{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:WHKBYFVEHG737OZ5ZNFISQ3AN2","short_pith_number":"pith:WHKBYFVE","schema_version":"1.0","canonical_sha256":"b1d41c16a439bfbfbb3dcb4a8943606eacdef326a9e19109f8ef9c7b4c22b4e3","source":{"kind":"arxiv","id":"hep-ph/0512220","version":1},"attestation_state":"computed","paper":{"title":"Ultra-High Energy Neutrino-Nucleon Scattering and Parton Distributions at Small $x$","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ernest M. Henley, Jamal Jalilian-Marian","submitted_at":"2005-12-16T23:31:12Z","abstract_excerpt":"The cross section for ultra-high energy neutrino-nucleon scattering is very sensitive to the parton distributions at very small values of Bjorken x ($x \\leq 10^{-4})$. We numerically investigate the effects of modifying the behavior of the gluon distribution function at very small $x$ in the DGLAP evolution equation. We then use the Color Glass Condensate formalism to calculate the neutrino-nucleon cross section at ultra-high energies and compare the result with those based on modification of DGLAP evolution equation."},"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/0512220","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-12-16T23:31:12Z","cross_cats_sorted":[],"title_canon_sha256":"63c0f33a276526c206bedd86020096ec55351e2f57ef0c90fb8353ac068f3926","abstract_canon_sha256":"5ecdc487abb7b24473305ca0f07a95348615b8389e9e80c3910615c7d0c74bb3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:36:18.980154Z","signature_b64":"GrDOMRpTnMRMYUtqntcCbH1PB4eE29KfC2yQhBEEmUJmxDjyMbbbWALpWF9HrrtZ6TCUwacrY2qQakBUXoFIAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b1d41c16a439bfbfbb3dcb4a8943606eacdef326a9e19109f8ef9c7b4c22b4e3","last_reissued_at":"2026-05-18T02:36:18.979537Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:36:18.979537Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Ultra-High Energy Neutrino-Nucleon Scattering and Parton Distributions at Small $x$","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ernest M. Henley, Jamal Jalilian-Marian","submitted_at":"2005-12-16T23:31:12Z","abstract_excerpt":"The cross section for ultra-high energy neutrino-nucleon scattering is very sensitive to the parton distributions at very small values of Bjorken x ($x \\leq 10^{-4})$. We numerically investigate the effects of modifying the behavior of the gluon distribution function at very small $x$ in the DGLAP evolution equation. We then use the Color Glass Condensate formalism to calculate the neutrino-nucleon cross section at ultra-high energies and compare the result with those based on modification of DGLAP evolution equation."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0512220","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":"hep-ph/0512220","created_at":"2026-05-18T02:36:18.979620+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0512220v1","created_at":"2026-05-18T02:36:18.979620+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0512220","created_at":"2026-05-18T02:36:18.979620+00:00"},{"alias_kind":"pith_short_12","alias_value":"WHKBYFVEHG73","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_16","alias_value":"WHKBYFVEHG737OZ5","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_8","alias_value":"WHKBYFVE","created_at":"2026-05-18T12:25:53.939244+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/WHKBYFVEHG737OZ5ZNFISQ3AN2","json":"https://pith.science/pith/WHKBYFVEHG737OZ5ZNFISQ3AN2.json","graph_json":"https://pith.science/api/pith-number/WHKBYFVEHG737OZ5ZNFISQ3AN2/graph.json","events_json":"https://pith.science/api/pith-number/WHKBYFVEHG737OZ5ZNFISQ3AN2/events.json","paper":"https://pith.science/paper/WHKBYFVE"},"agent_actions":{"view_html":"https://pith.science/pith/WHKBYFVEHG737OZ5ZNFISQ3AN2","download_json":"https://pith.science/pith/WHKBYFVEHG737OZ5ZNFISQ3AN2.json","view_paper":"https://pith.science/paper/WHKBYFVE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0512220&json=true","fetch_graph":"https://pith.science/api/pith-number/WHKBYFVEHG737OZ5ZNFISQ3AN2/graph.json","fetch_events":"https://pith.science/api/pith-number/WHKBYFVEHG737OZ5ZNFISQ3AN2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WHKBYFVEHG737OZ5ZNFISQ3AN2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WHKBYFVEHG737OZ5ZNFISQ3AN2/action/storage_attestation","attest_author":"https://pith.science/pith/WHKBYFVEHG737OZ5ZNFISQ3AN2/action/author_attestation","sign_citation":"https://pith.science/pith/WHKBYFVEHG737OZ5ZNFISQ3AN2/action/citation_signature","submit_replication":"https://pith.science/pith/WHKBYFVEHG737OZ5ZNFISQ3AN2/action/replication_record"}},"created_at":"2026-05-18T02:36:18.979620+00:00","updated_at":"2026-05-18T02:36:18.979620+00:00"}