{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:NESOSKN5HAWAMDQDKVHBJGJXPJ","short_pith_number":"pith:NESOSKN5","schema_version":"1.0","canonical_sha256":"6924e929bd382c060e03554e1499377a7d96f73f6885928e58433c4bb1a64574","source":{"kind":"arxiv","id":"1501.04745","version":1},"attestation_state":"computed","paper":{"title":"Generalized Parton Distributions of proton for non zero skewness in transverse and longitudinal position spaces","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Harleen Dahiya, Narinder Kumar","submitted_at":"2015-01-20T09:35:00Z","abstract_excerpt":"We investigate the Generalized Parton Distributions(GPDs) of proton by expressing them in terms of overlaps of light front wave functions (LFWFs) using a simulated model which is able to qualitatively improve the convergence near the end points of $x$. We study the spin non-flip $H(x, \\zeta, t)$ and spin flip $E(x, \\zeta, t)$ part of GPDs for the particle conserving $n \\rightarrow n$ overlap in the DGLAP region $(\\zeta<x<1)$. The Fourier transform (FT) of the GPDs w.r.t. to the transverse momentum transfer as well the FT of the GPDs w.r.t. $\\zeta$ have also been obtained giving the distributio"},"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":"1501.04745","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-01-20T09:35:00Z","cross_cats_sorted":[],"title_canon_sha256":"18d7542c74db7a7453d6bc58327e1dfb96631785f6fb609b671cfb35ca7c126a","abstract_canon_sha256":"1aa84d623740449e3f97cb40be4f25932d5679af27aa6a2972341d30e88cd8e4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:29:02.942811Z","signature_b64":"xyQn/HhXrXYr3Uf/Jb+0tvLYbMAs8Jux0I5DjlwQwP1k1e7gnj9iITcd4rSb2714MRoow83Vxxf+WzBInJbHDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6924e929bd382c060e03554e1499377a7d96f73f6885928e58433c4bb1a64574","last_reissued_at":"2026-05-18T02:29:02.942362Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:29:02.942362Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Generalized Parton Distributions of proton for non zero skewness in transverse and longitudinal position spaces","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Harleen Dahiya, Narinder Kumar","submitted_at":"2015-01-20T09:35:00Z","abstract_excerpt":"We investigate the Generalized Parton Distributions(GPDs) of proton by expressing them in terms of overlaps of light front wave functions (LFWFs) using a simulated model which is able to qualitatively improve the convergence near the end points of $x$. We study the spin non-flip $H(x, \\zeta, t)$ and spin flip $E(x, \\zeta, t)$ part of GPDs for the particle conserving $n \\rightarrow n$ overlap in the DGLAP region $(\\zeta<x<1)$. The Fourier transform (FT) of the GPDs w.r.t. to the transverse momentum transfer as well the FT of the GPDs w.r.t. $\\zeta$ have also been obtained giving the distributio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.04745","kind":"arxiv","version":1},"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":"1501.04745","created_at":"2026-05-18T02:29:02.942433+00:00"},{"alias_kind":"arxiv_version","alias_value":"1501.04745v1","created_at":"2026-05-18T02:29:02.942433+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.04745","created_at":"2026-05-18T02:29:02.942433+00:00"},{"alias_kind":"pith_short_12","alias_value":"NESOSKN5HAWA","created_at":"2026-05-18T12:29:32.376354+00:00"},{"alias_kind":"pith_short_16","alias_value":"NESOSKN5HAWAMDQD","created_at":"2026-05-18T12:29:32.376354+00:00"},{"alias_kind":"pith_short_8","alias_value":"NESOSKN5","created_at":"2026-05-18T12:29:32.376354+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"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":54,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NESOSKN5HAWAMDQDKVHBJGJXPJ","json":"https://pith.science/pith/NESOSKN5HAWAMDQDKVHBJGJXPJ.json","graph_json":"https://pith.science/api/pith-number/NESOSKN5HAWAMDQDKVHBJGJXPJ/graph.json","events_json":"https://pith.science/api/pith-number/NESOSKN5HAWAMDQDKVHBJGJXPJ/events.json","paper":"https://pith.science/paper/NESOSKN5"},"agent_actions":{"view_html":"https://pith.science/pith/NESOSKN5HAWAMDQDKVHBJGJXPJ","download_json":"https://pith.science/pith/NESOSKN5HAWAMDQDKVHBJGJXPJ.json","view_paper":"https://pith.science/paper/NESOSKN5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1501.04745&json=true","fetch_graph":"https://pith.science/api/pith-number/NESOSKN5HAWAMDQDKVHBJGJXPJ/graph.json","fetch_events":"https://pith.science/api/pith-number/NESOSKN5HAWAMDQDKVHBJGJXPJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NESOSKN5HAWAMDQDKVHBJGJXPJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NESOSKN5HAWAMDQDKVHBJGJXPJ/action/storage_attestation","attest_author":"https://pith.science/pith/NESOSKN5HAWAMDQDKVHBJGJXPJ/action/author_attestation","sign_citation":"https://pith.science/pith/NESOSKN5HAWAMDQDKVHBJGJXPJ/action/citation_signature","submit_replication":"https://pith.science/pith/NESOSKN5HAWAMDQDKVHBJGJXPJ/action/replication_record"}},"created_at":"2026-05-18T02:29:02.942433+00:00","updated_at":"2026-05-18T02:29:02.942433+00:00"}