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        <identifier>oai:www.ideals.illinois.edu:2142/23945</identifier>
        <datestamp>2023-07-10</datestamp>
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        <setSpec>col_2142_5131</setSpec>
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        <thesis xmlns="http://www.ndltd.org/standards/metadata/etdms/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:dc="http://purl.org/dc/elements/1.1/" xsi:schemaLocation="http://www.ndltd.org/standards/metadata/etdms/1.1/ http://www.ndltd.org/standards/metadata/etdms/1.1/etdms11.xsd http://purl.org/dc/elements/1.1/ http://www.ndltd.org/standards/metadata/etdms/1.1/etdmsdc.xsd">
          <dc:contributor>Chang, Shau-Jin</dc:contributor>
          <dc:creator>Sagalovsky, Leonid</dc:creator>
          <dc:date>2011-05-18T17:15:59Z</dc:date>
          <dc:date>2011-05-18T17:15:59Z</dc:date>
          <dc:date>10000-01-01</dc:date>
          <dc:date>1989</dc:date>
          <dc:description>The motion of a charged particle through a magnetic field configuration can be described
in terms of deviation from a certain ideal trajectory. One uses power series expansion of the
phase-space coordinates to obtain the transfer matrices for a particular optical system.
In this thesis we present a complete third-order theory of computing transfer matrices and
apply it to magnetic elements in an accelerator beam-line. A particular attention is devoted
to studying particles' orbits in an extended fringing field of a dipole magnet. Analytical
solutions are obtained up to the third order in the formalism of the matrix theory. They
contain form factors describing the fall-off pattern of the field. These form factors are
dimensionless line integrals of the field strength and its derivative. There is one such integral
in the first-order solution, two in the second, and nine in the third.
An alternate way of describing charged particle optics is also presented. It is based on
a Hamiltonian treatment and uses certain symplectic operators, which are defined in terms
of Poisson brackets, to parametrize the transfer map of a system. We apply this approach
to the fringing field problem and obtain a third-order solution. We furthermore show how
to convert this solution into conventional transfer matrices by examining the connection
between the non-canonical matrix theory and the Hamiltonian description.</dc:description>
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  Previous issue date: 1989</dc:description>
          <dc:description>Restriction data tranferred 2014-07-01T11:14:44-05:00
Original Data
Group with Access UIUC Users [automated]
Release Date: none
Reason: Thesis</dc:description>
          <dc:description>Item marked as restricted to the 'UIUC Users [automated]' Group (id=2) by Carolyn Mead (cmead2@illinois.edu) on 2011-05-18T17:16:00Z
Item is restricted indefinitely.</dc:description>
          <dc:description>Thesis</dc:description>
          <dc:description>U of I Only</dc:description>
          <dc:identifier>3478193</dc:identifier>
          <dc:identifier>http://hdl.handle.net/2142/23945</dc:identifier>
          <dc:language>en</dc:language>
          <dc:rights>1989 Leonid Sagalovsky</dc:rights>
          <dc:subject>third-order</dc:subject>
          <dc:subject>charged particle</dc:subject>
          <dc:subject>beam optics</dc:subject>
          <dc:subject>power series expansion</dc:subject>
          <dc:subject>transfer matrices</dc:subject>
          <dc:title>Third-order charged particle beam optics</dc:title>
          <dc:type>Dissertation / Thesis</dc:type>
          <dc:type>text</dc:type>
          <degree>
            <department>Physics</department>
            <discipline>Physics</discipline>
            <disciplineCode>University of Illinois at Urbana-Champaign</disciplineCode>
            <level>Dissertation</level>
            <name>Ph.D.</name>
          </degree>
        </thesis>
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