{"id":{"repo_id":"uiuc","oai_identifier":"oai:www.ideals.illinois.edu:2142/77363"},"canonical_url":"https://search.dev.ndltd.org/etd/uiuc/oai:www.ideals.illinois.edu:2142/77363","repository":{"repo_id":"uiuc","name":"University of Illinois - Urbana-Champaign","base_url":"https://www.ideals.illinois.edu/oai-pmh"},"display":{"title":"Exclusive Diffractive Dissociation of K(l) Mesons at High Energies","abstract":"Using the hadronic component of the Fermilab broad band neutral beam, we have observed diffractive dissociation of K(,L) mesons with a carbon target into the exclusive final states Ks (pi)('+)(pi)('-), K*(890)('(+OR-)) (pi)('(-OR+)), Ks (rho)('0), Ks (omega)('0), and Ks (phi), but not Ks (psi). The diffractive production cross section for these states is not strongly dependent on incident energy varying at most by 30 percent between 75 and 150 Gev. The shapes of the mass distributions do not change appreciably as a function of lab energy. The ratio of the diffractive mass threshold production of K*(890)('(+OR-))(pi)('(-OR+)), Ks (rho)('0), Ks (omega)('0) and Ks (phi) is compared with results of two other experiments at lower lab energies with charged kaon beams on a hydrogen target.","abstract_html":"Using the hadronic component of the Fermilab broad band neutral beam, we have observed diffractive dissociation of K(,L) mesons with a carbon target into the exclusive final states Ks (pi)('+)(pi)('-), K*(890)('(+OR-)) (pi)('(-OR+)), Ks (rho)('0), Ks (omega)('0), and Ks (phi), but not Ks (psi). The diffractive production cross section for these states is not strongly dependent on incident energy varying at most by 30 percent between 75 and 150 Gev. The shapes of the mass distributions do not change appreciably as a function of lab energy. The ratio of the diffractive mass threshold production of K*(890)('(+OR-))(pi)('(-OR+)), Ks (rho)('0), Ks (omega)('0) and Ks (phi) is compared with results of two other experiments at lower lab energies with charged kaon beams on a hydrogen target.","abstract_has_math":false,"creators":["Lamm, Michael Joseph"],"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)AAI8409977"],"render_values":[{"text":"(UMI)AAI8409977","href":null,"code":true}]}]},"links":{"outbound_url":"http://hdl.handle.net/2142/77363","outbound_label":"Handle","outbound_source":"dc:identifier"},"metadata_groups":[{"id":"people","label":"People","entries":[{"key":"dc:creator","label":"Author","values":["Lamm, Michael Joseph"]}]},{"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/2142/77363","(UMI)AAI8409977"]}]},{"id":"additional","label":"Additional Metadata","entries":[{"key":"dc:description","label":"Description","values":["Using the hadronic component of the Fermilab broad band neutral beam, we have observed diffractive dissociation of K(,L) mesons with a carbon target into the exclusive final states Ks (pi)('+)(pi)('-), K*(890)('(+OR-)) (pi)('(-OR+)), Ks (rho)('0), Ks (omega)('0), and Ks (phi), but not Ks (psi). The diffractive production cross section for these states is not strongly dependent on incident energy varying at most by 30 percent between 75 and 150 Gev. The shapes of the mass distributions do not change appreciably as a function of lab energy. The ratio of the diffractive mass threshold production of K*(890)('(+OR-))(pi)('(-OR+)), Ks (rho)('0), Ks (omega)('0) and Ks (phi) is compared with results of two other experiments at lower lab energies with charged kaon beams on a hydrogen target.","Made available in DSpace on 2015-05-13T15:41:41Z (GMT). No. of bitstreams: 2 license.txt: 4848 bytes, checksum: 96035ab3f5e1c23cc7138a224ce498bd (MD5) 8409977.PDF: 3452051 bytes, checksum: ac081d1ecface903b8fd89a7944ce3ec (MD5) Previous issue date: 1983","Embargo set by: Seth Robbins for item 78574 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","152 p.","Thesis (Ph.D.)--University of Illinois at Urbana-Champaign, 1983."]},{"key":"dc:title","label":"Title","values":["Exclusive Diffractive Dissociation of K(l) Mesons at High Energies"]}]}],"canonical_facts":{"dc:creator":["Lamm, Michael Joseph"],"dc:date":["2015-05-13T15:41:41Z","10000-01-01","1983"],"dc:description":["Using the hadronic component of the Fermilab broad band neutral beam, we have observed diffractive dissociation of K(,L) mesons with a carbon target into the exclusive final states Ks (pi)('+)(pi)('-), K*(890)('(+OR-)) (pi)('(-OR+)), Ks (rho)('0), Ks (omega)('0), and Ks (phi), but not Ks (psi). The diffractive production cross section for these states is not strongly dependent on incident energy varying at most by 30 percent between 75 and 150 Gev. The shapes of the mass distributions do not change appreciably as a function of lab energy. The ratio of the diffractive mass threshold production of K*(890)('(+OR-))(pi)('(-OR+)), Ks (rho)('0), Ks (omega)('0) and Ks (phi) is compared with results of two other experiments at lower lab energies with charged kaon beams on a hydrogen target.","Made available in DSpace on 2015-05-13T15:41:41Z (GMT). No. of bitstreams: 2 license.txt: 4848 bytes, checksum: 96035ab3f5e1c23cc7138a224ce498bd (MD5) 8409977.PDF: 3452051 bytes, checksum: ac081d1ecface903b8fd89a7944ce3ec (MD5) Previous issue date: 1983","Embargo set by: Seth Robbins for item 78574 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","152 p.","Thesis (Ph.D.)--University of Illinois at Urbana-Champaign, 1983."],"dc:identifier":["http://hdl.handle.net/2142/77363","(UMI)AAI8409977"],"dc:language":["eng"],"dc:subject":["Physics, Elementary Particles and High Energy"],"dc:title":["Exclusive Diffractive Dissociation of K(l) Mesons at High Energies"],"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"}