{"paper":{"title":"Inclusive {\\Lambda} production in proton-proton collisions at 3.5 GeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. Blanco, A. Dybczak, A. Ierusalimov, A. Ivashkin, A. Kr\\'asa, A. Kugler, A. Kurepin, A. Kurilkin, A. Lebedev, A. Mangiarotti, A. Reshetin, A. Rost, A. Rustamov, A. Sadovsky, A. Tarantola, B. K\\\"ampfer, B. Kardan, B. Ramstein, B. W. Kolb, C. Behnke, C. Blume, C. Deveaux, C. Franco, C. H\\\"ohne, C. M\\\"untz, C. Sturm, C. Wendisch, E. Epple, E. Krebs, E.T. Atomssa, F. Guber, G. Agakishiev, G. Korcyl, G. Kornakov, H. Kuc, H. Schuldes, H. Str\\\"obele, H. Tsertos, I. Fr\\\"ohlich, I. Koenig, J. Adamczewski-Musch, J. A. Garz\\'on, J. Biernat, J.C. Berger-Chen, J. Dreyer, J. Friese, J. Markert, J. Michel, J. Pietraszko, J. Siebenson, J. Stroth, J. Wirth, K. Gill, K. Lapidus, K. Schmidt-Sommerfeld, K. Teilab, L. Fabbietti, L. Lopes, L. Maier, L. Naumann, L. Rehnisch, L. Silva, M. B\\\"ohmer, M. Golubeva, M. Gumberidze, M. Jurkovic, M. Lorenz, M. Palka, M. Traxler, O. Arnold, O. Fateev, O. Pechenova, O. Svoboda, P. Bordalo, P. Fonte, P. Kurilkin, P. Salabura, P. Sellheim, P. Strzempek, P. Tlusty, P. Zumbruch, R. Holzmann, R. Kotte, R. Lalik, R. M\\\"unzer, S. Chernenko, S. Harabasz, S. Hlavac, S. Maurus, S. Morozov, S. Ramos, S. Spataroe, T. Galatyuk, T. Hennino, T. Karavicheva, T. Kunz, T. Mahmoud, T. Scheib, T. Vasiliev, V. Ladygin, V. Metag, V. Pechenov, V. Petousis, V. Wagner, W. Koenig, W. Przygoda, Y. Parpottas, Yu.G. Sobolev, Y. Zanevsky","submitted_at":"2016-11-03T14:24:38Z","abstract_excerpt":"The inclusive production of {\\Lambda} hyperons in proton-proton collisions at $\\sqrt{s}$ = 3.18 GeV was measured with HADES at the GSI Helmholtzzentrum f\\\"ur Schwerionenforschung in Darmstadt. The experimental data are compared to a data-based model for individual exclusive {\\Lambda} production channels in the same reaction. The contributions of intermediate resonances such as {\\Sigma}(1385), {\\Delta}++ or N* are considered in detail. In particular, the result of a partial wave analysis is accounted for the abundant pK$^+${\\Lambda} final state. Model and data show a reasonable agreement at mid"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.01040","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"}