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		<title>User:TedJanssen - Revision history</title>
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	<entry>
		<id>https://dictionary.iucr.org/index.php?title=User:TedJanssen&amp;diff=3016&amp;oldid=prev</id>
		<title>TedJanssen at 13:04, 16 May 2009</title>
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				<updated>2009-05-16T13:04:30Z</updated>
		
		<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;[[Acceptance Domain]]&lt;br /&gt;
&lt;br /&gt;
Synonyms: window, atomic domain&lt;br /&gt;
&lt;br /&gt;
Domaine d'acceptation, fenetre (Fr.)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
When an aperiodic crystalline point set is obtained by the intersection method, as the intersection of a periodic array of finite, disjoint components in superspace and the physical&lt;br /&gt;
space, then  there is, for each point , a component in the higher-dimensional&lt;br /&gt;
unit cell. These components are called ''acceptance domains'',  ''atomic surfaces'', ''atomic domains'', or&lt;br /&gt;
''windows'' in the literature. The positions of  atoms in aperiodic crystals (or vertices in the case of a tiling)&lt;br /&gt;
are the intersection of the atomic surfaces with the physical space. This construction of the&lt;br /&gt;
points is called the ''intersection method''.&lt;br /&gt;
&lt;br /&gt;
'''History'''&lt;br /&gt;
&lt;br /&gt;
The term ''window'' comes from an alternative construction. One considers a 'tube'&lt;br /&gt;
in ''n''-dimensional superspace&lt;br /&gt;
that is the product of the ''m''-dimensional physical space ''V'' and a transversal finite (''n-m'')-dimensional object ''O'':&lt;br /&gt;
''V times O''. Then the points of the ''n''-dimensional lattice, corresponding&lt;br /&gt;
to the periodic embedding of the structure in ''V'',&lt;br /&gt;
that lie inside the tube are projected&lt;br /&gt;
on ''V'' (See Fig.[[Image:BO02F20.jpg]]). These are the points of the aperiodic structure in ''V''. &lt;br /&gt;
The construction is called the ''cut-and-project method''. The object ''O''&lt;br /&gt;
is the ''window'', or ''acceptance domain''. The latter expresses the fact that only&lt;br /&gt;
lattice points inside the tube are projected. The result is the same as attaching a copy&lt;br /&gt;
of ''O'' to each lattice point, and considering the intersection of this&lt;br /&gt;
periodic array with ''V''. Actually, the latter construction is more special, in the&lt;br /&gt;
sense that the atomic surfaces in this are by definition flat, whereas the intersection&lt;br /&gt;
method allows arbitrarily shaped ones.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
See also: ''atomic surface''.&lt;/div&gt;</summary>
		<author><name>TedJanssen</name></author>	</entry>

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