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	<title>A Semi-Classical Theory of Baryon Structure - Revision history</title>
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&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Infobox paper&lt;br /&gt;
| title = A Semi-Classical Theory of Baryon Structure&lt;br /&gt;
| author = [[]]&lt;br /&gt;
| keywords = [[half-spin particle model]], [[Bohr-Sommerfeld model]], [[heavy baryon masses]], [[neutron magnetic moment]], [[proton radius]]&lt;br /&gt;
| published = 1988&lt;br /&gt;
| journal = [[Physics Essays]]&lt;br /&gt;
| volume = [[1]]&lt;br /&gt;
| number = [[2]]&lt;br /&gt;
| pages = 109-120&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
==Abstract==&lt;br /&gt;
&lt;br /&gt;
A&amp;lt;sup&amp;gt;&amp;lt;span style=&amp;quot;FONT-SIZE: x-small&amp;quot;&amp;gt;&amp;amp;nbsp;&amp;lt;/span&amp;gt;&amp;lt;/sup&amp;gt;theory of elementary particle structure is presented that has been&amp;lt;sup&amp;gt;&amp;lt;span style=&amp;quot;FONT-SIZE: x-small&amp;quot;&amp;gt;&amp;amp;nbsp;&amp;lt;/span&amp;gt;&amp;lt;/sup&amp;gt;built around a physical model analogous to the Bohr-Sommerfeld atomic&amp;lt;sup&amp;gt;&amp;lt;span style=&amp;quot;FONT-SIZE: x-small&amp;quot;&amp;gt;&amp;amp;nbsp;&amp;lt;/span&amp;gt;&amp;lt;/sup&amp;gt;model. The first installment of the theory has been published&amp;lt;sup&amp;gt;&amp;lt;span style=&amp;quot;FONT-SIZE: x-small&amp;quot;&amp;gt;&amp;amp;nbsp;&amp;lt;/span&amp;gt;&amp;lt;/sup&amp;gt;in a previous paper [L. Bess and L. Chandler, Prog.&amp;lt;sup&amp;gt;&amp;lt;span style=&amp;quot;FONT-SIZE: x-small&amp;quot;&amp;gt;&amp;amp;nbsp;&amp;lt;/span&amp;gt;&amp;lt;/sup&amp;gt;Theor. Phys. &amp;lt;b&amp;gt;46&amp;lt;/b&amp;gt;, 235(1971)]. In the present work, the theory&amp;lt;sup&amp;gt;&amp;lt;span style=&amp;quot;FONT-SIZE: x-small&amp;quot;&amp;gt;&amp;amp;nbsp;&amp;lt;/span&amp;gt;&amp;lt;/sup&amp;gt;is extended to deal with all the known half-spin particles.&amp;lt;sup&amp;gt;&amp;lt;span style=&amp;quot;FONT-SIZE: x-small&amp;quot;&amp;gt;&amp;amp;nbsp;&amp;lt;/span&amp;gt;&amp;lt;/sup&amp;gt;The main new result of the extended theory is the&amp;lt;sup&amp;gt;&amp;lt;span style=&amp;quot;FONT-SIZE: x-small&amp;quot;&amp;gt;&amp;amp;nbsp;&amp;lt;/span&amp;gt;&amp;lt;/sup&amp;gt;calculation of seven associated physical parameters that compare well with&amp;lt;sup&amp;gt;&amp;lt;span style=&amp;quot;FONT-SIZE: x-small&amp;quot;&amp;gt;&amp;amp;nbsp;&amp;lt;/span&amp;gt;&amp;lt;/sup&amp;gt;their experimentally measured counterparts. These include the neutron magnetic moment&amp;lt;sup&amp;gt;&amp;lt;span style=&amp;quot;FONT-SIZE: x-small&amp;quot;&amp;gt;&amp;amp;nbsp;&amp;lt;/span&amp;gt;&amp;lt;/sup&amp;gt;and the masses of the six heaviest baryons.&lt;br /&gt;
&lt;br /&gt;
[[Category:Scientific Paper|semi-classical theory baryon structure]]&lt;/div&gt;</summary>
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