{"id":666,"date":"2012-07-04T05:23:41","date_gmt":"2012-07-04T10:23:41","guid":{"rendered":"http:\/\/www.journal-of-nuclear-physics.com\/?p=666"},"modified":"2012-07-04T05:26:20","modified_gmt":"2012-07-04T10:26:20","slug":"integral-charge-3-quark-bound-system-with-binding-energy","status":"publish","type":"post","link":"https:\/\/www.journal-of-nuclear-physics.com\/?p=666","title":{"rendered":"Integral charge 3 quark bound system with binding energy"},"content":{"rendered":"

by
\nU.V.S. Seshavatharam
\nDIP QA Engineer, Lanco Industries Ltd, Srikalahasti-517641, A.P, India
\nE-mail: seshavatharam.uvs@gmail.com<\/em><\/p>\n

Prof. S. LAKSHMINARAYANA<\/em><\/div>\n
Department Of Nuclear Physics, Andhra University, Vizag-530003, AP, India.<\/em><\/div>\n
E-mail: lnsrirama@yahoo.com<\/em><\/div>\n

\n<\/em><\/div>\n
\n
Read the whole article<\/a><\/div>\n
Download the ZIP file<\/a><\/div>\n<\/div>\n
<\/div>\n

\nAbstract
\n<\/strong>In the previous paper [1] it is suggested that there exists integral charge effective quark fermi-gluons and quark boso-gluons.<\/span><\/div>\n
\n
Effective quark fermi-gluons generates charged ground state baryons and quark boso-gluons generates ground state neutral mesons.<\/div>\n
In this paper it is suggested that with a binding energy of 939 MeV any 3 (effective) quark fermi-gluons couples together to form a charged ground state baryon.<\/div>\n
Square root of any 2 quark fermi-gluons or cubic root of any 3 quark fermi-gluons can be called as `hybrid’ quark fermi-gluons.<\/div>\n
Hybrid quark fermi-gluons of up and down are 746 MeV, 779 MeV and 813 MeV. Out of 6 quark fermi-gluons, for a three quark bound system (with binding energy 939 MeV) different combinations of quark fermi-gluons and hybrid quark fermi-gluons can be possible and hence different ground state baryons can be generated with different quark flavors.<\/div>\n
If n=1, 2, 3,.. excited energy levels follows<\/div>\n
\n

\"\"<\/p>\n

X sum of 3 quark fermi-gluons rest energy.<\/div>\n
Another interesting thing is that light quark bosons like up boson mass=1.94 MeV and down boson mass=4.2 MeV couples with these ground or excited states to form doublets and triplets.<\/div>\n
3 up quark fermi-gluons having rest energy 3×685 MeV and binding energy 939 MeV generates a ground state charged baryon of rest energy (3×685)-939\u22481116MeV<\/em>.
\nUp boson mass =1.94 MeV couples with this charged state and generates a neutral baryon at 1118 MeV.
\nTwo up and one down quark fermi-gluons having binding energy 939 MeV generates charged (2×685+885)-939\u22481316MeV<\/em> .
\nOne up and two down quark fermi-gluons having binding enegy 939 MeV generates charged (685+2×885)-939 1516MeV<\/em>.
\nThus 1177 MeV and 1377 MeV ground state charged baryons can be generated.
\nThis idea can be applied to other heavy quark fermi-gluons.<\/div>\n<\/div>\n<\/div>\n

Read the whole article<\/a>
\nDownload the ZIP file<\/a><\/p>\n","protected":false},"excerpt":{"rendered":"

by U.V.S. Seshavatharam DIP QA Engineer, Lanco Industries Ltd, Srikalahasti-517641, A.P, India E-mail: seshavatharam.uvs@gmail.com<\/p>\n

Prof. S. LAKSHMINARAYANA Department Of Nuclear Physics, Andhra University, Vizag-530003, AP, India. E-mail: lnsrirama@yahoo.com Read the whole article Download the ZIP file Abstract In the previous paper [1] it is suggested that there exists integral charge effective quark fermi-gluons […]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":[],"categories":[3],"tags":[],"_links":{"self":[{"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=\/wp\/v2\/posts\/666"}],"collection":[{"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=666"}],"version-history":[{"count":11,"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=\/wp\/v2\/posts\/666\/revisions"}],"predecessor-version":[{"id":677,"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=\/wp\/v2\/posts\/666\/revisions\/677"}],"wp:attachment":[{"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=666"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=666"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=666"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}