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	<id>http://naturalphilosophy.org/wiki/index.php?action=history&amp;feed=atom&amp;title=A_Dirac_Equation</id>
	<title>A Dirac Equation - Revision history</title>
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	<updated>2026-04-10T02:01:27Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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	<entry>
		<id>http://naturalphilosophy.org/wiki/index.php?title=A_Dirac_Equation&amp;diff=16388&amp;oldid=prev</id>
		<title>Maintenance script: Imported from text file</title>
		<link rel="alternate" type="text/html" href="http://naturalphilosophy.org/wiki/index.php?title=A_Dirac_Equation&amp;diff=16388&amp;oldid=prev"/>
		<updated>2017-01-01T16:54:47Z</updated>

		<summary type="html">&lt;p&gt;Imported from text file&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 12:54, 1 January 2017&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l7&quot;&gt;Line 7:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 7:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;==Abstract==&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;==Abstract==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The time evolution of electrons and other fermions is described by the first-order Dirac equation.  Although typically interpreted probabilistically, the Dirac equation is fundamentally a deterministic  equation for the evolution of physical observables such as angular momentum density. The Dirac  equation can be considered as a second-order wave equation if the wave function is a representation of  the first derivatives. The conventional Dirac formalism has two serious flaws. First, the conventional  derivation of the parity operator is incorrect. Conventional theory holds that the wave function of a  Dirac particle is its own mirror image but certain mirrored interactions do not occur. Such mirror  particles have never been observed. Experimental evidence, such as beta decay, supports the  alternative hypothesis that the mirror image of matter is antimatter. This problem is solved by  identifying a flaw in the conventional derivation of the parity operator, then deriving a new parity  operator based on the algebraic properties of vectors. Second, the conjugate momenta (p&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;) in the freeparticle  Hamiltonian (H) do not have the proper relation ( p&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; =&amp;amp;#948;H &amp;amp;#948;q&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; ) to the time derivatives of  coordinates ( q&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; ). This problem is solved by replacing the mass term with convection and rotation  terms. We then show that the resultant bispinor equation of evolution is equivalent to a classical  second-order wave equation for angular momentum density in an elastic solid. The co-existence of  forward- and backward-propagating waves along a single axis is the basis of half-integer spin. Wave  interference produces both the Lorenz force and the Pauli Exclusion Principle. Mass is associated with  radially inward acceleration of the wave such as occurs in a soliton. Angular correlations between spin  states are equal to the quantum correlations. Bell?s Theorem is not applicable to classical bispinors.  Matter and anti-matter are related by spatial inversion, consistent with experimental observations. The  classical wave formulation therefore provides a conceptually clear interpretation of fermion dynamics.[[Category:Scientific Paper]]&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The time evolution of electrons and other fermions is described by the first-order Dirac equation.  Although typically interpreted probabilistically, the Dirac equation is fundamentally a deterministic  equation for the evolution of physical observables such as angular momentum density. The Dirac  equation can be considered as a second-order wave equation if the wave function is a representation of  the first derivatives. The conventional Dirac formalism has two serious flaws. First, the conventional  derivation of the parity operator is incorrect. Conventional theory holds that the wave function of a  Dirac particle is its own mirror image but certain mirrored interactions do not occur. Such mirror  particles have never been observed. Experimental evidence, such as beta decay, supports the  alternative hypothesis that the mirror image of matter is antimatter. This problem is solved by  identifying a flaw in the conventional derivation of the parity operator, then deriving a new parity  operator based on the algebraic properties of vectors. Second, the conjugate momenta (p&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;) in the freeparticle  Hamiltonian (H) do not have the proper relation ( p&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; =&amp;amp;#948;H &amp;amp;#948;q&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; ) to the time derivatives of  coordinates ( q&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; ). This problem is solved by replacing the mass term with convection and rotation  terms. We then show that the resultant bispinor equation of evolution is equivalent to a classical  second-order wave equation for angular momentum density in an elastic solid. The co-existence of  forward- and backward-propagating waves along a single axis is the basis of half-integer spin. Wave  interference produces both the Lorenz force and the Pauli Exclusion Principle. Mass is associated with  radially inward acceleration of the wave such as occurs in a soliton. Angular correlations between spin  states are equal to the quantum correlations. Bell?s Theorem is not applicable to classical bispinors.  Matter and anti-matter are related by spatial inversion, consistent with experimental observations. The  classical wave formulation therefore provides a conceptually clear interpretation of fermion dynamics.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;[[Category:Scientific Paper&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;|dirac equation&lt;/ins&gt;]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
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		<author><name>Maintenance script</name></author>
	</entry>
	<entry>
		<id>http://naturalphilosophy.org/wiki/index.php?title=A_Dirac_Equation&amp;diff=9211&amp;oldid=prev</id>
		<title>Maintenance script: Imported from text file</title>
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		<updated>2016-12-30T17:21:06Z</updated>

		<summary type="html">&lt;p&gt;Imported from text file&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Infobox paper&lt;br /&gt;
| title = A Dirac Equation&lt;br /&gt;
| author = [[Robert A Close]]&lt;br /&gt;
| published = 2008&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
==Abstract==&lt;br /&gt;
&lt;br /&gt;
The time evolution of electrons and other fermions is described by the first-order Dirac equation.  Although typically interpreted probabilistically, the Dirac equation is fundamentally a deterministic  equation for the evolution of physical observables such as angular momentum density. The Dirac  equation can be considered as a second-order wave equation if the wave function is a representation of  the first derivatives. The conventional Dirac formalism has two serious flaws. First, the conventional  derivation of the parity operator is incorrect. Conventional theory holds that the wave function of a  Dirac particle is its own mirror image but certain mirrored interactions do not occur. Such mirror  particles have never been observed. Experimental evidence, such as beta decay, supports the  alternative hypothesis that the mirror image of matter is antimatter. This problem is solved by  identifying a flaw in the conventional derivation of the parity operator, then deriving a new parity  operator based on the algebraic properties of vectors. Second, the conjugate momenta (p&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;) in the freeparticle  Hamiltonian (H) do not have the proper relation ( p&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; =&amp;amp;#948;H &amp;amp;#948;q&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; ) to the time derivatives of  coordinates ( q&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt; ). This problem is solved by replacing the mass term with convection and rotation  terms. We then show that the resultant bispinor equation of evolution is equivalent to a classical  second-order wave equation for angular momentum density in an elastic solid. The co-existence of  forward- and backward-propagating waves along a single axis is the basis of half-integer spin. Wave  interference produces both the Lorenz force and the Pauli Exclusion Principle. Mass is associated with  radially inward acceleration of the wave such as occurs in a soliton. Angular correlations between spin  states are equal to the quantum correlations. Bell?s Theorem is not applicable to classical bispinors.  Matter and anti-matter are related by spatial inversion, consistent with experimental observations. The  classical wave formulation therefore provides a conceptually clear interpretation of fermion dynamics.[[Category:Scientific Paper]]&lt;/div&gt;</summary>
		<author><name>Maintenance script</name></author>
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