{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:USJRMA7C35TNAQ7TRPBI2GWRTK","short_pith_number":"pith:USJRMA7C","schema_version":"1.0","canonical_sha256":"a4931603e2df66d043f38bc28d1ad19ab5d05a755aab914b9a1ad4ada00b0e44","source":{"kind":"arxiv","id":"1510.02567","version":2},"attestation_state":"computed","paper":{"title":"Modelling the nucleon structure","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"B. Pasquini (Pavia U., INFN-Pavia), M. Burkardt (New Mexico State U.)","submitted_at":"2015-10-09T04:27:20Z","abstract_excerpt":"We review the status of our understanding of nucleon structure based on the modelling of different kinds of parton distributions. We use the concept of generalized transverse momentum dependent parton distributions and Wigner distributions, which combine the features of transverse-momentum dependent parton distributions and generalized parton distributions. We revisit various quark models which account for different aspects of these parton distributions. We then identify applications of these distributions to gain a simple interpretation of key properties of the quark and gluon dynamics in the"},"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":"1510.02567","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-10-09T04:27:20Z","cross_cats_sorted":["hep-ex","nucl-th"],"title_canon_sha256":"83b0f3ba20e5b949bb54143735958765817dcce7608de3e2aba873c04bbb8940","abstract_canon_sha256":"4c7a6db7828a4607af309a15f869539656b23a760233525c4219ce03f39295a8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:10:52.274081Z","signature_b64":"VR+YSgX38VjFPdyZbOzHbY2vxKQKCUudkNvjFmGUaXNI0WU9maC8n/QLhXfW37rN9C52yrkhgfm/zeFDB08MBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a4931603e2df66d043f38bc28d1ad19ab5d05a755aab914b9a1ad4ada00b0e44","last_reissued_at":"2026-05-18T01:10:52.273424Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:10:52.273424Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Modelling the nucleon structure","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"B. Pasquini (Pavia U., INFN-Pavia), M. Burkardt (New Mexico State U.)","submitted_at":"2015-10-09T04:27:20Z","abstract_excerpt":"We review the status of our understanding of nucleon structure based on the modelling of different kinds of parton distributions. We use the concept of generalized transverse momentum dependent parton distributions and Wigner distributions, which combine the features of transverse-momentum dependent parton distributions and generalized parton distributions. We revisit various quark models which account for different aspects of these parton distributions. We then identify applications of these distributions to gain a simple interpretation of key properties of the quark and gluon dynamics in the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.02567","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":"1510.02567","created_at":"2026-05-18T01:10:52.273540+00:00"},{"alias_kind":"arxiv_version","alias_value":"1510.02567v2","created_at":"2026-05-18T01:10:52.273540+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.02567","created_at":"2026-05-18T01:10:52.273540+00:00"},{"alias_kind":"pith_short_12","alias_value":"USJRMA7C35TN","created_at":"2026-05-18T12:29:44.643036+00:00"},{"alias_kind":"pith_short_16","alias_value":"USJRMA7C35TNAQ7T","created_at":"2026-05-18T12:29:44.643036+00:00"},{"alias_kind":"pith_short_8","alias_value":"USJRMA7C","created_at":"2026-05-18T12:29:44.643036+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2512.24855","citing_title":"QCD Wehrl and entanglement entropies in a gluon spectator model at small-$x$","ref_index":52,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/USJRMA7C35TNAQ7TRPBI2GWRTK","json":"https://pith.science/pith/USJRMA7C35TNAQ7TRPBI2GWRTK.json","graph_json":"https://pith.science/api/pith-number/USJRMA7C35TNAQ7TRPBI2GWRTK/graph.json","events_json":"https://pith.science/api/pith-number/USJRMA7C35TNAQ7TRPBI2GWRTK/events.json","paper":"https://pith.science/paper/USJRMA7C"},"agent_actions":{"view_html":"https://pith.science/pith/USJRMA7C35TNAQ7TRPBI2GWRTK","download_json":"https://pith.science/pith/USJRMA7C35TNAQ7TRPBI2GWRTK.json","view_paper":"https://pith.science/paper/USJRMA7C","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1510.02567&json=true","fetch_graph":"https://pith.science/api/pith-number/USJRMA7C35TNAQ7TRPBI2GWRTK/graph.json","fetch_events":"https://pith.science/api/pith-number/USJRMA7C35TNAQ7TRPBI2GWRTK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/USJRMA7C35TNAQ7TRPBI2GWRTK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/USJRMA7C35TNAQ7TRPBI2GWRTK/action/storage_attestation","attest_author":"https://pith.science/pith/USJRMA7C35TNAQ7TRPBI2GWRTK/action/author_attestation","sign_citation":"https://pith.science/pith/USJRMA7C35TNAQ7TRPBI2GWRTK/action/citation_signature","submit_replication":"https://pith.science/pith/USJRMA7C35TNAQ7TRPBI2GWRTK/action/replication_record"}},"created_at":"2026-05-18T01:10:52.273540+00:00","updated_at":"2026-05-18T01:10:52.273540+00:00"}