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        <identifier>oai:www.ideals.illinois.edu:2142/23967</identifier>
        <datestamp>2023-07-10</datestamp>
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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>Nishijima, K.</dc:contributor>
          <dc:creator>Cawley, Robert Gerald</dc:creator>
          <dc:date>2011-05-19T15:59:55Z</dc:date>
          <dc:date>2011-05-19T15:59:55Z</dc:date>
          <dc:date>10000-01-01</dc:date>
          <dc:date>1965</dc:date>
          <dc:description>"A set of coupled inhomogeneous integral equations is found
for the imaginary parts of the four invariant amplitudes of
the anomalous deuteron vertex. The equations are algebraically
homogeneous~ however, so the possibility of an eigenvalue con=
\
dition exists if unsubtracted dispersion relations are
postulatedo The anomalous region is treated by means of a
modification of the Nishijima continuation procedure. The
equations are derived in a one pion model to illustrate the
method. A partial diagrammatic analysis of the deuteron vertex
is performed below the normal threshold o So = {M+~)2o
In the second part a proof is given that the propagator
normalization of a scalar or a vector particle is equivalent
to the normalization of its electromagnetic form fqctoro
The basis for the proof is the Ward identityo This permits
a direct comparison of the two normalization conditions and
this is done in lowest approximation for two scalar deuteron
models and for the vector case as welL The normalization of
the deuteron vertex is computed from the triangl,e·graph
apprbximation to the deuteron ·electromagnet:i.c form factor.
, I . This result is. inserted into the eXJ?ansion arising from the·
dispersion relatio~ for' the inverse deuteron propagator at
infinity, and an approximation to the deuteron field operator
renormalization constant Z is thereby found. The result in
each of the scalar models is Z = O. The vector case is more
,
sensitive to the form factors which enter 'in, but in a model
which is in spirit comparable to the scalar examples yields
Z =: o.
An independent argument for Z = 0 for a vector field
is advanced when no zero"":mass scalar particles are present."</dc:description>
          <dc:description>Submitted by Carolyn Mead (cmead2@illinois.edu) on 2011-05-19T15:59:55Z
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  Previous issue date: 1965</dc:description>
          <dc:description>Item marked as restricted to the 'UIUC Users [automated]' Group (id=2) by Carolyn Mead (cmead2@illinois.edu) on 2011-05-19T15:59:55Z
Item is restricted indefinitely.</dc:description>
          <dc:description>Restriction data tranferred 2014-07-01T11:14:01-05:00
Original Data
Group with Access UIUC Users [automated]
Release Date: none
Reason: Thesis</dc:description>
          <dc:description>Thesis</dc:description>
          <dc:description>U of I Only</dc:description>
          <dc:identifier>6199209</dc:identifier>
          <dc:identifier>http://hdl.handle.net/2142/23967</dc:identifier>
          <dc:language>en</dc:language>
          <dc:rights>1965 Robert Gerald Cawley</dc:rights>
          <dc:subject>coupled inhomogeneous integral equations</dc:subject>
          <dc:subject>anomalous deutron vertex</dc:subject>
          <dc:subject>normalization conditions</dc:subject>
          <dc:subject>eigenvalue condition</dc:subject>
          <dc:subject>Nishijima continuation</dc:subject>
          <dc:title>An integral equation for the anomalous deuteron vertex and a comparison of two normalization conditions</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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