{"id":{"repo_id":"uiuc","oai_identifier":"oai:www.ideals.illinois.edu:2142/77360"},"canonical_url":"https://search.dev.ndltd.org/etd/uiuc/oai:www.ideals.illinois.edu:2142/77360","repository":{"repo_id":"uiuc","name":"University of Illinois - Urbana-Champaign","base_url":"https://www.ideals.illinois.edu/oai-pmh"},"display":{"title":"Forward Charge Distributions Associated With Hadronically Produced J/psi Particles","abstract":"We have measured the forward charge as a function of x(,F) of the psi for events produced by 225 Gev/c (pi)('-) Be interactions. The forward charge is the average difference between the number of positive hadrons and negative hadrons produced in the forward hemisphere. The standard Drell-Yan model predicts that the forward charge should become less negative as the x(,F) of the J/psi increases. The measured forward charge becomes more negative as the x(,F) of the J/psi increases although it is consistent with being flat as a function of x(,F). Hence, the data is not consistent with any Drell-Yan type model which assumes the forward charge is not strongly dependent on the hadronic energy left over after the J/psi is formed.","abstract_html":"We have measured the forward charge as a function of x(,F) of the psi for events produced by 225 Gev/c (pi)(&#x27;-) Be interactions. The forward charge is the average difference between the number of positive hadrons and negative hadrons produced in the forward hemisphere. The standard Drell-Yan model predicts that the forward charge should become less negative as the x(,F) of the J/psi increases. The measured forward charge becomes more negative as the x(,F) of the J/psi increases although it is consistent with being flat as a function of x(,F). Hence, the data is not consistent with any Drell-Yan type model which assumes the forward charge is not strongly dependent on the hadronic energy left over after the J/psi is formed.","abstract_has_math":false,"creators":["Budd, Howard Scott"],"institution":"University of Illinois at Urbana-Champaign","degree_name":"Ph.D.","degree_level":"Dissertation","degree_discipline":"Physics","degree_department":null,"school":null,"contributors":[],"advisors":[],"committee_chairs":[],"committee_members":[],"year":2015,"date_issued":"2015-05-13T15:41:41Z","date_published":"2015-05-13T15:41:41Z","updated_at":"2026-07-22T22:26:10Z","subjects":["Physics, Elementary Particles and High Energy"],"languages":["eng"],"rights":[],"rights_urls":[],"identifier_entries":[{"key":"dc:identifier","label":"Identifier","values":["(UMI)AAI8409875"],"render_values":[{"text":"(UMI)AAI8409875","href":null,"code":true}]}]},"links":{"outbound_url":"http://hdl.handle.net/2142/77360","outbound_label":"Handle","outbound_source":"dc:identifier"},"metadata_groups":[{"id":"people","label":"People","entries":[{"key":"dc:creator","label":"Author","values":["Budd, Howard Scott"]}]},{"id":"academic_context","label":"Academic Context","entries":[{"key":"dc:date","label":"Dc Date","values":["2015-05-13T15:41:41Z","10000-01-01","1983"]},{"key":"dc:type","label":"Dc Type","values":["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."]},{"key":"thesis:institution_name","label":"Thesis Institution Name","values":["University of Illinois at Urbana-Champaign"]}]},{"id":"subjects_keywords","label":"Subjects and Keywords","entries":[{"key":"dc:subject","label":"Dc Subject","values":["Physics, Elementary Particles and High Energy"]}]},{"id":"language_rights","label":"Language and Rights","entries":[{"key":"dc:language","label":"Dc Language","values":["eng"]}]},{"id":"identifiers","label":"Identifiers","entries":[{"key":"dc:identifier","label":"Identifier","values":["http://hdl.handle.net/2142/77360","(UMI)AAI8409875"]}]},{"id":"additional","label":"Additional Metadata","entries":[{"key":"dc:description","label":"Description","values":["We have measured the forward charge as a function of x(,F) of the psi for events produced by 225 Gev/c (pi)('-) Be interactions. The forward charge is the average difference between the number of positive hadrons and negative hadrons produced in the forward hemisphere. The standard Drell-Yan model predicts that the forward charge should become less negative as the x(,F) of the J/psi increases. The measured forward charge becomes more negative as the x(,F) of the J/psi increases although it is consistent with being flat as a function of x(,F). Hence, the data is not consistent with any Drell-Yan type model which assumes the forward charge is not strongly dependent on the hadronic energy left over after the J/psi is formed.","Made available in DSpace on 2015-05-13T15:41:41Z (GMT). No. of bitstreams: 2 license.txt: 4848 bytes, checksum: 96035ab3f5e1c23cc7138a224ce498bd (MD5) 8409875.PDF: 4910232 bytes, checksum: a51860e81ecf0ec6e9280fd417ace85d (MD5) Previous issue date: 1983","Embargo set by: Seth Robbins for item 78571 Lift date: Forever Reason: Restricted to the U of I community idenfinitely during batch ingest of legacy ETDs","Restricted to the U of I community idenfinitely during batch ingest of legacy ETDs","U of I Only","176 p.","Thesis (Ph.D.)--University of Illinois at Urbana-Champaign, 1983."]},{"key":"dc:title","label":"Title","values":["Forward Charge Distributions Associated With Hadronically Produced J/psi Particles"]}]}],"canonical_facts":{"dc:creator":["Budd, Howard Scott"],"dc:date":["2015-05-13T15:41:41Z","10000-01-01","1983"],"dc:description":["We have measured the forward charge as a function of x(,F) of the psi for events produced by 225 Gev/c (pi)('-) Be interactions. The forward charge is the average difference between the number of positive hadrons and negative hadrons produced in the forward hemisphere. The standard Drell-Yan model predicts that the forward charge should become less negative as the x(,F) of the J/psi increases. The measured forward charge becomes more negative as the x(,F) of the J/psi increases although it is consistent with being flat as a function of x(,F). Hence, the data is not consistent with any Drell-Yan type model which assumes the forward charge is not strongly dependent on the hadronic energy left over after the J/psi is formed.","Made available in DSpace on 2015-05-13T15:41:41Z (GMT). No. of bitstreams: 2 license.txt: 4848 bytes, checksum: 96035ab3f5e1c23cc7138a224ce498bd (MD5) 8409875.PDF: 4910232 bytes, checksum: a51860e81ecf0ec6e9280fd417ace85d (MD5) Previous issue date: 1983","Embargo set by: Seth Robbins for item 78571 Lift date: Forever Reason: Restricted to the U of I community idenfinitely during batch ingest of legacy ETDs","Restricted to the U of I community idenfinitely during batch ingest of legacy ETDs","U of I Only","176 p.","Thesis (Ph.D.)--University of Illinois at Urbana-Champaign, 1983."],"dc:identifier":["http://hdl.handle.net/2142/77360","(UMI)AAI8409875"],"dc:language":["eng"],"dc:subject":["Physics, Elementary Particles and High Energy"],"dc:title":["Forward Charge Distributions Associated With Hadronically Produced J/psi Particles"],"dc:type":["text"],"thesis:degree_discipline":["Physics"],"thesis:degree_level":["Dissertation"],"thesis:degree_name":["Ph.D."],"thesis:institution_name":["University of Illinois at Urbana-Champaign"]},"updated_at":"2026-07-22T22:26:10Z"}