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		<id>https://en.formulasearchengine.com/index.php?title=Substitution_matrix&amp;diff=229139</id>
		<title>Substitution matrix</title>
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		<updated>2014-02-24T01:37:45Z</updated>

		<summary type="html">&lt;p&gt;115.248.50.22: /* BLOSUM */&lt;/p&gt;
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		<title>Subbayya Sivasankaranarayana Pillai</title>
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		<updated>2013-12-05T10:04:51Z</updated>

		<summary type="html">&lt;p&gt;115.248.50.22: &lt;/p&gt;
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&lt;div&gt;In [[functional analysis]], the &#039;&#039;&#039;compression&#039;&#039;&#039; of a [[linear operator]] &#039;&#039;T&#039;&#039; on a [[Hilbert space]] to a [[Linear subspace|subspace]] &#039;&#039;K&#039;&#039; is the operator&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;P_K T \vert_K : K \rightarrow K &amp;lt;/math&amp;gt;,&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;P_K : H \rightarrow K&amp;lt;/math&amp;gt; is the [[orthogonal projection]] onto &#039;&#039;K&#039;&#039;. This is a natural way to obtain an operator on &#039;&#039;K&#039;&#039; from an operator on the whole Hilbert space. If &#039;&#039;K&#039;&#039; is an [[invariant subspace]] for &#039;&#039;T&#039;&#039;, then the compression of &#039;&#039;T&#039;&#039; to &#039;&#039;K&#039;&#039; is the [[restriction|restricted]] operator &#039;&#039;K&amp;amp;rarr;K&#039;&#039; sending &#039;&#039;k&#039;&#039; to &#039;&#039;Tk&#039;&#039;. &lt;br /&gt;
&lt;br /&gt;
More generally, for a linear operator &#039;&#039;T&#039;&#039; on a Hilbert space &amp;lt;math&amp;gt;H&amp;lt;/math&amp;gt; and an [[isometry]] &#039;&#039;V&#039;&#039; on a subspace &amp;lt;math&amp;gt;W&amp;lt;/math&amp;gt; of &amp;lt;math&amp;gt;H&amp;lt;/math&amp;gt;, define the &#039;&#039;&#039;compression&#039;&#039;&#039; of &#039;&#039;T&#039;&#039; to &amp;lt;math&amp;gt;W&amp;lt;/math&amp;gt; by &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;T_W = V^*TV : W \rightarrow W&amp;lt;/math&amp;gt;, &lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;V^*&amp;lt;/math&amp;gt; is the [[hermitian adjoint|adjoint]] of &#039;&#039;V&#039;&#039;. If &#039;&#039;T&#039;&#039; is a [[self-adjoint operator|self-adjoint]] operator, then the compression &amp;lt;math&amp;gt;T_W&amp;lt;/math&amp;gt; is also self-adjoint.&lt;br /&gt;
When &#039;&#039;V&#039;&#039; is replaced by the [[identity function]] &amp;lt;math&amp;gt;I: W -&amp;gt; H&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;V^* = I^*=P_K : H -&amp;gt; W&amp;lt;/math&amp;gt;, and we acquire the special definition above.&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
* [[Dilation (operator theory)|Dilation]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
* P. Halmos, A Hilbert Space Problem Book, Second Edition, Springer-Verlag, 1982.&lt;br /&gt;
&lt;br /&gt;
[[Category:Functional analysis]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{mathanalysis-stub}}&lt;/div&gt;</summary>
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