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	<title>NA-MIC/Projects/Structural/Conformal Flattening in ITK - Revision history</title>
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		<title>Andy: Update from Wiki</title>
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		<updated>2006-12-18T19:32:30Z</updated>

		<summary type="html">&lt;p&gt;Update from Wiki&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;== Description ==&lt;br /&gt;
&lt;br /&gt;
A general description of this project is given on page: [[NA-MIC/Projects/fMRI_Analysis/Conformal_Flattening_for_fMRI_Visualization|Conformal Flattening for fMRI Visualization]].&lt;br /&gt;
&lt;br /&gt;
This page outlines the steps we will take to code the Conformal Flattening mapping in ITK.&lt;br /&gt;
&lt;br /&gt;
For the detail of the algorithm please refer to the paper: S. Angenent, S. Haker, A. Tannenbaum, and R. Kikinis, “On the Laplace-Beltrami operator and brain surface flattening,” IEEE Trans. on Medical Imaging, Vol. 18, pp. 700-711, 1999.&lt;br /&gt;
&lt;br /&gt;
An angle preserving flattening mapping is proposed in this paper. The explicit transform is obtained by solving a partial differential equation. Such transform will map the original surface to a plane(flattening) and then one can use classic stereographic transformation to map the plane to a sphere.&lt;br /&gt;
&lt;br /&gt;
The process of the algorithm is brifly given below:&lt;br /&gt;
&lt;br /&gt;
# The conformal mapping &amp;lt;span class=&amp;quot;texhtml&amp;quot;&amp;gt;''f''&amp;lt;/span&amp;gt; is defined on the originla surface &amp;lt;span class=&amp;quot;texhtml&amp;quot;&amp;gt;Σ&amp;lt;/span&amp;gt; as [[Image:89ff38a84b2fcde5fa7c5ea0f8c97a6b.png|\triangle f = (\frac{\partial}{\partial u} - i\frac{\partial}{\partial v})\delta_p]]. In that &amp;lt;span class=&amp;quot;texhtml&amp;quot;&amp;gt;''u''&amp;lt;/span&amp;gt; and &amp;lt;span class=&amp;quot;texhtml&amp;quot;&amp;gt;''v''&amp;lt;/span&amp;gt; are the conformal coordinates defined on the surface and the &amp;lt;span class=&amp;quot;texhtml&amp;quot;&amp;gt;δ&amp;lt;sub&amp;gt;''p''&amp;lt;/sub&amp;gt;&amp;lt;/span&amp;gt; is a Dirac function whose value is non-zero only at point &amp;lt;span class=&amp;quot;texhtml&amp;quot;&amp;gt;''p''&amp;lt;/span&amp;gt;. By solving this partial differential equation the mapping &amp;lt;span class=&amp;quot;texhtml&amp;quot;&amp;gt;''f''&amp;lt;/span&amp;gt; can be obtained.&lt;br /&gt;
# To solve that equation on the discrete mesh representation of the surface, finite element method(FEM) is used. The problem is turned to solving a linear system &amp;lt;span class=&amp;quot;texhtml&amp;quot;&amp;gt;''D''''x'' = ''b''&amp;lt;/span&amp;gt;. Since b is complex vector, the real and imaginary parts of the mapping &amp;lt;span class=&amp;quot;texhtml&amp;quot;&amp;gt;''f''&amp;lt;/span&amp;gt; can be calculated separately by two linear system.&lt;br /&gt;
# Having the mapping &amp;lt;span class=&amp;quot;texhtml&amp;quot;&amp;gt;''f''&amp;lt;/span&amp;gt;, the original surface can be mapped to a plane.&lt;br /&gt;
# Further, the plane can be mapped to a sphere by the stereographic projection.&lt;br /&gt;
&lt;br /&gt;
The code for doing this is currently local codes, not having been embeded into ITK class hierarchy. This is what we are working on now.&lt;br /&gt;
&lt;br /&gt;
== Current Status ==&lt;br /&gt;
&lt;br /&gt;
* We have written and tested the itkConformalFlatteningFilter&lt;br /&gt;
* Our paper on this was accepted for oral presentation at the 2006 MICCAI Open-source Workshop&lt;br /&gt;
&lt;br /&gt;
== Next Steps ==&lt;br /&gt;
&lt;br /&gt;
* We will help integrate this into the ITK CVS repository&lt;br /&gt;
&lt;br /&gt;
== Members ==&lt;br /&gt;
&lt;br /&gt;
* Yi Gao (Gatech)&lt;br /&gt;
* John Melonakos (Gatech)&lt;br /&gt;
* Jim Miller (GE)&lt;br /&gt;
* Luis Ibanez (Kitware)&lt;br /&gt;
&lt;br /&gt;
== Links ==&lt;br /&gt;
&lt;br /&gt;
* [[NA-MIC/Projects/fMRI_Analysis/Conformal_Flattening_for_fMRI_Visualization|Conformal Flattening for fMRI Visualization]]&lt;/div&gt;</summary>
		<author><name>Andy</name></author>
		
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