{"id":776,"date":"2013-01-07T10:08:53","date_gmt":"2013-01-07T15:08:53","guid":{"rendered":"http:\/\/www.journal-of-nuclear-physics.com\/?p=776"},"modified":"2013-01-07T12:52:26","modified_gmt":"2013-01-07T17:52:26","slug":"formulas-for-magnetic-moments-of-the-proton-and-neutron","status":"publish","type":"post","link":"https:\/\/www.journal-of-nuclear-physics.com\/?p=776","title":{"rendered":"Formulas for Magnetic Moments of the Proton and Neutron"},"content":{"rendered":"
.<\/span><\/div>\n
by<\/em><\/div>\n
Sergey P.Efimov<\/em><\/div>\n
Senior-lecturer, Department of mathematics,<\/em><\/div>\n
Bauman Moscow State Technical University. Moscow. Russia<\/em><\/div>\n
E-mail: serg.efimo2012@yandex.ru<\/em><\/div>\n
.<\/span><\/div>\n
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Short Content<\/strong><\/div>\n
\n
Modern ideas presume that the nucleon has a complex structure. Accordingly, one should not expect simple and exact formulas for the above quantities in future theory. Still, if we suppose that future theory possesses hidden symmetry then there possibly exist simple formulas for the magnetic moments, since in quantum theory, symmetries normally generate comparatively simple formulas involving integer numbers. The hypothesis can be verified by a simple, but not at all obvious, method of numerical analysis of the experimental data.<\/div>\n
Based on it, we find simple phenomenological formulas for the magnetic moments of the proton and neutron with 10 valid digits. We also obtain a compact formula for the relation of the electron\u2019s anomalous moment to the summary magnetic moment of the nucleon with 11 valid digits, and propose dependencies of the neutron and proton masses in electron mass units as functions with argument \u03c0.<\/div>\n
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. by Sergey P.Efimov Senior-lecturer, Department of mathematics, Bauman Moscow State Technical University. Moscow. Russia E-mail: serg.efimo2012@yandex.ru . Read the whole article Download the ZIP file . Short Content Modern ideas presume that the nucleon has a complex structure. Accordingly, one should not expect simple and exact formulas for the above quantities in future theory. […]<\/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\/776"}],"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=776"}],"version-history":[{"count":4,"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=\/wp\/v2\/posts\/776\/revisions"}],"predecessor-version":[{"id":778,"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=\/wp\/v2\/posts\/776\/revisions\/778"}],"wp:attachment":[{"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=776"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=776"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=776"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}