<?xml version="1.0"?>
<feed xmlns="http://www.w3.org/2005/Atom" xml:lang="en">
	<id>https://www.conservapedia.com/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=FixingPhysics</id>
	<title>Conservapedia - User contributions [en]</title>
	<link rel="self" type="application/atom+xml" href="https://www.conservapedia.com/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=FixingPhysics"/>
	<link rel="alternate" type="text/html" href="https://www.conservapedia.com/Special:Contributions/FixingPhysics"/>
	<updated>2026-10-20T15:53:56Z</updated>
	<subtitle>User contributions</subtitle>
	<generator>MediaWiki 1.35.14</generator>
	<entry>
		<id>https://www.conservapedia.com/index.php?title=Hermitian_matrix&amp;diff=1652127</id>
		<title>Hermitian matrix</title>
		<link rel="alternate" type="text/html" href="https://www.conservapedia.com/index.php?title=Hermitian_matrix&amp;diff=1652127"/>
		<updated>2020-05-29T19:00:54Z</updated>

		<summary type="html">&lt;p&gt;FixingPhysics: Fixed sloppy description where diagonal entries were mistakenly allowed to be complex.&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;A '''Hermitian matrix''' is one that satisfies &amp;lt;math&amp;gt;M=M^\dagger&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;M^\dagger&amp;lt;/math&amp;gt; is the Hermitian conjugate of &amp;lt;math&amp;gt;M&amp;lt;/math&amp;gt; (i.e., the matrix formed by transposing &amp;lt;math&amp;gt;M&amp;lt;/math&amp;gt; and taking the [[complex conjugate]] of each element). As an example, the most general 2x2 Hermitian [[matrix]] has the form&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\begin{pmatrix}&lt;br /&gt;
  a      &amp;amp; b      \\&lt;br /&gt;
  b^*      &amp;amp; c &lt;br /&gt;
\end{pmatrix}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
for any complex number &amp;lt;math&amp;gt;b&amp;lt;/math&amp;gt; and real numbers &amp;lt;math&amp;gt;a&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;c&amp;lt;/math&amp;gt;. In the case where all elements of the matrix are real, a Hermitian matrix becomes symmetric (as Hermitian conjugation then becomes equivalent to transposition).&lt;br /&gt;
&lt;br /&gt;
==Properties of Hermitian matrices==&lt;br /&gt;
* The [[eigenvalue]]s are all real.&lt;br /&gt;
* The [[eigenvector]]s corresponding to different eigenvalues are orthogonal.&lt;br /&gt;
&lt;br /&gt;
Because of these properties, Hermitian matrices have important applications in [[quantum mechanics]].&lt;br /&gt;
[[Category:Linear Algebra]]&lt;/div&gt;</summary>
		<author><name>FixingPhysics</name></author>
	</entry>
</feed>