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	<title>Physics:+ h.c. - Revision history</title>
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	<updated>2026-05-23T01:46:33Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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		<title>WikiHarold: change</title>
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		<updated>2024-02-05T10:07:07Z</updated>

		<summary type="html">&lt;p&gt;change&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;&amp;#039;&amp;#039;&amp;#039;+ h.c.&amp;#039;&amp;#039;&amp;#039; is an abbreviation for &amp;quot;&amp;lt;u&amp;gt;plus&amp;lt;/u&amp;gt; the &amp;lt;u&amp;gt;&amp;#039;&amp;#039;H&amp;#039;&amp;#039; &amp;lt;/u&amp;gt;ermitian &amp;lt;u&amp;gt;&amp;#039;&amp;#039;c&amp;#039;&amp;#039; &amp;lt;/u&amp;gt;onjugate&amp;quot;; it means is that there are additional terms which are the Hermitian conjugates of all of the preceding terms, and is a convenient shorthand to omit half the terms actually present.&amp;lt;ref name=Özkan-HueyWen-2019-03-16/&amp;gt;&amp;lt;ref name=&amp;quot;physfrms2010&amp;quot;/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Context and use==&lt;br /&gt;
The [[Language of mathematics|notation convention]] &amp;quot;+&amp;amp;nbsp;h.c.&amp;quot; is common in [[Physics:Quantum mechanics|quantum mechanics]] in the context of writing out formulas for [[Lagrangian mechanics#Quantum mechanics|Lagrangian]]s and [[Physics:Hamiltonian (quantum mechanics)|Hamiltonians]], which conventionally are both required to be Hermitian operators.&amp;lt;ref name=physfrms2010&amp;gt;{{cite web |title=Meaning of h.c. in Lagrangians (&amp;amp; elsewhere?) |url=https://www.physicsforums.com/threads/meaning-of-h-c-in-lagrangians-elsewhere.454071/ |date=2010-12-05 |website=Physics Forums |access-date=2018-05-23 |df=dmy-all}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The expression&lt;br /&gt;
:&amp;lt;math&amp;gt;\mathcal{L} = A + B + C + ~ \text{h.c.} ~&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
means&lt;br /&gt;
:&amp;lt;math&amp;gt;\mathcal{L} = A + B + C + A^\dagger + B^\dagger + C^\dagger ~.&amp;lt;/math&amp;gt;&amp;lt;ref name=physfrms2010/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The mathematics of quantum mechanics is based on [[Complex number|complex number]]s, whereas almost all observations (measurements) are only [[Real number|real number]]s. Adding its own conjugate to an operator guarantees that the combination is Hermitian, which in turn guarantees that the combined operator&amp;#039;s eigenvalues will be real numbers, suitable for predicting values of observations / measurements.&amp;lt;ref name=Özkan-HueyWen-2019-03-16&amp;gt;{{cite book |last1=Özkan |first1=Tristan |last2=Lin |first2=Huey-Wen |chapter=Quantum3: Learning QCD through Intuitive Play |title=Proceedings of the 36th Annual International Symposium on Lattice Field Theory (LATTICE2018) |series=Proceedings of Science |volume=334 |date=29 May 2019 |pages=326 |arxiv=1901.00022 |doi=10.22323/1.334.0326 |s2cid=119383350 |oclc=1082145757 |doi-access=free }}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Dagger and asterisk notation===&lt;br /&gt;
In the expressions above, &amp;lt;math&amp;gt;A^\dagger&amp;lt;/math&amp;gt; is used as the symbol for the Hermitian conjugate (also called the &amp;#039;&amp;#039;[[Conjugate transpose|conjugate transpose]]&amp;#039;&amp;#039;) of &amp;lt;math&amp;gt;A&amp;lt;/math&amp;gt;, defined as applying both the [[Complex conjugate|complex conjugate]] and the [[Transpose|transpose]] transformations to the operator &amp;lt;math&amp;gt;A&amp;lt;/math&amp;gt;, in any order.&lt;br /&gt;
&lt;br /&gt;
The dagger (&amp;lt;math&amp;gt;\dagger&amp;lt;/math&amp;gt;) is an old notation in mathematics, but is still widespread in quantum-mechanics. In mathematics (particularly [[Linear algebra|linear algebra]]) the Hermitian conjugate of &amp;lt;math&amp;gt;A&amp;lt;/math&amp;gt; is commonly written as &amp;lt;math&amp;gt;A^\ast&amp;lt;/math&amp;gt;, but in quantum mechanics the asterisk (&amp;lt;math&amp;gt;\ast&amp;lt;/math&amp;gt;) notation is sometimes used for the [[Complex conjugate|complex conjugate]] only, and not the combined [[Conjugate transpose|conjugate transpose]] (Hermitian conjugate).&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Hamiltonian mechanics]]&lt;br /&gt;
[[Category:Quantum mechanics]]&lt;br /&gt;
[[Category:Lagrangian mechanics]]&lt;br /&gt;
[[Category:Operator theory]]&lt;br /&gt;
&lt;br /&gt;
{{Sourceattribution|+ h.c.}}&lt;/div&gt;</summary>
		<author><name>WikiHarold</name></author>
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