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		<title>en&gt;ChrisGualtieri: Remove stub template(s). Page is start class or higher. Also check for and do General Fixes + Checkwiki fixes using AWB</title>
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		<summary type="html">&lt;p&gt;Remove stub template(s). Page is start class or higher. Also check for and do General Fixes + Checkwiki fixes using &lt;a href=&quot;/index.php?title=Testwiki:AWB&amp;amp;action=edit&amp;amp;redlink=1&quot; class=&quot;new&quot; title=&quot;Testwiki:AWB (page does not exist)&quot;&gt;AWB&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Orphan|date=June 2013}}&lt;br /&gt;
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The &amp;#039;&amp;#039;&amp;#039;Stimulated Raman adiabatic passage&amp;#039;&amp;#039;&amp;#039; (STIRAP) process permits transfer of a population between two applicable [[quantum state]]s via at least two coherent  [[Electromagnetic pulse|electromagnetic (light) pulses]]. These light pulses drive the transitions of the three level Ʌ [[atom]] or multilevel system.&amp;lt;ref&amp;gt;{{cite book | author= Heike Schwager. | title = A quantum memory for light in nuclear spin of quantum dot, p. 53, 2008}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
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==Population transfer in three level Ʌ atom==&lt;br /&gt;
Consider the description of three level Ʌ atom having [[ground state]] &amp;lt;math&amp;gt;|g_1\rangle &amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;|g_2\rangle &amp;lt;/math&amp;gt;  (for simplicity consider the energy of both ground states are same) and [[excited state]] &amp;lt;math&amp;gt;|e\rangle &amp;lt;/math&amp;gt; respectively. Suppose in the beginning the total population is in the ground state &amp;lt;math&amp;gt;|g_1\rangle &amp;lt;/math&amp;gt;. Here the logic for transformation of the population from ground state &amp;lt;math&amp;gt;|g_1\rangle &amp;lt;/math&amp;gt; to &amp;lt;math&amp;gt;|g_2\rangle &amp;lt;/math&amp;gt; is that initially the unpopulated states &amp;lt;math&amp;gt;|g_2\rangle &amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;|e\rangle &amp;lt;/math&amp;gt; couple, afterward superposition of state &amp;lt;math&amp;gt;|g_2\rangle &amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;|e\rangle &amp;lt;/math&amp;gt; couple to the state &amp;lt;math&amp;gt;|g_1\rangle &amp;lt;/math&amp;gt;. Thereby a state is formed that permits the transformation of the population into state &amp;lt;math&amp;gt;|g_2\rangle &amp;lt;/math&amp;gt; without populating the excited state &amp;lt;math&amp;gt;|e\rangle &amp;lt;/math&amp;gt;. This process of transforming the population without populating the excited state is called the stimulated [[Raman]] adiabatic passage.&amp;lt;ref&amp;gt;{{cite journal |author=P. Marte, P. Zoller, J.L.Hall |title= Quantum state-mapping between multi-level atoms and cavity light fields, Phys. Rev A44 , 1991}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
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==References==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
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[[Category:Quantum mechanics]]&lt;/div&gt;</summary>
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