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        <identifier>oai:www.ideals.illinois.edu:2142/23910</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:subject>FNAL Tevatron</dc:subject>
          <dc:title>Production of charm mesons by high energy neutrons</dc:title>
          <dc:type>Dissertation / Thesis</dc:type>
          <dc:type>text</dc:type>
          <dc:contributor>Wiss, J.E.</dc:contributor>
          <dc:creator>Shipbaugh, Calvin Leroy</dc:creator>
          <dc:date>2011-05-17T15:17:12Z</dc:date>
          <dc:date>2011-05-17T15:17:12Z</dc:date>
          <dc:date>10000-01-01</dc:date>
          <dc:date>1988</dc:date>
          <dc:description>"The charmed mesons D""'±, DO, and D; have been observed in neutron-nucleus collisions at the FNAL Tevatron. A sample of 134 ± 19 events was investigated in the decay D""'±-+ D°1r± with the subsequent decay mode D°-+ K+ K-. The cross section per nucleon for D""'±, at most probable energy ...;s = 35 GeV, was measured to be:
d:(xf) . BR = 2.11 ± .43 (±.63)JLb/nucleon
Xf
for 0.0 &lt; x f &lt; 0.14 (xf = .07). The branching ratio (BR) is defined as: BR =BR(D'"" -+ D1r) x BR(D -+ K+ K-). The dependence of the cross section per nucleus on number of nucleons in the target was fit to a form A a and it was found that a = .96 .17. A sample of 64 ±.16 D; events was investigated for the decay D; -+ 4&gt;1r±. The differential cross section for D; production averaged over the particle and antiparticle states is:
1 (dO'(D+) dO'(D-»)
BR· ""2 dx fS + dx / = 2.85 ± 0.80 ± .86 JLb/nucleon at x f = 0.175 where the first error is statistical and the second error is systematic. The branching fraction is defined as BR =BR(Ds -+ 4&gt;n'), and a linear A dependence was assumed."</dc:description>
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  Previous issue date: 1988</dc:description>
          <dc:description>Item marked as restricted to the 'UIUC Users [automated]' Group (id=2) by Carolyn Mead (cmead2@illinois.edu) on 2011-05-17T15:17:12Z
Item is restricted indefinitely.</dc:description>
          <dc:description>Restriction data tranferred 2014-07-01T11:13:42-05:00
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>3478307</dc:identifier>
          <dc:identifier>http://hdl.handle.net/2142/23910</dc:identifier>
          <dc:language>en</dc:language>
          <dc:rights>1988 Calvin Leroy Shipbaugh</dc:rights>
          <dc:subject>charm mesons</dc:subject>
          <dc:subject>high energy neutrons</dc:subject>
          <dc:subject>neutron-nucleus collisions</dc:subject>
          <degree>
            <department>Physics</department>
            <discipline>Physics</discipline>
            <disciplineCode>University of Illinois at Urbana-Champaign</disciplineCode>
            <level>Dissertation</level>
            <name>Ph.D.</name>
          </degree>
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