d24010dc077778c57e41cb8b7e3c17bf3edbc2ce3aed28de5","abstract_canon_sha256":"a6ae08ff73aaab70353202abc535e6f3420e154dc9fa05ef4380702e8d676134"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:35:38.545134Z","signature_b64":"gwRQ3xpdRhVcT7SdEgomr7FkCZjJR21WxfOWqNAhxgeo45opBnd6F5UH9n/b9FlZo7SKmsGNc8GjMV1CP9RMCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fc409c5e17b6046af9e3f202351a8e3af03f2f3914fd8b7603773c45cb1a01bd","last_reissued_at":"2026-07-05T07:35:38.544673Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:35:38.544673Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Spatial imaging of proton via leading-twist non-skewed GPDs with basis light-front quantization","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Chandan Mondal, James P. Vary, Satvir Kaur, Siqi Xu, Xingbo Zhao","submitted_at":"2023-07-19T09:58:03Z","abstract_excerpt":"The internal image of the proton is unveiled by examining the generalized parton distributions (GPDs) at zero skewness, within the basis light-front quantized environment. Several distributions emerge when a quark is sampled with different currents depending upon the helicity arrangements of the active quark and the proton target. We investigate six of the eight leading-twist proton GPDs of the valence quarks, the helicity conserving distributions $(H, E, \\tilde{H})$ and the helicity non-conserving $(H_T,E_T,\\tilde{H}_T)$ distributions at skewness set to zero ($\\zeta=0$). We consider purely tr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2307.09869","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/2307.09869/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":"2307.09869","created_at":"2026-07-05T07:35:38.544730+00:00"},{"alias_kind":"arxiv_version","alias_value":"2307.09869v2","created_at":"2026-07-05T07:35:38.544730+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2307.09869","created_at":"2026-07-05T07:35:38.544730+00:00"},{"alias_kind":"pith_short_12","alias_value":"7RAJYXQXWYCG","created_at":"2026-07-05T07:35:38.544730+00:00"},{"alias_kind":"pith_short_16","alias_value":"7RAJYXQXWYCGV6PD","created_at":"2026-07-05T07:35:38.544730+00:00"},{"alias_kind":"pith_short_8","alias_value":"7RAJYXQX","created_at":"2026-07-05T07:35:38.544730+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.24435","citing_title":"Multipole structure of the nucleon tensor form factors","ref_index":72,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7RAJYXQXWYCGV6PD6IBDKGUOHL","json":"https://pith.science/pith/7RAJYXQXWYCGV6PD6IBDKGUOHL.json","graph_json":"https://pith.science/api/pith-number/7RAJYXQXWYCGV6PD6IBDKGUOHL/graph.json","events_json":"https://pith.science/api/pith-number/7RAJYXQXWYCGV6PD6IBDKGUOHL/events.json","paper":"https://pith.science/paper/7RAJYXQX"},"agent_actions":{"view_html":"https://pith.science/pith/7RAJYXQXWYCGV6PD6IBDKGUOHL","download_json":"https://pith.science/pith/7RAJYXQXWYCGV6PD6IBDKGUOHL.json","view_paper":"https://pith.science/paper/7RAJYXQX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2307.09869&json=true","fetch_graph":"https://pith.science/api/pith-number/7RAJYXQXWYCGV6PD6IBDKGUOHL/graph.json","fetch_events":"https://pith.science/api/pith-number/7RAJYXQXWYCGV6PD6IBDKGUOHL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7RAJYXQXWYCGV6PD6IBDKGUOHL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7RAJYXQXWYCGV6PD6IBDKGUOHL/action/storage_attestation","attest_author":"https://pith.science/pith/7RAJYXQXWYCGV6PD6IBDKGUOHL/action/author_attestation","sign_citation":"https://pith.science/pith/7RAJYXQXWYCGV6PD6IBDKGUOHL/action/citation_signature","submit_replication":"https://pith.science/pith/7RAJYXQXWYCGV6PD6IBDKGUOHL/action/replication_record"}},"created_at":"2026-07-05T07:35:38.544730+00:00","updated_at":"2026-07-05T07:35:38.544730+00:00"}