{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:P5RHFRMEYJ77LPR2HIBDHJZ65W","short_pith_number":"pith:P5RHFRME","schema_version":"1.0","canonical_sha256":"7f6272c584c27ff5be3a3a0233a73eedb37646ea7c176f2311bd8c9fa8c69550","source":{"kind":"arxiv","id":"hep-ph/0504030","version":3},"attestation_state":"computed","paper":{"title":"Unraveling hadron structure with generalized parton distributions","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"A.V. Belitsky, A.V. Radyushkin","submitted_at":"2005-04-05T12:37:57Z","abstract_excerpt":"The generalized parton distributions, introduced nearly a decade ago, have emerged as a universal tool to describe hadrons in terms of quark and gluonic degrees of freedom. They combine the features of form factors, parton densities and distribution amplitudes--the functions used for a long time in studies of hadronic structure. Generalized parton distributions are analogous to the phase-space Wigner quasi-probability function of non-relativistic quantum mechanics which encodes full information on a quantum-mechanical system. We give an extensive review of main achievements in the development "},"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":"hep-ph/0504030","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-04-05T12:37:57Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"e2a40ddcfe683d7a4066d08e849d3c9c9352987d891efcbc13f0009db9f12d37","abstract_canon_sha256":"c27f452e8f75ef79e5689d6ca9039f97621cee43601da8856d1fda30578c6520"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:52:35.955456Z","signature_b64":"iJjgVYM9D5KrqAUmdn38PvDUJPmSj1LhxBT0LqvmyLGuPKmbLogXtHtdq+aAsve5AKztDxcuT5AvifbD8+UzBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7f6272c584c27ff5be3a3a0233a73eedb37646ea7c176f2311bd8c9fa8c69550","last_reissued_at":"2026-07-04T15:52:35.955050Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:52:35.955050Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Unraveling hadron structure with generalized parton distributions","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"A.V. Belitsky, A.V. Radyushkin","submitted_at":"2005-04-05T12:37:57Z","abstract_excerpt":"The generalized parton distributions, introduced nearly a decade ago, have emerged as a universal tool to describe hadrons in terms of quark and gluonic degrees of freedom. They combine the features of form factors, parton densities and distribution amplitudes--the functions used for a long time in studies of hadronic structure. Generalized parton distributions are analogous to the phase-space Wigner quasi-probability function of non-relativistic quantum mechanics which encodes full information on a quantum-mechanical system. We give an extensive review of main achievements in the development "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0504030","kind":"arxiv","version":3},"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/hep-ph/0504030/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":"hep-ph/0504030","created_at":"2026-07-04T15:52:35.955112+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0504030v3","created_at":"2026-07-04T15:52:35.955112+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0504030","created_at":"2026-07-04T15:52:35.955112+00:00"},{"alias_kind":"pith_short_12","alias_value":"P5RHFRMEYJ77","created_at":"2026-07-04T15:52:35.955112+00:00"},{"alias_kind":"pith_short_16","alias_value":"P5RHFRMEYJ77LPR2","created_at":"2026-07-04T15:52:35.955112+00:00"},{"alias_kind":"pith_short_8","alias_value":"P5RHFRME","created_at":"2026-07-04T15:52:35.955112+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":25,"internal_anchor_count":14,"sample":[{"citing_arxiv_id":"2607.08457","citing_title":"Electron-Ion Collision Environment: Distribution of Quark Spin and Orbital Angular Momentum","ref_index":10,"is_internal_anchor":true},{"citing_arxiv_id":"2606.22602","citing_title":"Quantum Simulation of Generalized Parton Distributions in the Schwinger Model","ref_index":7,"is_internal_anchor":true},{"citing_arxiv_id":"2606.20981","citing_title":"Gluon GTMD at strong coupling: fixed-spin saddle factorization and Reggeization","ref_index":25,"is_internal_anchor":true},{"citing_arxiv_id":"2606.09732","citing_title":"Finite-$t$ and target mass corrections for the short-distance expansion of quasi(pseudo) GPDs","ref_index":34,"is_internal_anchor":true},{"citing_arxiv_id":"2606.09152","citing_title":"Constraining DVCS Compton Form Factors Using Lattice QCD informed Neural Network","ref_index":11,"is_internal_anchor":true},{"citing_arxiv_id":"2606.07073","citing_title":"Mechanical distribution of the pseudoscalar charmonium and bottomonium on the light-front","ref_index":10,"is_internal_anchor":true},{"citing_arxiv_id":"2605.03880","citing_title":"Exclusive photoproduction of a di-meson pair with large invariant mass","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2605.24435","citing_title":"Multipole structure of the nucleon tensor form factors","ref_index":63,"is_internal_anchor":true},{"citing_arxiv_id":"2512.24921","citing_title":"Valence quark distribution of the pion inside a medium with finite baryon density: A Nambu--Jona-Lasinio model approach","ref_index":5,"is_internal_anchor":true},{"citing_arxiv_id":"2408.03600","citing_title":"T-odd Wigner Distributions in boost-invariant longitudinal position space and Spin-momentum correlation in proton","ref_index":17,"is_internal_anchor":true},{"citing_arxiv_id":"2512.12315","citing_title":"Gluon Gravitational $ D$-Form Factor: The $\\sigma$-Meson as a Dilaton Confronted with Lattice Data II","ref_index":91,"is_internal_anchor":true},{"citing_arxiv_id":"2603.09686","citing_title":"Probing GPDs in exclusive electroproduction of dijets","ref_index":26,"is_internal_anchor":true},{"citing_arxiv_id":"2604.25677","citing_title":"Coherent deeply virtual Compton scattering on helium-4 beyond leading power","ref_index":8,"is_internal_anchor":true},{"citing_arxiv_id":"2512.14295","citing_title":"Conformal moments of the two-loop coefficient functions in DVCS","ref_index":32,"is_internal_anchor":true},{"citing_arxiv_id":"2604.03832","citing_title":"Gravitational transverse momentum distribution of proton","ref_index":6,"is_internal_anchor":false},{"citing_arxiv_id":"2605.03880","citing_title":"Exclusive photoproduction of a di-meson pair with large invariant mass","ref_index":4,"is_internal_anchor":false},{"citing_arxiv_id":"2604.25677","citing_title":"Coherent deeply virtual Compton scattering on helium-4 beyond leading power","ref_index":8,"is_internal_anchor":false},{"citing_arxiv_id":"2604.24629","citing_title":"On the Two $R$-Factors in the Small-$x$ Shockwave Formalism","ref_index":11,"is_internal_anchor":false},{"citing_arxiv_id":"2605.06412","citing_title":"GTMDs, orbital angular momentum, and pretzelosity","ref_index":4,"is_internal_anchor":false},{"citing_arxiv_id":"2604.21476","citing_title":"Reconstructing the full kinematic dependence of GPDs from pseudo-distributions","ref_index":89,"is_internal_anchor":false},{"citing_arxiv_id":"2604.12038","citing_title":"Holographic Open/Closed Exchange in Double Deeply Virtual Compton Scattering: Fixed-$j$ Structural Matching to the $\\pm$-Basis Wilson Kernels","ref_index":28,"is_internal_anchor":false},{"citing_arxiv_id":"2604.12037","citing_title":"From Vacuum to Nucleon: Fixed-$j$ Kernel Matching of Holographic Current Correlators to QCD","ref_index":6,"is_internal_anchor":false},{"citing_arxiv_id":"2604.11116","citing_title":"Extraction of Pion Unpolarized Quark Generalized Parton Distribution from Charge Form Factors","ref_index":8,"is_internal_anchor":false},{"citing_arxiv_id":"2604.10025","citing_title":"Toward selective quantum advantage in hadronic tomography:explicit cases from Compton form factors, GPDs, TMDs, and GTMDs","ref_index":11,"is_internal_anchor":false},{"citing_arxiv_id":"2605.06994","citing_title":"Neural Network Representation of Generalized Parton Distributions (NNGPD)","ref_index":12,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/P5RHFRMEYJ77LPR2HIBDHJZ65W","json":"https://pith.science/pith/P5RHFRMEYJ77LPR2HIBDHJZ65W.json","graph_json":"https://pith.science/api/pith-number/P5RHFRMEYJ77LPR2HIBDHJZ65W/graph.json","events_json":"https://pith.science/api/pith-number/P5RHFRMEYJ77LPR2HIBDHJZ65W/events.json","paper":"https://pith.science/paper/P5RHFRME"},"agent_actions":{"view_html":"https://pith.science/pith/P5RHFRMEYJ77LPR2HIBDHJZ65W","download_json":"https://pith.science/pith/P5RHFRMEYJ77LPR2HIBDHJZ65W.json","view_paper":"https://pith.science/paper/P5RHFRME","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0504030&json=true","fetch_graph":"https://pith.science/api/pith-number/P5RHFRMEYJ77LPR2HIBDHJZ65W/graph.json","fetch_events":"https://pith.science/api/pith-number/P5RHFRMEYJ77LPR2HIBDHJZ65W/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/P5RHFRMEYJ77LPR2HIBDHJZ65W/action/timestamp_anchor","attest_storage":"https://pith.science/pith/P5RHFRMEYJ77LPR2HIBDHJZ65W/action/storage_attestation","attest_author":"https://pith.science/pith/P5RHFRMEYJ77LPR2HIBDHJZ65W/action/author_attestation","sign_citation":"https://pith.science/pith/P5RHFRMEYJ77LPR2HIBDHJZ65W/action/citation_signature","submit_replication":"https://pith.science/pith/P5RHFRMEYJ77LPR2HIBDHJZ65W/action/replication_record"}},"created_at":"2026-07-04T15:52:35.955112+00:00","updated_at":"2026-07-04T15:52:35.955112+00:00"}