{"paper":{"title":"Diffractive $\\phi$-meson photoproduction on proton near threshold","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A.I. Titov, A. Sakaguchi, A. Wakai, C. Rangacharyulu, C.W. Wang, D.S. Ahn, D.S. Oshuev, H. Akimune, H. Ejiri, H. Fujimura, H. Kawai, H. Kohri, H. Ohkuma, H. Shimizu, H. Toyokawa, J.K. Ahn, K. Hicks, K. Imai, K. Kino, K. Miwa, K. Yonehara, M. Fujiwara, M. Miyabe, M. Morita, M. Niiyama, M. Nomachi, M. Sumihama, M. Yoshimura, M. Yosoi, N. Kumagai, N. Matsuoka, N. Muramatsu, P.M. Shagin, R.G.T. Zegers, S.C. Wang, S. Date\\', S. Makino, T. Hotta, T. Ishikawa, T. Iwata, T. Matsuda, T. Matsumura, T. Mibe, T. Nakano, T. Ooba, T. Sasaki, T. Yorita, W.C. Chang, Y. Asano, Y. Miyachi, Y. Ohashi, Y. Shiino, Y. Sugaya, Y. Toi, Z.Y. Kim","submitted_at":"2005-06-10T23:12:10Z","abstract_excerpt":"Photoproduction of $\\phi$-meson on protons was studied by means of linearly polarized photons at forward angles in the low-energy region from threshold to $E_{\\gamma}$= 2.37 GeV. The differential cross sections at $t = -|t|_{min}$ do not increase smoothly as $E_{\\gamma}$ increases, but show a local maximum at around 2.0 GeV. The angular distributions demonstrate that $\\phi$-mesons are photo-produced predominantly by helicity-conserving processes, and the local maximum is not likely due to unnatural-parity processes."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-ex/0506015","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/nucl-ex/0506015/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"}