{"id":{"repo_id":"uiuc","oai_identifier":"oai:www.ideals.illinois.edu:2142/25677"},"canonical_url":"https://search.dev.ndltd.org/etd/uiuc/oai:www.ideals.illinois.edu:2142/25677","repository":{"repo_id":"uiuc","name":"University of Illinois - Urbana-Champaign","base_url":"https://www.ideals.illinois.edu/oai-pmh"},"display":{"title":"Three pion production on complex nuclei at 23 GeV/c","abstract":"An analysis of three pion production data at 23 GeV/c is described; these reactions are of the form pi- -> pi+pi-pi-A where A is one of the nuclear targets: carbon, aluminum, copper, silver, or lead. Total and differential cross-sections are quoted, and the method of their computation is outlined. The spin-parity composition of the three-pion system has been analyzed using the Illinois method of partial wave analysis. The partial wave structure of the data is remarkably similar to that of the data from hydrogen, excepting the distributions in momentum transfer, which exhibit the usual coherent and incoherent contributions of nuclear scattering. The partial~wave results have been fitted with an optical model for three-pion production, with very good results. With this model the absorptions of the three-pion system (in nuclear matter) turn out to be roughly equal to that of a single pion, 25 millibarns, except for the JP = 0-component of the production, which is roughly 50 millibarns. In particular, the A2 (JP = 2+, mass = 1310 MeV) is coherently produced, with an absorption of roughly 25 millibarns.","abstract_html":"An analysis of three pion production data at 23 GeV/c is described; these reactions are of the form pi- -> pi+pi-pi-A where A is one of the nuclear targets: carbon, aluminum, copper, silver, or lead. Total and differential cross-sections are quoted, and the method of their computation is outlined. The spin-parity composition of the three-pion system has been analyzed using the Illinois method of partial wave analysis. The partial wave structure of the data is remarkably similar to that of the data from hydrogen, excepting the distributions in momentum transfer, which exhibit the usual coherent and incoherent contributions of nuclear scattering. The partial~wave results have been fitted with an optical model for three-pion production, with very good results. With this model the absorptions of the three-pion system (in nuclear matter) turn out to be roughly equal to that of a single pion, 25 millibarns, except for the JP = 0-component of the production, which is roughly 50 millibarns. In particular, the A2 (JP = 2+, mass = 1310 MeV) is coherently produced, with an absorption of roughly 25 millibarns.","abstract_has_math":false,"creators":["Roberts, Thomas John"],"institution":null,"degree_name":"Ph.D.","degree_level":"Dissertation","degree_discipline":"Physics","degree_department":null,"school":null,"contributors":["Kruse, U.E."],"advisors":[],"committee_chairs":[],"committee_members":[],"year":2011,"date_issued":"2011-07-06T18:43:00Z","date_published":"2011-07-06T18:43:00Z","updated_at":"2026-07-22T22:25:26Z","subjects":["three pion production","complex nuclei","spin-parity composition"],"languages":["en"],"rights":["1975 Thomas John Roberts"],"rights_urls":[],"identifier_entries":[{"key":"dc:identifier","label":"Identifier","values":["2737502"],"render_values":[{"text":"2737502","href":null,"code":true}]}]},"links":{"outbound_url":"http://hdl.handle.net/2142/25677","outbound_label":"Handle","outbound_source":"dc:identifier"},"metadata_groups":[{"id":"people","label":"People","entries":[{"key":"dc:contributor","label":"Contributor","values":["Kruse, U.E."]},{"key":"dc:creator","label":"Author","values":["Roberts, Thomas John"]}]},{"id":"academic_context","label":"Academic Context","entries":[{"key":"dc:date","label":"Dc Date","values":["2011-07-06T18:43:00Z","10000-01-01","1975"]},{"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":["three pion production","complex nuclei","spin-parity composition"]}]},{"id":"language_rights","label":"Language and Rights","entries":[{"key":"dc:language","label":"Dc Language","values":["en"]},{"key":"dc:rights","label":"Dc Rights","values":["1975 Thomas John Roberts"]}]},{"id":"identifiers","label":"Identifiers","entries":[{"key":"dc:identifier","label":"Identifier","values":["2737502","http://hdl.handle.net/2142/25677"]}]},{"id":"additional","label":"Additional Metadata","entries":[{"key":"dc:description","label":"Description","values":["An analysis of three pion production data at 23 GeV/c is described; these reactions are of the form pi- -> pi+pi-pi-A where A is one of the nuclear targets: carbon, aluminum, copper, silver, or lead. Total and differential cross-sections are quoted, and the method of their computation is outlined. The spin-parity composition of the three-pion system has been analyzed using the Illinois method of partial wave analysis. The partial wave structure of the data is remarkably similar to that of the data from hydrogen, excepting the distributions in momentum transfer, which exhibit the usual coherent and incoherent contributions of nuclear scattering. The partial~wave results have been fitted with an optical model for three-pion production, with very good results. With this model the absorptions of the three-pion system (in nuclear matter) turn out to be roughly equal to that of a single pion, 25 millibarns, except for the JP = 0-component of the production, which is roughly 50 millibarns. In particular, the A2 (JP = 2+, mass = 1310 MeV) is coherently produced, with an absorption of roughly 25 millibarns.","Submitted by Carolyn Mead (cmead2@illinois.edu) on 2011-07-06T18:43:00Z No. of bitstreams: 1 1975_roberts.pdf: 3882257 bytes, checksum: f6f7e63e549516bc9b2cc47d725adbf5 (MD5)","Made available in DSpace on 2011-07-06T18:43:00Z (GMT). No. of bitstreams: 1 1975_roberts.pdf: 3882257 bytes, checksum: f6f7e63e549516bc9b2cc47d725adbf5 (MD5) Previous issue date: 1975","Item marked as restricted to the 'UIUC Users [automated]' Group (id=2) by Carolyn Mead (cmead2@illinois.edu) on 2011-07-06T18:43:00Z Item is restricted indefinitely.","Restriction data tranferred 2014-07-01T11:32:34-05:00 Original Data Group with Access UIUC Users [automated] Release Date: none Reason: Thesis","Thesis","U of I Only"]},{"key":"dc:title","label":"Title","values":["Three pion production on complex nuclei at 23 GeV/c"]}]}],"canonical_facts":{"dc:contributor":["Kruse, U.E."],"dc:creator":["Roberts, Thomas John"],"dc:date":["2011-07-06T18:43:00Z","10000-01-01","1975"],"dc:description":["An analysis of three pion production data at 23 GeV/c is described; these reactions are of the form pi- -> pi+pi-pi-A where A is one of the nuclear targets: carbon, aluminum, copper, silver, or lead. Total and differential cross-sections are quoted, and the method of their computation is outlined. The spin-parity composition of the three-pion system has been analyzed using the Illinois method of partial wave analysis. The partial wave structure of the data is remarkably similar to that of the data from hydrogen, excepting the distributions in momentum transfer, which exhibit the usual coherent and incoherent contributions of nuclear scattering. The partial~wave results have been fitted with an optical model for three-pion production, with very good results. With this model the absorptions of the three-pion system (in nuclear matter) turn out to be roughly equal to that of a single pion, 25 millibarns, except for the JP = 0-component of the production, which is roughly 50 millibarns. In particular, the A2 (JP = 2+, mass = 1310 MeV) is coherently produced, with an absorption of roughly 25 millibarns.","Submitted by Carolyn Mead (cmead2@illinois.edu) on 2011-07-06T18:43:00Z No. of bitstreams: 1 1975_roberts.pdf: 3882257 bytes, checksum: f6f7e63e549516bc9b2cc47d725adbf5 (MD5)","Made available in DSpace on 2011-07-06T18:43:00Z (GMT). No. of bitstreams: 1 1975_roberts.pdf: 3882257 bytes, checksum: f6f7e63e549516bc9b2cc47d725adbf5 (MD5) Previous issue date: 1975","Item marked as restricted to the 'UIUC Users [automated]' Group (id=2) by Carolyn Mead (cmead2@illinois.edu) on 2011-07-06T18:43:00Z Item is restricted indefinitely.","Restriction data tranferred 2014-07-01T11:32:34-05:00 Original Data Group with Access UIUC Users [automated] Release Date: none Reason: Thesis","Thesis","U of I Only"],"dc:identifier":["2737502","http://hdl.handle.net/2142/25677"],"dc:language":["en"],"dc:rights":["1975 Thomas John Roberts"],"dc:subject":["three pion production","complex nuclei","spin-parity composition"],"dc:title":["Three pion production on complex nuclei at 23 GeV/c"],"dc:type":["Dissertation / Thesis","text"],"thesis:degree_discipline":["Physics"],"thesis:degree_level":["Dissertation"],"thesis:degree_name":["Ph.D."]},"updated_at":"2026-07-22T22:25:26Z"}