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		<title>WikiSysop at 07:09, 18 September 2009</title>
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		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;== Citation ==&lt;br /&gt;
&lt;br /&gt;
Fanelli, D. &amp;amp; Öktem, O. Electron tomography: a short overview with an emphasis on the absorption potential model for the forward problem Inverse Problems, 2008, 24, 013001&lt;br /&gt;
&lt;br /&gt;
[http://scholar.google.com/scholar?cites=15589599254688959234&amp;amp;hl=en Cited by]&lt;br /&gt;
&lt;br /&gt;
== Abstract ==&lt;br /&gt;
&lt;br /&gt;
This review of the development and current status of electron tomography&lt;br /&gt;
deals mainly with the mathematical and algorithmic aspects. After a very&lt;br /&gt;
brief description of the role of electron tomography in structural biology, we&lt;br /&gt;
turn our attention to the derivation of the forward operator. Starting from&lt;br /&gt;
the Schr¨odinger equation, the electron–specimen interaction is modelled as&lt;br /&gt;
a diffraction tomography problem and the picture is completed by adding a&lt;br /&gt;
description of the optical system of the transmission electron microscope. The&lt;br /&gt;
first-order Born approximation enables one to explicitly express the intensity&lt;br /&gt;
for any finite wavenumber in terms of the propagation operator acting on the&lt;br /&gt;
specimen convolved with a point spread function, derived from the optics in the&lt;br /&gt;
transmission electron microscope. Next, we focus on the difficulties that cause&lt;br /&gt;
the reconstruction problem to be quite challenging. Special emphasis is put on&lt;br /&gt;
explaining the extremely low signal-to-noise ratio in the data combined with&lt;br /&gt;
the incomplete data problems, which lead to severe ill-posedness. The next step&lt;br /&gt;
is to derive the standard phase contrast model used in the electron tomography&lt;br /&gt;
community. The above-mentioned expression for the intensity generalizes&lt;br /&gt;
the standard phase contrast model which can be obtained by replacing the&lt;br /&gt;
propagation operator by its high-energy limit, the x-ray transform, as the&lt;br /&gt;
wavenumber tends to infinity. The importance of more carefully including&lt;br /&gt;
the wave nature of the electron–specimen interaction is supported by&lt;br /&gt;
performing an asymptotic analysis of the intensity as the wavenumber tends&lt;br /&gt;
to infinity. Next we provide an overview of the various reconstruction&lt;br /&gt;
methods that have been employed in electron tomography and we conclude by&lt;br /&gt;
mentioning a number of open problems. Besides providing an introduction to&lt;br /&gt;
electron tomography written in the ‘language of inverse problems’, the authors&lt;br /&gt;
hope to raise interest among experts in integral geometry and regularization&lt;br /&gt;
theory for the mathematical and algorithmic difficulties that are encountered in&lt;br /&gt;
electron tomography.&lt;br /&gt;
&lt;br /&gt;
== Keywords ==&lt;br /&gt;
&lt;br /&gt;
Image formation model, quantum physics, electron waves&lt;br /&gt;
&lt;br /&gt;
== Links ==&lt;br /&gt;
&lt;br /&gt;
Article http://www.ncbi.nlm.nih.gov/pubmed/18427122&lt;br /&gt;
&lt;br /&gt;
== Related software ==&lt;br /&gt;
&lt;br /&gt;
== Related methods ==&lt;br /&gt;
&lt;br /&gt;
== Comments ==&lt;/div&gt;</summary>
		<author><name>WikiSysop</name></author>
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