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	<title>Lysario - by Panagiotis Chatzichrisafis &#187; Quantum Mechanics</title>
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		<title>Liboff: &#8220;Introductory Quantum Mechanics&#8221;, 2nd edition p.86 exercise 3.16</title>
		<link>https://lysario.de/solved_problems/liboff-introductory-quantum-mechanics-2nd-edition-p86-exercise-316</link>
		<comments>https://lysario.de/solved_problems/liboff-introductory-quantum-mechanics-2nd-edition-p86-exercise-316#comments</comments>
		<pubDate>Fri, 02 Jan 2009 16:55:15 +0000</pubDate>
		<dc:creator>Panagiotis</dc:creator>
				<category><![CDATA[Quantum Mechanics]]></category>
		<category><![CDATA[Solved Problems]]></category>

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		<description><![CDATA[The exercise [1, p. 86 ex. 3.16] asks to prove that if the eigenfunctions and eigenvalues of an operator are and , respectively () then the eigenfunctions of a function having an expansion of the form: (1) will also be   with corresponding eigenvalues , . That is . Solution:To prove this feature, one must [...]]]></description>
				<content:encoded><![CDATA[The exercise <a href="https://lysario.de/solved_problems/liboff-introductory-quantum-mechanics-2nd-edition-p86-exercise-316#lysario.desolved_problemsliboff-introductory-quantum-mechanics-2nd-edition-p86-exercise-316bib1">[1, p. 86 ex. 3.16]</a> asks to prove that if the eigenfunctions and eigenvalues of an operator <img src="https://lysario.de/wp-content/cache/tex_b3ed6bb9c1b2052f1127a36eac2e3581.png" align="bottom" class="tex" alt=" \widehat{A} " /> are <img src="https://lysario.de/wp-content/cache/tex_22cb07ffb7cbef612619dadcb9fb8f24.png" align="bottom" class="tex" alt="\{\phi_{n}\}" /> and <img src="https://lysario.de/wp-content/cache/tex_3d0299a906f22a56ae7e72f5cb3590bf.png" align="bottom" class="tex" alt="\{a_{n}\}" />, respectively (<img src="https://lysario.de/wp-content/cache/tex_94d1ab37768c8258c37cfbfc17f97813.png" align="bottom" class="tex" alt="\ensuremath{\widehat{A}}\phi_{n}=a_{n}\phi_{n}" />) then the eigenfunctions of a function <img src="https://lysario.de/wp-content/cache/tex_50bbd36e1fd2333108437a2ca378be62.png" align="bottom" class="tex" alt="f(x)" /> having an expansion of the form:  
<br/><table>
<tr><td colspan="3"><img src="https://lysario.de/wp-content/cache/tex_8ca88a08affac30c043b4776d37acfa3.png" align="bottom" class="tex" alt="f(x)=\sum\limits^{\infty}_{l=0}b_{l}x^{l}" /></td><td><a name="lysario.desolved_problemsliboff-introductory-quantum-mechanics-2nd-edition-p86-exercise-316eq1"> (1)</a></td></tr>
</table><br/> will also be <img src="https://lysario.de/wp-content/cache/tex_581fb7c8c3b369d95df763246ef47876.png" align="bottom" class="tex" alt="\phi_n" />   with corresponding eigenvalues <img src="https://lysario.de/wp-content/cache/tex_a028a664e96d2b31b390545ece9969c3.png" align="bottom" class="tex" alt="f(a_n)" /> , <img src="https://lysario.de/wp-content/cache/tex_8cb260b52b7b4ede9487cad98386bbb5.png" align="bottom" class="tex" alt="n=0,1..." /> . That is <img src="https://lysario.de/wp-content/cache/tex_4dfbc4bf5e6b1da61439dbfadb155cb8.png" align="bottom" class="tex" alt="f(\widehat{A})\phi_n=f(a_n)\phi_n" />.

<span id="more-6"></span>

<br /> <strong>Solution:</strong>To prove this feature, one must have the distributive property of operators in mind which can be stated as:   <img src="https://lysario.de/wp-content/cache/tex_23e4957c21889f377b2c37a9a0cc1da4.png" align="bottom" class="tex" alt="\widehat{A}^{l}=\widehat{A}^{l-1}\cdot \widehat{A}." />
Iterative application of the operator <img src="https://lysario.de/wp-content/cache/tex_24071035eccd8ece496226e53a63b2e0.png" align="bottom" class="tex" alt="\widehat{A}^{l}" /> to the eigenfunction <img src="https://lysario.de/wp-content/cache/tex_581fb7c8c3b369d95df763246ef47876.png" align="bottom" class="tex" alt="\phi_n" /> gives the following result:

<br/><table>
<tr><td colspan="3"><img src="https://lysario.de/wp-content/cache/tex_4648ba85db138dce23db3c4fe10734e4.png" align="bottom" class="tex" alt="\widehat{A}^{l}\phi_n=\widehat{A}^{l-1}\widehat{A}\phi_n = a_n\widehat{A}^{l-1}\phi_n
=...= a^{k}\widehat{A}^{l-k}\phi_n=...=a^{l}_{n}\phi_n." /></td><td><a name="lysario.desolved_problemsliboff-introductory-quantum-mechanics-2nd-edition-p86-exercise-316eq2"> (2)</a></td></tr>
</table><br/>

The function <img src="https://lysario.de/wp-content/cache/tex_6327221576695c69d71fe41d5100117a.png" align="bottom" class="tex" alt="f(\widehat{A})" /> can be written with the use of the given expansion as:
<img src="https://lysario.de/wp-content/cache/tex_dbf3b4a541e0e9c57051d29e1ce08f4d.png" align="bottom" class="tex" alt="f(\widehat{A})=\sum^{\infty}_{l=0}b_{l}\widehat{A}^{l}" />
Applying the right hand side to an eigenfunction <img src="https://lysario.de/wp-content/cache/tex_c611363cf5b86cfb587bd9e56e622ef4.png" align="bottom" class="tex" alt="\phi_{n}" /> results in:

<br/><table>
<tr> <td><img src="https://lysario.de/wp-content/cache/tex_d639a4c4600df0eaf391a28f0113bf10.png" align="bottom" class="tex" alt="f(\widehat{A})\phi_n" /></td><td><img src="https://lysario.de/wp-content/cache/tex_43ec3e5dee6e706af7766fffea512721.png" align="bottom" class="tex" alt="=" /></td><td><img src="https://lysario.de/wp-content/cache/tex_1e5eeb43735ce8c3528450f64e764913.png" align="bottom" class="tex" alt="\sum\limits^{\infty}_{l=0}b_{l}\widehat{A}^{l}\phi_n  " /></td><td></td></tr>
<tr><td></td><td><img src="https://lysario.de/wp-content/cache/tex_43ec3e5dee6e706af7766fffea512721.png" align="bottom" class="tex" alt="=" /></td><td><img src="https://lysario.de/wp-content/cache/tex_5316bfd36c47ca886696964245bd1078.png" align="bottom" class="tex" alt="\sum\limits^{\infty}_{l=0}b_{l}a^{l}_{n}\phi_n " /></td><td></td></tr>
<tr><td></td><td><img src="https://lysario.de/wp-content/cache/tex_43ec3e5dee6e706af7766fffea512721.png" align="bottom" class="tex" alt="=" /></td><td><img src="https://lysario.de/wp-content/cache/tex_88822f54b7153e3762f5cca11ccf128a.png" align="bottom" class="tex" alt="f(a_n)\phi_n " /></td><td><a name="lysario.desolved_problemsliboff-introductory-quantum-mechanics-2nd-edition-p86-exercise-316eqeq1"> (3)</a></td></tr>
</table><br/>
The last result (<a href="#lysario.desolved_problemsliboff-introductory-quantum-mechanics-2nd-edition-p86-exercise-316eqeq1">3</a>) means that the eigenfunctions of an operator <img src="https://lysario.de/wp-content/cache/tex_6327221576695c69d71fe41d5100117a.png" align="bottom" class="tex" alt="f(\widehat{A})" /> are the same as for the operator <img src="https://lysario.de/wp-content/cache/tex_b7b021f2a04a520229ceac20d373084a.png" align="bottom" class="tex" alt="\widehat{A}" /> but the eigenvalues are given by <img src="https://lysario.de/wp-content/cache/tex_a028a664e96d2b31b390545ece9969c3.png" align="bottom" class="tex" alt="f(a_n)" /> where <img src="https://lysario.de/wp-content/cache/tex_825b3fd5bafbc46b9a560ea9f16b21dd.png" align="bottom" class="tex" alt="a_n" /> are the eigenvalues of the operator <img src="https://lysario.de/wp-content/cache/tex_b7b021f2a04a520229ceac20d373084a.png" align="bottom" class="tex" alt="\widehat{A}" />; Q.E.D..
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