{"id":{"repo_id":"uiuc","oai_identifier":"oai:www.ideals.illinois.edu:2142/23980"},"canonical_url":"https://search.dev.ndltd.org/etd/uiuc/oai:www.ideals.illinois.edu:2142/23980","repository":{"repo_id":"uiuc","name":"University of Illinois - Urbana-Champaign","base_url":"https://www.ideals.illinois.edu/oai-pmh"},"display":{"title":"Bound states in a system of two vector mesons","abstract":"\"We propose that p-exchange gives the major contribution to the forces between two p-mesons. Using dispersion relations techniques, we look for s-wave bound states between two such particles. vIe find three bound states in the 1.2 BeV region. These have the IJ PG assignments: 02++, 11++ and 00'1-+, \\ve identify the f and the B .. resonances with the first Bnd the second of these states. There are no known resonances corresponding to the third state. Next, lilB extend the above mechanism to the octet of vector mesons. t-Je require invariance under SU 3 and G, the charge pad. ty operator. Again there flre bound states in the energy region cited above. these have the following quantum numbers: ~. ,+ 2 (8 or 1)1 1 (8 1 ) and 0+(8 or 1). The numbers in parenthesis refer to the dimension of the corresponding irreducible representAtion of SU3 • vIe assign the f and the A2 to the 2+ octet, the 13 and the Kc to the 1+ octet. For the rest. there is 1.\"\"10 eXperimental evidence yet.\"","abstract_html":"&quot;We propose that p-exchange gives the major contribution to the forces between two p-mesons. Using dispersion relations techniques, we look for s-wave bound states between two such particles. vIe find three bound states in the 1.2 BeV region. These have the IJ PG assignments: 02++, 11++ and 00&#x27;1-+, \\ve identify the f and the B .. resonances with the first Bnd the second of these states. There are no known resonances corresponding to the third state. Next, lilB extend the above mechanism to the octet of vector mesons. t-Je require invariance under SU 3 and G, the charge pad. ty operator. Again there flre bound states in the energy region cited above. these have the following quantum numbers: ~. ,+ 2 (8 or 1)1 1 (8 1 ) and 0+(8 or 1). The numbers in parenthesis refer to the dimension of the corresponding irreducible representAtion of SU3 • vIe assign the f and the A2 to the 2+ octet, the 13 and the Kc to the 1+ octet. For the rest. there is 1.&quot;&quot;10 eXperimental evidence yet.&quot;","abstract_has_math":false,"creators":["Saffouri, Mohammad Hussein"],"institution":null,"degree_name":"Ph.D.","degree_level":"Dissertation","degree_discipline":"Physics","degree_department":null,"school":null,"contributors":["Nishijima, K."],"advisors":[],"committee_chairs":[],"committee_members":[],"year":2011,"date_issued":"2011-05-20T15:17:31Z","date_published":"2011-05-20T15:17:31Z","updated_at":"2026-07-22T22:25:23Z","subjects":["bound states","two vector mesons systems","p-exchange","dispersion relations","s-wave bound states"],"languages":["en"],"rights":["1965 Mohammad Hussein Saffouri"],"rights_urls":[],"identifier_entries":[{"key":"dc:identifier","label":"Identifier","values":["6187559"],"render_values":[{"text":"6187559","href":null,"code":true}]}]},"links":{"outbound_url":"http://hdl.handle.net/2142/23980","outbound_label":"Handle","outbound_source":"dc:identifier"},"metadata_groups":[{"id":"people","label":"People","entries":[{"key":"dc:contributor","label":"Contributor","values":["Nishijima, K."]},{"key":"dc:creator","label":"Author","values":["Saffouri, Mohammad Hussein"]}]},{"id":"academic_context","label":"Academic Context","entries":[{"key":"dc:date","label":"Dc Date","values":["2011-05-20T15:17:31Z","10000-01-01","1965"]},{"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":["bound states","two vector mesons systems","p-exchange","dispersion relations","s-wave bound states"]}]},{"id":"language_rights","label":"Language and Rights","entries":[{"key":"dc:language","label":"Dc Language","values":["en"]},{"key":"dc:rights","label":"Dc Rights","values":["1965 Mohammad Hussein Saffouri"]}]},{"id":"identifiers","label":"Identifiers","entries":[{"key":"dc:identifier","label":"Identifier","values":["6187559","http://hdl.handle.net/2142/23980"]}]},{"id":"additional","label":"Additional Metadata","entries":[{"key":"dc:description","label":"Description","values":["\"We propose that p-exchange gives the major contribution to the forces between two p-mesons. Using dispersion relations techniques, we look for s-wave bound states between two such particles. vIe find three bound states in the 1.2 BeV region. These have the IJ PG assignments: 02++, 11++ and 00'1-+, \\ve identify the f and the B .. resonances with the first Bnd the second of these states. There are no known resonances corresponding to the third state. Next, lilB extend the above mechanism to the octet of vector mesons. t-Je require invariance under SU 3 and G, the charge pad. ty operator. Again there flre bound states in the energy region cited above. these have the following quantum numbers: ~. ,+ 2 (8 or 1)1 1 (8 1 ) and 0+(8 or 1). The numbers in parenthesis refer to the dimension of the corresponding irreducible representAtion of SU3 • vIe assign the f and the A2 to the 2+ octet, the 13 and the Kc to the 1+ octet. For the rest. there is 1.\"\"10 eXperimental evidence yet.\"","Submitted by Carolyn Mead (cmead2@illinois.edu) on 2011-05-20T15:17:31Z No. of bitstreams: 1 1965_saffouri.pdf: 1364987 bytes, checksum: d3ca6b070cd968cc44ad2aa6658a74a0 (MD5)","Made available in DSpace on 2011-05-20T15:17:31Z (GMT). No. of bitstreams: 1 1965_saffouri.pdf: 1364987 bytes, checksum: d3ca6b070cd968cc44ad2aa6658a74a0 (MD5) Previous issue date: 1965","Item marked as restricted to the 'UIUC Users [automated]' Group (id=2) by Carolyn Mead (cmead2@illinois.edu) on 2011-05-20T15:17:31Z Item is restricted indefinitely.","Restriction data tranferred 2014-07-01T11:12:54-05:00 Original Data Group with Access UIUC Users [automated] Release Date: none Reason: Thesis","Thesis","U of I Only"]},{"key":"dc:title","label":"Title","values":["Bound states in a system of two vector mesons"]}]}],"canonical_facts":{"dc:contributor":["Nishijima, K."],"dc:creator":["Saffouri, Mohammad Hussein"],"dc:date":["2011-05-20T15:17:31Z","10000-01-01","1965"],"dc:description":["\"We propose that p-exchange gives the major contribution to the forces between two p-mesons. Using dispersion relations techniques, we look for s-wave bound states between two such particles. vIe find three bound states in the 1.2 BeV region. These have the IJ PG assignments: 02++, 11++ and 00'1-+, \\ve identify the f and the B .. resonances with the first Bnd the second of these states. There are no known resonances corresponding to the third state. Next, lilB extend the above mechanism to the octet of vector mesons. t-Je require invariance under SU 3 and G, the charge pad. ty operator. Again there flre bound states in the energy region cited above. these have the following quantum numbers: ~. ,+ 2 (8 or 1)1 1 (8 1 ) and 0+(8 or 1). The numbers in parenthesis refer to the dimension of the corresponding irreducible representAtion of SU3 • vIe assign the f and the A2 to the 2+ octet, the 13 and the Kc to the 1+ octet. For the rest. there is 1.\"\"10 eXperimental evidence yet.\"","Submitted by Carolyn Mead (cmead2@illinois.edu) on 2011-05-20T15:17:31Z No. of bitstreams: 1 1965_saffouri.pdf: 1364987 bytes, checksum: d3ca6b070cd968cc44ad2aa6658a74a0 (MD5)","Made available in DSpace on 2011-05-20T15:17:31Z (GMT). No. of bitstreams: 1 1965_saffouri.pdf: 1364987 bytes, checksum: d3ca6b070cd968cc44ad2aa6658a74a0 (MD5) Previous issue date: 1965","Item marked as restricted to the 'UIUC Users [automated]' Group (id=2) by Carolyn Mead (cmead2@illinois.edu) on 2011-05-20T15:17:31Z Item is restricted indefinitely.","Restriction data tranferred 2014-07-01T11:12:54-05:00 Original Data Group with Access UIUC Users [automated] Release Date: none Reason: Thesis","Thesis","U of I Only"],"dc:identifier":["6187559","http://hdl.handle.net/2142/23980"],"dc:language":["en"],"dc:rights":["1965 Mohammad Hussein Saffouri"],"dc:subject":["bound states","two vector mesons systems","p-exchange","dispersion relations","s-wave bound states"],"dc:title":["Bound states in a system of two vector mesons"],"dc:type":["Dissertation / Thesis","text"],"thesis:degree_discipline":["Physics"],"thesis:degree_level":["Dissertation"],"thesis:degree_name":["Ph.D."]},"updated_at":"2026-07-22T22:25:23Z"}