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		<id>https://en.formulasearchengine.com/w/index.php?title=Kolmogorov_automorphism&amp;diff=27998</id>
		<title>Kolmogorov automorphism</title>
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		<summary type="html">&lt;p&gt;76.24.31.52: removed extra apostrophe&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{One source|date=September 2013}}&lt;br /&gt;
&#039;&#039;&#039;Küpfmüller&#039;s uncertainty principle&#039;&#039;&#039; states that the relation of the rise time of a bandlimited signal to its bandwidth is a constant.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\Delta f\Delta t \ge k&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
with &amp;lt;math&amp;gt;k&amp;lt;/math&amp;gt; either &amp;lt;math&amp;gt;1&amp;lt;/math&amp;gt; or &amp;lt;math&amp;gt;\frac{1}{2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Proof==&lt;br /&gt;
A bandlimited signal &amp;lt;math&amp;gt;u(t)&amp;lt;/math&amp;gt; with [[fourier transform]] &amp;lt;math&amp;gt;\hat{u}(f)&amp;lt;/math&amp;gt; in frequency space is given by the multiplication of any signal &amp;lt;math&amp;gt;\underline{\hat{u}}(f)&amp;lt;/math&amp;gt; with &amp;lt;math&amp;gt;\hat{u}(f) = {{\underline{\hat{u}}(f)}}{{\Big|}_{\Delta f}}&amp;lt;/math&amp;gt; with a [[rectangular function]] of width &amp;lt;math&amp;gt;\Delta f&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\hat{g}(f) = \operatorname{rect} \left(\frac{f}{\Delta f} \right) =\chi_{[-\Delta f/2,\Delta f/2]}(f)&lt;br /&gt;
      := \begin{cases}1 &amp;amp; |f|\le\Delta f/2 \\ 0 &amp;amp; \text{else} \end{cases} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
as (applying the [[convolution theorem]])&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\hat{g}(f) \cdot \hat{u}(f) = (g * u)(t)  &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Since the fourier transform of a rectangular function is a [[sinc function]] and vice versa, follows&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; g(t) = \frac1{\sqrt{2\pi}}  \int \limits_{-\frac{\Delta f}{2}}^{\frac{\Delta f}{2}} 1 \cdot e^{j 2 \pi f t} df = \frac1{\sqrt{2\pi}} \cdot \Delta f \cdot \operatorname{si} \left( \frac{2 \pi t \cdot \Delta f}{2} \right)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Now the first root of &amp;lt;math&amp;gt; g(t) &amp;lt;/math&amp;gt; is at &amp;lt;math&amp;gt; \pm \frac{1}{\Delta f} &amp;lt;/math&amp;gt;, which is the rise time &amp;lt;math&amp;gt; \Delta t &amp;lt;/math&amp;gt; of the [[Pulse (signal processing)|pulse]] &amp;lt;math&amp;gt; g(t) &amp;lt;/math&amp;gt;, now follows&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; \Delta t =  \frac{1}{\Delta f} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Equality is given as long as &amp;lt;math&amp;gt;\Delta t&amp;lt;/math&amp;gt; is finite.&lt;br /&gt;
&lt;br /&gt;
Regarding that a real signal has both positive and negative frequencies of the same frequency band, &amp;lt;math&amp;gt;\Delta f&amp;lt;/math&amp;gt; becomes &amp;lt;math&amp;gt;2 \cdot \Delta f&amp;lt;/math&amp;gt;,&lt;br /&gt;
which leads to &amp;lt;math&amp;gt;k = \frac{1}{2}&amp;lt;/math&amp;gt; instead of &amp;lt;math&amp;gt;k = 1&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
*{{Citation | last1=Küpfmüller | first1=Karl | last2=Kohn | first2=Gerhard | title=Theoretische Elektrotechnik und Elektronik | publisher=[[Springer-Verlag]] | location=Berlin, Heidelberg  | isbn=978-3-540-56500-0 | year=2000}}.&lt;br /&gt;
&lt;br /&gt;
{{DEFAULTSORT:Kupfmuller&#039;s uncertainty principle}}&lt;br /&gt;
[[Category:Electronic engineering]]&lt;/div&gt;</summary>
		<author><name>76.24.31.52</name></author>
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