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	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Du_Bois_singularity&amp;diff=24230</id>
		<title>Du Bois singularity</title>
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		<updated>2013-01-07T07:37:50Z</updated>

		<summary type="html">&lt;p&gt;89.244.108.152: added &amp;lt;math&amp;gt; instead of &amp;#039;&amp;#039;foo&amp;#039;&amp;#039;&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{about|an extension of the theory of the [[Lebesgue integral]] to [[manifold]]s|numerical method|geometric integrator}}&lt;br /&gt;
In the [[mathematics|mathematical]] fields of [[differential geometry]] and [[geometric measure theory]], &#039;&#039;&#039;homological integration&#039;&#039;&#039; or &#039;&#039;&#039;geometric integration&#039;&#039;&#039; is a method for extending the notion of the [[integral]] to [[manifold]]s.  Rather than functions or [[differential form]]s, the integral is defined over [[current (mathematics)|currents]] on a manifold.&lt;br /&gt;
&lt;br /&gt;
The theory is &amp;quot;homological&amp;quot; because currents themselves are defined by duality with differential forms.  To wit, the space &#039;&#039;D&#039;&#039;&amp;lt;sup&amp;gt;&#039;&#039;k&#039;&#039;&amp;lt;/sup&amp;gt; of &#039;&#039;k&#039;&#039;-currents on a manifold &#039;&#039;M&#039;&#039; is defined as the [[dual space]], in the sense of [[distribution (mathematics)|distributions]], of the space of &#039;&#039;k&#039;&#039;-forms Ω&amp;lt;sup&amp;gt;&#039;&#039;k&#039;&#039;&amp;lt;/sup&amp;gt; on &#039;&#039;M&#039;&#039;.  Thus there is a pairing between &#039;&#039;k&#039;&#039;-currents &#039;&#039;T&#039;&#039; and &#039;&#039;k&#039;&#039;-forms α, denoted here by&lt;br /&gt;
:&amp;lt;math&amp;gt;\langle T, \alpha\rangle.&amp;lt;/math&amp;gt;&lt;br /&gt;
Under this duality pairing, the [[exterior derivative]] &lt;br /&gt;
:&amp;lt;math&amp;gt;d : \Omega^{k-1} \to \Omega^k&amp;lt;/math&amp;gt;&lt;br /&gt;
goes over to a [[boundary operator]]&lt;br /&gt;
:&amp;lt;math&amp;gt;\partial : D^k \to D^{k-1} &amp;lt;/math&amp;gt;&lt;br /&gt;
defined by&lt;br /&gt;
:&amp;lt;math&amp;gt;\langle\partial T,\alpha\rangle = \langle T, d\alpha\rangle&amp;lt;/math&amp;gt;&lt;br /&gt;
for all α&amp;amp;nbsp;∈&amp;amp;nbsp;Ω&amp;lt;sup&amp;gt;&#039;&#039;k&#039;&#039;&amp;lt;/sup&amp;gt;.  This is a homological rather than [[cohomology theory|cohomological]] construction.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
* {{citation&lt;br /&gt;
| last = Federer&lt;br /&gt;
| first = Herbert&lt;br /&gt;
| authorlink = Herbert Federer&lt;br /&gt;
| title = Geometric measure theory&lt;br /&gt;
| publisher = Springer-Verlag New York Inc.&lt;br /&gt;
| location = New York&lt;br /&gt;
| year = 1969&lt;br /&gt;
| pages = xiv+676&lt;br /&gt;
| isbn = 978-3-540-60656-7&lt;br /&gt;
| id= {{MathSciNet|id=0257325}}&lt;br /&gt;
| series = series Die Grundlehren der mathematischen Wissenschaften&lt;br /&gt;
| volume = 153 }}&lt;br /&gt;
* {{citation&lt;br /&gt;
|first=H.&lt;br /&gt;
|last=Whitney&lt;br /&gt;
|author-link=Hassler Whitney&lt;br /&gt;
|title=Geometric Integration Theory&lt;br /&gt;
|series=Princeton Mathematical Series&lt;br /&gt;
|volume=21&lt;br /&gt;
|publisher=[[Princeton University Press]] and [[Oxford University Press]]&lt;br /&gt;
|place=Princeton, NJ and London&lt;br /&gt;
|year=1957&lt;br /&gt;
|pages= XV+387&lt;br /&gt;
|mr=0087148&lt;br /&gt;
|zbl=0083.28204&lt;br /&gt;
}}.&lt;br /&gt;
&lt;br /&gt;
[[Category:Definitions of mathematical integration]]&lt;br /&gt;
[[Category:Measure theory]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{geometry-stub}}&lt;/div&gt;</summary>
		<author><name>89.244.108.152</name></author>
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