{"paper":{"title":"Production cross sections of gamma-rays, electrons, and positrons in p-p collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-ph"],"primary_cat":"astro-ph.HE","authors_text":"K. Kohri, R. Yamazaki, T. Shibata, Y. Ohira","submitted_at":"2013-04-03T09:11:55Z","abstract_excerpt":"Because the production cross sections of gamma-rays, electrons, and positrons made in p-p collisions, $\\sigma_{pp\\rightarrow \\gamma}$ and $\\sigma_{pp\\rightarrow {e}^\\pm}$, respectively, are kinematically equivalent with respect to the parent pion-production cross section $\\sigma_{pp\\rightarrow \\pi}$, we obtain $\\sigma_{pp\\rightarrow {e}^\\pm}$ directly from the machine data on $\\sigma_{pp\\rightarrow \\gamma}$. In Sato et al. (2012), we give explicitly $\\sigma_{pp\\rightarrow \\gamma}$, reproducing quite well the accelerator data with LHC, namely $\\sigma_{pp\\rightarrow {e}^\\pm}$ is applicable enoug"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1304.0879","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":""},"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"}