{"paper":{"title":"Technical Supplement to \"Polarization Transfer Observables in Elastic Electron-Proton Scattering at Q$^2$ = 2.5, 5.2, 6.8, and 8.5 GeV$^2$\"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"nucl-ex","authors_text":"A. Ahmidouch, A. Asaturyan, A. Daniel, A. Davidenko, A. J. R. Puckett, A. Marsh, A. Mkrtchyan, A. Narayan, A. Shahinyan, A. Vasiliev, B. B. Wojtsekhowski, B. Hu, B. Moffit, C. Butuceanu, C. F. Perdrisat, C. Keppel, D. Day, D. Dutta, D. Gaskell, D. Hamilton, D. J. Margaziotis, D. Kirillov, D. Meekins, D. S. Razin, D. W. Higinbotham, E. Christy, E. Frlez, E. J. Brash, E. Jensen, E. Piasetzky, E. Tomasi-Gustafsson, F. Benmokhtar, F. Garibaldi, F. R. Wesselmann, GEp-2Gamma Collaborations), G. Kumbartzki, G. Mbianda, G. M. Huber, G. Smith, H. Baghdasaryan, H. Fenker, H. Mkrtchyan, I. Albayrak, I. Sitnik, J. Arrington, J. C. Cornejo, J. Huang, J. Maxwell, J. Miller, J. Mulholland, J. Reinhold, K. A. Aniol, K. Hafidi, K. Shestermanov, L. Bimbot, L. Pentchev, L. Smykov, L. Solovyev, L. Zhu (GEp-III, M. Commisso, M. Khandaker, M. K. Jones, M. Kohl, M. Meziane, M. Shabestari, M. Veilleux, N. M. Piskunov, Nurruzzaman, O. Moreno, O. Rondon, P. Bosted, P. Carter, P. King, P. Reimer, P. Solvignon, R. D. Ransome, R. Ent, R. Gilman, R. Subedi, S. Chernenko, S. Covrig, S. Danagoulian, S. Dhamija, S. Frullani, S. Gilad, S. Nedev, S. Sirca, S. Wood, T. Horn, V. Kravtsov, V. Mamyan, V. Punjabi, W. Bertozzi, W. Boeglin, W. Hinton, W. Luo, W. Pierce, X. Zhang, X. Zheng, Y. Goncharenko, Y. Li, Y. Matulenko, Y. Melnik, Y. Prok, Y. Zanevsky, Y. Zhang, Z. Ye","submitted_at":"2017-07-24T21:02:58Z","abstract_excerpt":"The GEp-III and GEp-2$\\gamma$ experiments, carried out in Jefferson Lab's Hall C from 2007-2008, consisted of measurements of polarization transfer in elastic electron-proton scattering at momentum transfers of $Q^2 = 2.5, 5.2, 6.8,$ and $8.54$ GeV$^2$. These measurements were carried out to improve knowledge of the proton electromagnetic form factor ratio $R = \\mu_p G_E^p/G_M^p$ at large values of $Q^2$ and to search for effects beyond the Born approximation in polarization transfer observables at $Q^2 = 2.5$ GeV$^2$. The final results of both experiments were reported in a recent archival pu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.07750","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1707.07750/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"}