{"id":9583,"date":"1997-11-22T18:25:00","date_gmt":"1997-11-22T16:25:00","guid":{"rendered":"https:\/\/www.jassemajaka.com\/?p=9583"},"modified":"2019-02-22T19:19:35","modified_gmt":"2019-02-22T17:19:35","slug":"%ce%b7-meson-photoproduction-dynamics-and-missing-resonances","status":"publish","type":"post","link":"https:\/\/www.jassemajaka.com\/?p=9583","title":{"rendered":"Eta-meson photoproduction Dynamics and Missing Resonances"},"content":{"rendered":"<div class=\"hlFld-Title articleMeta padded-content\">\n<header class=\"publicationContentTitle\">\n<h3 dir=\"ltr\">Eta-meson photoproduction dynamics and missing resonances<\/h3>\n<\/header>\n<\/div>\n<div class=\"articleMetaDrop publicationContentDropZone\" dir=\"ltr\" data-pb-dropzone=\"articleMetaDropZone\"><\/div>\n<div class=\"publicationContentCitation\" dir=\"ltr\">AIP Conference Proceedings <b>412<\/b>, 567 (1997); <a href=\"https:\/\/doi.org\/10.1063\/1.54349\">https:\/\/doi.org\/10.1063\/1.54349<\/a><\/div>\n<div class=\"publicationContentAuthors padded-content\" dir=\"ltr\">\n<div class=\"hlFld-ContribAuthor\">\n<div class=\"entryAuthor\" aria-label=\"authors\"><span class=\"contrib-author\"> B. Saghai<i class=\"pubContent-comma\">, <\/i><\/span><span class=\"contrib-author\"> F. Tabakin<i class=\"pubContent-comma\">, <\/i><\/span><span class=\"contrib-author\"> J. Ajaka<i class=\"pubContent-comma\">, and <\/i><\/span><span class=\"contrib-author\"> P. Hoffmann-Rothe<\/span><\/div>\n<\/div>\n<\/div>\n<div class=\"sectionInfo abstractSectionHeading\" dir=\"ltr\">\n<div id=\"fragmentNav_0\" class=\"sectionHeading\">Abstract<\/div>\n<\/div>\n<div class=\"NLM_paragraph\" dir=\"ltr\">The general nodal structure approach is applied to the recent <span class=\"equationTd inline-formula\"><span id=\"MathJax-Element-1-Frame\" class=\"MathJax\" tabindex=\"0\" role=\"presentation\" data-mathml=\"&lt;math xmlns=&quot;http:\/\/www.w3.org\/1998\/Math\/MathML&quot; overflow=&quot;scroll&quot; altimg=&quot;eq-00001.gif&quot;&gt;&lt;mi&gt;&amp;#x3B3;p&amp;#x20D7;&amp;#x2192;&amp;#x3B7;p&lt;\/mi&gt;&lt;\/math&gt;\"><span id=\"MathJax-Span-1\" class=\"math\"><span id=\"MathJax-Span-2\" class=\"mrow\"><span id=\"MathJax-Span-3\" class=\"mi\">\u03b3p\u20d7\u2192\u03b7p <\/span><\/span><\/span><\/span><\/span><span class=\"equationTd inline-formula\"><span id=\"MathJax-Element-2-Frame\" class=\"MathJax\" tabindex=\"0\" role=\"presentation\" data-mathml=\"&lt;math xmlns=&quot;http:\/\/www.w3.org\/1998\/Math\/MathML&quot; overflow=&quot;scroll&quot; altimg=&quot;eq-00002.gif&quot;&gt;&lt;mi mathvariant=&quot;normal&quot;&gt;T&lt;\/mi&gt;&lt;\/math&gt;\"><span id=\"MathJax-Span-4\" class=\"math\"><span id=\"MathJax-Span-5\" class=\"mrow\"><span id=\"MathJax-Span-6\" class=\"mi\">T<\/span><\/span><\/span><\/span><\/span>-asymmetry data from ELSA. The reaction mechanism is found to require, in addition to the dominant <span class=\"equationTd inline-formula\"><span id=\"MathJax-Element-3-Frame\" class=\"MathJax\" tabindex=\"0\" role=\"presentation\" data-mathml=\"&lt;math xmlns=&quot;http:\/\/www.w3.org\/1998\/Math\/MathML&quot; overflow=&quot;scroll&quot; altimg=&quot;eq-00003.gif&quot;&gt;&lt;msub&gt;&lt;mi&gt;S&lt;\/mi&gt;&lt;mrow&gt;&lt;mn&gt;11&lt;\/mn&gt;&lt;\/mrow&gt;&lt;\/msub&gt;&lt;\/math&gt;\"><span id=\"MathJax-Span-7\" class=\"math\"><span id=\"MathJax-Span-8\" class=\"mrow\"><span id=\"MathJax-Span-9\" class=\"msub\"><span id=\"MathJax-Span-10\" class=\"mi\">S<\/span><span id=\"MathJax-Span-11\" class=\"mrow\"><span id=\"MathJax-Span-12\" class=\"mn\">11<\/span><\/span><\/span><\/span><\/span><\/span><\/span> and <span class=\"equationTd inline-formula\"><span id=\"MathJax-Element-4-Frame\" class=\"MathJax\" tabindex=\"0\" role=\"presentation\" data-mathml=\"&lt;math xmlns=&quot;http:\/\/www.w3.org\/1998\/Math\/MathML&quot; overflow=&quot;scroll&quot; altimg=&quot;eq-00004.gif&quot;&gt;&lt;msub&gt;&lt;mi&gt;D&lt;\/mi&gt;&lt;mrow&gt;&lt;mn&gt;13&lt;\/mn&gt;&lt;\/mrow&gt;&lt;\/msub&gt;&lt;\/math&gt;\"><span id=\"MathJax-Span-13\" class=\"math\"><span id=\"MathJax-Span-14\" class=\"mrow\"><span id=\"MathJax-Span-15\" class=\"msub\"><span id=\"MathJax-Span-16\" class=\"mi\">D<\/span><span id=\"MathJax-Span-17\" class=\"mrow\"><span id=\"MathJax-Span-18\" class=\"mn\">13<\/span><\/span><\/span><\/span><\/span><\/span><\/span> resonances, contributions from <span class=\"equationTd inline-formula\"><span id=\"MathJax-Element-5-Frame\" class=\"MathJax\" tabindex=\"0\" role=\"presentation\" data-mathml=\"&lt;math xmlns=&quot;http:\/\/www.w3.org\/1998\/Math\/MathML&quot; overflow=&quot;scroll&quot; altimg=&quot;eq-00005.gif&quot;&gt;&lt;msub&gt;&lt;mi&gt;P&lt;\/mi&gt;&lt;mrow&gt;&lt;mn&gt;13&lt;\/mn&gt;&lt;\/mrow&gt;&lt;\/msub&gt;&lt;\/math&gt;\"><span id=\"MathJax-Span-19\" class=\"math\"><span id=\"MathJax-Span-20\" class=\"mrow\"><span id=\"MathJax-Span-21\" class=\"msub\"><span id=\"MathJax-Span-22\" class=\"mi\">P<\/span><span id=\"MathJax-Span-23\" class=\"mrow\"><span id=\"MathJax-Span-24\" class=\"mn\">13<\/span><\/span><\/span><\/span><\/span><\/span><\/span> and <span class=\"equationTd inline-formula\"><span id=\"MathJax-Element-6-Frame\" class=\"MathJax\" tabindex=\"0\" role=\"presentation\" data-mathml=\"&lt;math xmlns=&quot;http:\/\/www.w3.org\/1998\/Math\/MathML&quot; overflow=&quot;scroll&quot; altimg=&quot;eq-00006.gif&quot;&gt;&lt;msub&gt;&lt;mi&gt;D&lt;\/mi&gt;&lt;mrow&gt;&lt;mn&gt;15&lt;\/mn&gt;&lt;\/mrow&gt;&lt;\/msub&gt;&lt;\/math&gt;\"><span id=\"MathJax-Span-25\" class=\"math\"><span id=\"MathJax-Span-26\" class=\"mrow\"><span id=\"MathJax-Span-27\" class=\"msub\"><span id=\"MathJax-Span-28\" class=\"mi\">D<\/span><span id=\"MathJax-Span-29\" class=\"mrow\"><span id=\"MathJax-Span-30\" class=\"mn\">15<\/span><\/span><\/span><\/span><\/span><\/span><\/span> resonances. This finding is confirmed within a simple dynamical approach. An indication on the presence of a predicted <span class=\"equationTd inline-formula\"><span id=\"MathJax-Element-7-Frame\" class=\"MathJax\" tabindex=\"0\" role=\"presentation\" data-mathml=\"&lt;math xmlns=&quot;http:\/\/www.w3.org\/1998\/Math\/MathML&quot; overflow=&quot;scroll&quot; altimg=&quot;eq-00007.gif&quot;&gt;&lt;msub&gt;&lt;mi&gt;P&lt;\/mi&gt;&lt;mrow&gt;&lt;mn&gt;13&lt;\/mn&gt;&lt;\/mrow&gt;&lt;\/msub&gt;&lt;\/math&gt;\"><span id=\"MathJax-Span-31\" class=\"math\"><span id=\"MathJax-Span-32\" class=\"mrow\"><span id=\"MathJax-Span-33\" class=\"msub\"><span id=\"MathJax-Span-34\" class=\"mi\">P<\/span><span id=\"MathJax-Span-35\" class=\"mrow\"><span id=\"MathJax-Span-36\" class=\"mn\">13<\/span><\/span><\/span><\/span><\/span><\/span><\/span> nucleonic resonance is observed.<\/div>\n<p dir=\"ltr\">Download the pdf: <a href=\"https:\/\/www.jassemajaka.com\/wp-content\/uploads\/2019\/02\/etames.pdf\">etames<\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>The general nodal structure approach is applied to the recent \u03b3p\u20d7\u2192\u03b7p T-asymmetry data from ELSA. The reaction mechanism is found to require, in addition to the dominant S11 and D13 resonances, contributions from P13 and D15 resonances. This finding is confirmed within a simple dynamical approach. An indication on the presence of a predicted P13 nucleonic resonance is observed.<\/p>\n","protected":false},"author":12,"featured_media":9585,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"jetpack_post_was_ever_published":false,"_jetpack_newsletter_access":"","_jetpack_dont_email_post_to_subs":false,"_jetpack_newsletter_tier_id":0,"_jetpack_memberships_contains_paywalled_content":false,"_jetpack_memberships_contains_paid_content":false,"footnotes":""},"categories":[50],"tags":[942,949,946,788,791,790,679,943,947,881,948,676,945],"class_list":["post-9583","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-50","tag-american-institute-of-physics","tag-d15","tag-elsa","tag-eta-meson","tag-eta-photoproduction","tag-hadronic-physics","tag-jassem-ajaka","tag-missing-resonances","tag-nodal-structure","tag-nucleon-resonance","tag-p13","tag-scientific-article","tag-t-asymmetry"],"jetpack_featured_media_url":"https:\/\/www.jassemajaka.com\/wp-content\/uploads\/2019\/02\/eta.png","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/paTyQg-2uz","_links":{"self":[{"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=\/wp\/v2\/posts\/9583","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=\/wp\/v2\/users\/12"}],"replies":[{"embeddable":true,"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=9583"}],"version-history":[{"count":3,"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=\/wp\/v2\/posts\/9583\/revisions"}],"predecessor-version":[{"id":9591,"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=\/wp\/v2\/posts\/9583\/revisions\/9591"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=\/wp\/v2\/media\/9585"}],"wp:attachment":[{"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=9583"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=9583"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=9583"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}