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        <identifier>oai:www.ideals.illinois.edu:2142/25846</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>Anderson, A.C.</dc:contributor>
          <dc:creator>Robichaux, Joseph Emile</dc:creator>
          <dc:date>2011-07-26T19:49:47Z</dc:date>
          <dc:date>2011-07-26T19:49:47Z</dc:date>
          <dc:date>10000-01-01</dc:date>
          <dc:date>1970</dc:date>
          <dc:description>The thermal conductivity was measured in Lanthanum Magnesium Nitrate
(LMN) and Cerium Magnesium Nitrate (CMN) in zero external magnetic field and
was found to be independent of the particular rare-earth ion which occupied
the La site, the concentration of that ion, the thickness of the sample and
the condition of its surfaces. The thermal conductivity, measured both in the
direction perpendicular to that axis, was observed to vary according to a
power of the temperature which lay between 2.8 and 3.0'. It is suggested therefore
that the thermal conductivity in the double nitrate crystals is determined
by an internal scattering mechanism which is approximately independent
of frequency. The phonon mean free paths, calculated in the usual way from
the thermal conductivities of the individual samples, were appreciably greater
than the smallest dimensions of the respective samples.
A depression observed in the thermal conductivity of samples doped
with the non-Kramers rare-earth ions Pr+3 and Ho+3 was determined to be caused
by the resonant scattering of phonons by these ions due to electronic transitions
between the magnetic hyperfine levels. The splitting, in zero external
magnetic field, between the hyperfine levels in the Pr+3 ion inCMN is 0.048 K.
This splitting in the Ho+3 ion inLMN is estimated to be on the order of or
less than 0.03 K.</dc:description>
          <dc:description>Submitted by Carolyn Mead (cmead2@illinois.edu) on 2011-07-26T19:49:47Z
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  Previous issue date: 1970</dc:description>
          <dc:description>Item marked as restricted to the 'UIUC Users [automated]' Group (id=2) by Carolyn Mead (cmead2@illinois.edu) on 2011-07-26T19:49:47Z
Item is restricted indefinitely.</dc:description>
          <dc:description>Restriction data tranferred 2014-07-01T11:33:09-05:00
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>6044267</dc:identifier>
          <dc:identifier>http://hdl.handle.net/2142/25846</dc:identifier>
          <dc:language>en</dc:language>
          <dc:rights>Copyright 1970 Joseph Emile Robichaux, Jr.</dc:rights>
          <dc:subject>thermal conductivity</dc:subject>
          <dc:subject>double nitrate crystals</dc:subject>
          <dc:subject>lanthanum magnesium nitrate</dc:subject>
          <dc:subject>cerium magnesium nitrate</dc:subject>
          <dc:title>The thermal conductivity of double nitrate crystals below 1 K</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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