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	<title>Underactuation - Revision history</title>
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	<updated>2026-05-03T21:38:21Z</updated>
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		<id>https://en.formulasearchengine.com/index.php?title=Underactuation&amp;diff=13324&amp;oldid=prev</id>
		<title>en&gt;Yobot: Reference before punctuation and other fixes using AWB (9510)</title>
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		<updated>2013-10-04T14:21:17Z</updated>

		<summary type="html">&lt;p&gt;Reference before punctuation and other 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; (9510)&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Multiple issues|unreferenced = January 2010|unreferenced = December 2009}}&lt;br /&gt;
&lt;br /&gt;
In [[quantum chemistry]], the &amp;#039;&amp;#039;&amp;#039;Dyall Hamiltonian&amp;#039;&amp;#039;&amp;#039; is a modified [[Hamiltonian (quantum mechanics)|Hamiltonian]] with two-electron nature. It can be written as follows:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\hat{\mathcal{H}}^D = \hat{\mathcal{H}}^D_i + \hat{\mathcal{H}}^D_v + C&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\hat{\mathcal{H}}^D_i = \sum_{i}^{\rm core} \epsilon_i E_{ii} + \sum_r^{\rm virt} \epsilon_r E_{rr} &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;\hat{\mathcal{H}}^D_v = \sum_{ab}^{\rm act} h_{ab}^{\rm eff} E_{ab} +&lt;br /&gt;
\frac{1}{2} \sum_{abcd}^{\rm act} \left\langle ab \left.\right| cd \right\rangle \left(E_{ac}&lt;br /&gt;
E_{bd} - \delta_{bc} E_{ad} \right)&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;C = 2 \sum_{i}^{\rm core} h_{ii} + \sum_{ij}^{\rm core} \left( 2 \left\langle ij \left.\right| ij\right\rangle - \left \langle ij \left.\right| ji\right\rangle \right) - 2 \sum_{i}^{\rm core} \epsilon_i&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;h_{ab}^{\rm eff} =  h_{ab} + \sum_j \left( 2 \left\langle aj \left.\right| bj \right\rangle -&lt;br /&gt;
\left\langle aj \left.\right| jb \right\rangle \right)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where labels &amp;lt;math&amp;gt;i,j,\ldots&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;a,b,\ldots&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;r,s,\ldots&amp;lt;/math&amp;gt; denote core, active and virtual orbitals (see [[Complete active space]]) respectively, &amp;lt;math&amp;gt;\epsilon_i&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\epsilon_r&amp;lt;/math&amp;gt; are the orbital energies of the involved orbitals, and &amp;lt;math&amp;gt;E_{mn}&amp;lt;/math&amp;gt; operators are the spin-traced operators &amp;lt;math&amp;gt;a^{\dagger}_{m\alpha}a_{n\alpha} + a^{\dagger}_{m\beta}a_{n\beta}&amp;lt;/math&amp;gt;. These operators commute with &amp;lt;math&amp;gt;S^2&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;S_z&amp;lt;/math&amp;gt;, therefore the application of these operators on a spin-pure function produces again a spin-pure function. &lt;br /&gt;
&lt;br /&gt;
The Dyall Hamiltonian behaves like the true Hamiltonian inside the CAS space, having the same eigenvalues and eigenvectors of the true Hamiltonian projected onto the CAS space.&lt;br /&gt;
&lt;br /&gt;
[[Category:Quantum chemistry]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{theoretical-chem-stub}}&lt;/div&gt;</summary>
		<author><name>en&gt;Yobot</name></author>
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