{"id":{"repo_id":"uiuc","oai_identifier":"oai:www.ideals.illinois.edu:2142/18867"},"canonical_url":"https://search.dev.ndltd.org/etd/uiuc/oai:www.ideals.illinois.edu:2142/18867","repository":{"repo_id":"uiuc","name":"University of Illinois - Urbana-Champaign","base_url":"https://www.ideals.illinois.edu/oai-pmh"},"display":{"title":"\"Non- D`D decays of the y\"\" (3770)\"","abstract":"\"A search for inclusive non-D D decays of the '1'\"\"(3770) is performed in a sample of 9.56±0.48 pb-1 collected by the Mark III detector at the SPEAR storage ring, at the Stanford Linear Accelerator Center. To be more specific, a search for inclusive p, A, and c)l decay modes of the '1'\"\"(3770) is performed in this data sample. Backgrounds due to the decays of the radiatively produced '1''(3686) are subtracted. Also backgrounds due to the production of the same final state by ~onresonant e+e- annihilation are subtracted. After further background subtractions from D meson decays and particle misidentifiction and efficiency corrections no events are seen and upper limits are placed for each one of these decay channels.\"","abstract_html":""A search for inclusive non-D D decays of the '1'""(3770) is performed in a sample of 9.56±0.48 pb-1 collected by the Mark III detector at the SPEAR storage ring, at the Stanford Linear Accelerator Center. To be more specific, a search for inclusive p, A, and c)l decay modes of the '1'""(3770) is performed in this data sample. Backgrounds due to the decays of the radiatively produced '1''(3686) are subtracted. Also backgrounds due to the production of the same final state by ~onresonant e+e- annihilation are subtracted. After further background subtractions from D meson decays and particle misidentifiction and efficiency corrections no events are seen and upper limits are placed for each one of these decay channels."","abstract_has_math":false,"creators":["Majid, Walid Abdul"],"institution":null,"degree_name":"Ph.D.","degree_level":"Dissertation","degree_discipline":"Physics","degree_department":null,"school":null,"contributors":["Thaler, Jonathan J."],"advisors":[],"committee_chairs":[],"committee_members":[],"year":2011,"date_issued":"2011-04-25T15:22:01Z","date_published":"2011-04-25T15:22:01Z","updated_at":"2026-07-22T22:25:11Z","subjects":["inclusive non-DD decays","Mark III","Stanford Linear Accelerator Center","decay modes"],"languages":["en"],"rights":["Copyright 1993 Walid Abdul Majid"],"rights_urls":[],"identifier_entries":[{"key":"dc:identifier","label":"Identifier","values":["3644324"],"render_values":[{"text":"3644324","href":null,"code":true}]}]},"links":{"outbound_url":"http://hdl.handle.net/2142/18867","outbound_label":"Handle","outbound_source":"dc:identifier"},"metadata_groups":[{"id":"people","label":"People","entries":[{"key":"dc:contributor","label":"Contributor","values":["Thaler, Jonathan J."]},{"key":"dc:creator","label":"Author","values":["Majid, Walid Abdul"]}]},{"id":"academic_context","label":"Academic Context","entries":[{"key":"dc:date","label":"Dc Date","values":["2011-04-25T15:22:01Z","10000-01-01","1993-10"]},{"key":"dc:type","label":"Dc Type","values":["Dissertation / Thesis","text"]},{"key":"thesis:degree_discipline","label":"Discipline","values":["Physics"]},{"key":"thesis:degree_level","label":"Degree Level","values":["Dissertation"]},{"key":"thesis:degree_name","label":"Degree Name","values":["Ph.D."]}]},{"id":"subjects_keywords","label":"Subjects and Keywords","entries":[{"key":"dc:subject","label":"Dc Subject","values":["inclusive non-DD decays","Mark III","Stanford Linear Accelerator Center","decay modes"]}]},{"id":"language_rights","label":"Language and Rights","entries":[{"key":"dc:language","label":"Dc Language","values":["en"]},{"key":"dc:rights","label":"Dc Rights","values":["Copyright 1993 Walid Abdul Majid"]}]},{"id":"identifiers","label":"Identifiers","entries":[{"key":"dc:identifier","label":"Identifier","values":["3644324","http://hdl.handle.net/2142/18867"]}]},{"id":"additional","label":"Additional Metadata","entries":[{"key":"dc:description","label":"Description","values":["\"A search for inclusive non-D D decays of the '1'\"\"(3770) is performed in a sample of 9.56±0.48 pb-1 collected by the Mark III detector at the SPEAR storage ring, at the Stanford Linear Accelerator Center. To be more specific, a search for inclusive p, A, and c)l decay modes of the '1'\"\"(3770) is performed in this data sample. Backgrounds due to the decays of the radiatively produced '1''(3686) are subtracted. Also backgrounds due to the production of the same final state by ~onresonant e+e- annihilation are subtracted. After further background subtractions from D meson decays and particle misidentifiction and efficiency corrections no events are seen and upper limits are placed for each one of these decay channels.\"","Submitted by Carolyn Mead (cmead2@illinois.edu) on 2011-04-25T15:22:01Z No. of bitstreams: 1 1993_majid.pdf: 7917350 bytes, checksum: 44244885e98fbcf2b558f3fdd1987411 (MD5)","Made available in DSpace on 2011-04-25T15:22:01Z (GMT). No. of bitstreams: 1 1993_majid.pdf: 7917350 bytes, checksum: 44244885e98fbcf2b558f3fdd1987411 (MD5) Previous issue date: 1993-10","Item marked as restricted to the 'UIUC Users [automated]' Group (id=2) by Carolyn Mead (cmead2@illinois.edu) on 2011-04-25T15:22:01Z Item is restricted indefinitely.","Restriction data tranferred 2014-07-01T11:12:10-05:00 Original Data Group with Access UIUC Users [automated] Release Date: none Reason: Thesis","Thesis","U of I Only"]},{"key":"dc:title","label":"Title","values":["\"Non- D`D decays of the y\"\" (3770)\""]}]}],"canonical_facts":{"dc:contributor":["Thaler, Jonathan J."],"dc:creator":["Majid, Walid Abdul"],"dc:date":["2011-04-25T15:22:01Z","10000-01-01","1993-10"],"dc:description":["\"A search for inclusive non-D D decays of the '1'\"\"(3770) is performed in a sample of 9.56±0.48 pb-1 collected by the Mark III detector at the SPEAR storage ring, at the Stanford Linear Accelerator Center. To be more specific, a search for inclusive p, A, and c)l decay modes of the '1'\"\"(3770) is performed in this data sample. Backgrounds due to the decays of the radiatively produced '1''(3686) are subtracted. Also backgrounds due to the production of the same final state by ~onresonant e+e- annihilation are subtracted. After further background subtractions from D meson decays and particle misidentifiction and efficiency corrections no events are seen and upper limits are placed for each one of these decay channels.\"","Submitted by Carolyn Mead (cmead2@illinois.edu) on 2011-04-25T15:22:01Z No. of bitstreams: 1 1993_majid.pdf: 7917350 bytes, checksum: 44244885e98fbcf2b558f3fdd1987411 (MD5)","Made available in DSpace on 2011-04-25T15:22:01Z (GMT). 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