{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:REQQ577ST4VKJG66NVYHG4AI5M","short_pith_number":"pith:REQQ577S","schema_version":"1.0","canonical_sha256":"89210efff29f2aa49bde6d70737008eb3c8705d6358918c2c6ee0409622dcbc1","source":{"kind":"arxiv","id":"0903.1723","version":2},"attestation_state":"computed","paper":{"title":"The Nucleon Distribution Amplitudes and their application to nucleon form factors and the $N \\to \\Delta$ transition at intermediate values of $Q^2$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Alexander Lenz, Meinulf G\\\"ockeler, Nikolaus Warkentin, Thomas Kaltenbrunner","submitted_at":"2009-03-10T09:57:15Z","abstract_excerpt":"We compare a recent lattice determination of the nucleon distribution amplitudes with other approaches and models. We study the nucleon distribution amplitudes up to twist 6 in next-to leading conformal spin and we also investigate conformal d-wave contributions to the leading twist distribution amplitude. With the help of light-cone sum rules one can relate the distribution amplitudes to the form factors of the nucleon or the $ N \\to \\Delta$ transition at intermediate values of the momentum transfer. We compare our results with experimental data in the range 1 GeV$^2 \\leq Q^2 \\leq 10$ GeV$^2$"},"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":"0903.1723","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-03-10T09:57:15Z","cross_cats_sorted":["nucl-ex","nucl-th"],"title_canon_sha256":"7091d5e97d1ce6c78990fd2caf3bb5784e866d687a740cc93898b2eb8d16cff5","abstract_canon_sha256":"24b53927585e8e1388855db36d95e8d90ffa6f3f2dcd8f2aeefa58c13c9b3ee3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:47:02.486401Z","signature_b64":"BrAF71eqhMV7/KGfhFmjDjyajUeGLN2S6z6Jcmr7srDkwsu61Ly1SH9AdsR1vb4+rGQxkVq3j5xtwE9sejdaAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"89210efff29f2aa49bde6d70737008eb3c8705d6358918c2c6ee0409622dcbc1","last_reissued_at":"2026-07-04T15:47:02.486022Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:47:02.486022Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Nucleon Distribution Amplitudes and their application to nucleon form factors and the $N \\to \\Delta$ transition at intermediate values of $Q^2$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Alexander Lenz, Meinulf G\\\"ockeler, Nikolaus Warkentin, Thomas Kaltenbrunner","submitted_at":"2009-03-10T09:57:15Z","abstract_excerpt":"We compare a recent lattice determination of the nucleon distribution amplitudes with other approaches and models. We study the nucleon distribution amplitudes up to twist 6 in next-to leading conformal spin and we also investigate conformal d-wave contributions to the leading twist distribution amplitude. With the help of light-cone sum rules one can relate the distribution amplitudes to the form factors of the nucleon or the $ N \\to \\Delta$ transition at intermediate values of the momentum transfer. We compare our results with experimental data in the range 1 GeV$^2 \\leq Q^2 \\leq 10$ GeV$^2$"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0903.1723","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/0903.1723/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":"0903.1723","created_at":"2026-07-04T15:47:02.486096+00:00"},{"alias_kind":"arxiv_version","alias_value":"0903.1723v2","created_at":"2026-07-04T15:47:02.486096+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0903.1723","created_at":"2026-07-04T15:47:02.486096+00:00"},{"alias_kind":"pith_short_12","alias_value":"REQQ577ST4VK","created_at":"2026-07-04T15:47:02.486096+00:00"},{"alias_kind":"pith_short_16","alias_value":"REQQ577ST4VKJG66","created_at":"2026-07-04T15:47:02.486096+00:00"},{"alias_kind":"pith_short_8","alias_value":"REQQ577S","created_at":"2026-07-04T15:47:02.486096+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/REQQ577ST4VKJG66NVYHG4AI5M","json":"https://pith.science/pith/REQQ577ST4VKJG66NVYHG4AI5M.json","graph_json":"https://pith.science/api/pith-number/REQQ577ST4VKJG66NVYHG4AI5M/graph.json","events_json":"https://pith.science/api/pith-number/REQQ577ST4VKJG66NVYHG4AI5M/events.json","paper":"https://pith.science/paper/REQQ577S"},"agent_actions":{"view_html":"https://pith.science/pith/REQQ577ST4VKJG66NVYHG4AI5M","download_json":"https://pith.science/pith/REQQ577ST4VKJG66NVYHG4AI5M.json","view_paper":"https://pith.science/paper/REQQ577S","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0903.1723&json=true","fetch_graph":"https://pith.science/api/pith-number/REQQ577ST4VKJG66NVYHG4AI5M/graph.json","fetch_events":"https://pith.science/api/pith-number/REQQ577ST4VKJG66NVYHG4AI5M/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/REQQ577ST4VKJG66NVYHG4AI5M/action/timestamp_anchor","attest_storage":"https://pith.science/pith/REQQ577ST4VKJG66NVYHG4AI5M/action/storage_attestation","attest_author":"https://pith.science/pith/REQQ577ST4VKJG66NVYHG4AI5M/action/author_attestation","sign_citation":"https://pith.science/pith/REQQ577ST4VKJG66NVYHG4AI5M/action/citation_signature","submit_replication":"https://pith.science/pith/REQQ577ST4VKJG66NVYHG4AI5M/action/replication_record"}},"created_at":"2026-07-04T15:47:02.486096+00:00","updated_at":"2026-07-04T15:47:02.486096+00:00"}