{"paper":{"title":"Mass Effects On The Nucleon Sea Structure Functions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Sun Myong Kim","submitted_at":"2001-11-07T13:06:49Z","abstract_excerpt":"Nucleon sea structure functions are studied using Dokshitzer-Gribov-Lipatov-Altarelli-Parisi (DGLAP) equations with the massive gluon-quark splitting kernels for strange and charm quarks, the massless gluon-quark splitting kernels for up and down quarks, and the massless kernels for all other splitting parts. The $SU(2)_f$ flavor symmetry for two light quarks, `up' and `down', is assumed. Gl\\\"uck-Reya-Vogt(GRV) and Martin-Roberts-Stirling(MRS) sets are chosen to be the base structure functions at $Q_0^2=3$GeV$^2$. We evolve the sea structure functions from $Q_0^2=3$ GeV$^2$ to $Q^2=50$ GeV$^2$"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0111070","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"}