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	<title>Excursion probability - Revision history</title>
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	<entry>
		<id>https://en.formulasearchengine.com/index.php?title=Excursion_probability&amp;diff=28323&amp;oldid=prev</id>
		<title>en&gt;Michael Hardy at 19:29, 13 December 2012</title>
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		<updated>2012-12-13T19:29:04Z</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;Multipole magnets are magnets built from multiple individual magnets, typically used to control [[Charged particle beam|beams of charged particles]]. Each type of magnet serves a particular purpose.&lt;br /&gt;
&lt;br /&gt;
* [[Dipole magnet]]s are used to bend the trajectory of particles&lt;br /&gt;
* [[Quadrupole magnets]] are used to focus particle beams&lt;br /&gt;
* [[Sextupole magnet]]s are used to correct for [[chromaticity (accelerator)|chromaticity]] introduced by quadrupole magnets &amp;lt;ref&amp;gt;http://cas.web.cern.ch/cas/Bulgaria-2010/Talks-web/Brandt-1-web.pdf&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Magnetic field equations==&lt;br /&gt;
&lt;br /&gt;
The magnetic field of an ideal multipole magnet in an accelerators is typically modeled as having no (or a constant) component parallel to the nominal beam direction (&amp;lt;math&amp;gt;z&amp;lt;/math&amp;gt; direction)&lt;br /&gt;
and the for the transverse components can be written as complex numbers:&amp;lt;ref&amp;gt;http://cas.web.cern.ch/cas/Belgium-2009/Lectures/PDFs/Wolski-1.pdf&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
  B_y + i B_x = C_n \cdot ( x + iy )^{n-1}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y&amp;lt;/math&amp;gt; are the coordinates in the plane transverse to the nominal beam direction. &amp;lt;math&amp;gt;C_n&amp;lt;/math&amp;gt; is a complex number specifying the orientation and strength of the magnetic field. &amp;lt;math&amp;gt;B_x&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;B_y&amp;lt;/math&amp;gt; are the components of the magnetic field in the corresponding directions. Fields with a real &amp;lt;math&amp;gt;C_n&amp;lt;/math&amp;gt; are called &amp;#039;normal&amp;#039; while fields with &amp;lt;math&amp;gt;C_n&amp;lt;/math&amp;gt; purely imaginary are called &amp;#039;skewed&amp;#039;.&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot; style=&amp;quot;margin: 1em auto 1em auto;&amp;quot;&lt;br /&gt;
|+ First few multipole fields&lt;br /&gt;
|-&lt;br /&gt;
!n&lt;br /&gt;
!name&lt;br /&gt;
!magnetic field lines&lt;br /&gt;
!example device&lt;br /&gt;
|-&lt;br /&gt;
| 1 || [[dipole magnet|dipole]] || [[File:Magnetic field of an idealized dipole.svg|thumb]] || [[Image:Hetdipole.jpg|thumb|250px]] &lt;br /&gt;
|-&lt;br /&gt;
| 2 || [[quadrupole magnet|quadrupole]] || [[File:Magnetic field of an idealized quadrupole.svg|thumb]] || [[Image:Aust.-Synchrotron,-Quadrupole-Focusing-Magnet,-14.06.2007.jpg|thumb|250px]]&lt;br /&gt;
|-&lt;br /&gt;
| 3 || [[sextupole magnet|sextupole]] || [[File:Magnetic field of an idealized sextupole.svg|thumb]] || [[Image:Aust.-Synchrotron,-Sextupole-Focusing-Magnet,-14.06.2007.jpg|thumb|250px]]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{Reflist}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Types of magnets]]&lt;br /&gt;
[[Category:Accelerator physics]]&lt;/div&gt;</summary>
		<author><name>en&gt;Michael Hardy</name></author>
	</entry>
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