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        <identifier>oai:www.ideals.illinois.edu:2142/77420</identifier>
        <datestamp>2023-07-11</datestamp>
        <setSpec>col_2142_5131</setSpec>
        <setSpec>col_2142_8859</setSpec>
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        <setSpec>com_2142_8858</setSpec>
        <setSpec>com_2142_234</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:creator>Nienaber, Paul Joseph</dc:creator>
          <dc:date>2015-05-13T15:42:02Z</dc:date>
          <dc:date>2015-05-13T15:42:02Z</dc:date>
          <dc:date>10000-01-01</dc:date>
          <dc:date>1988</dc:date>
          <dc:date>1988</dc:date>
          <dc:description>An experiment run in the $\nu\sb\mu$ line of the Alternating Gradient Synchrotron at the Brookhaven National Laboratory is described, examining production of single $\pi\sp0$ final states in charged-current ($\nu\sb\mu n \to \mu\sp{-}p\pi\sp0$) and neutral-current ($\nu\sb\mu p \to \nu\sb\mu p\pi\sp0$ and $\nu\sb\mu n \to \nu\sb\mu n\pi\sp0$) reactions, observed in a $5{1\over2}$ ton (fiducial volume) detector consisting of aluminum spark chamber modules and plastic scintillation counters. The data sample contains approximately 470,000 beam pulses. The analysis selected for two-shower final states; the $\gamma\gamma$ and $p\gamma\gamma$ mass distributions are shown. The ratio of neutral- to charged-current single $\pi\sp0$ production is examined; and after corrections for efficiency, misidentification, and contamination from higher technology states are made, a value of R$\sp\prime$ = ${\sigma(\nu\sb\mu\ T \to \nu\sb\mu\ T\sp\prime\ \pi\sp0)}\over{2\sigma(\nu\sb\mu\ T \to \mu\sp{-} T\sp{\prime\prime} \pi\sp0)}$ = 0.248 $\pm$ 0.085 (where T is the target nucleus (for this experiment, aluminum) and T$\sp\prime$ and T$\sp{\prime\prime}$ are final target states), is obtained. The value of this ratio can be related to the Weinberg weak-mixing angle $\theta\sb{w}$, yielding a value of sin$\sp2\theta\sb{w}$ = 0.256 $\pm$ 0.156.</dc:description>
          <dc:description>Made available in DSpace on 2015-05-13T15:42:02Z (GMT). No. of bitstreams: 2
license.txt: 4848 bytes, checksum: 96035ab3f5e1c23cc7138a224ce498bd (MD5)
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  Previous issue date: 1988</dc:description>
          <dc:description>Embargo set by: Seth Robbins for item 78631
Lift date: Forever
Reason: Restricted to the U of I community idenfinitely during batch ingest of legacy ETDs</dc:description>
          <dc:description>Restricted to the U of I community idenfinitely during batch ingest of legacy ETDs</dc:description>
          <dc:description>U of I Only</dc:description>
          <dc:description>102 p.</dc:description>
          <dc:description>Thesis (Ph.D.)--University of Illinois at Urbana-Champaign, 1988.</dc:description>
          <dc:identifier>http://hdl.handle.net/2142/77420</dc:identifier>
          <dc:identifier>(UMI)AAI8823214</dc:identifier>
          <dc:language>eng</dc:language>
          <dc:subject>Physics, Elementary Particles and High Energy</dc:subject>
          <dc:title>Single Neutral Pion Production in Charged Current and Neutral Current Neutrino Interactions</dc:title>
          <dc:type>text</dc:type>
          <degree>
            <department>Physics</department>
            <discipline>Physics</discipline>
            <grantor>University of Illinois at Urbana-Champaign</grantor>
            <level>Dissertation</level>
            <name>Ph.D.</name>
          </degree>
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