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  <title>NOPR Collection:</title>
  <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/24319" />
  <subtitle />
  <id>http://nopr.niscpr.res.in/handle/123456789/24319</id>
  <updated>2026-10-09T10:03:36Z</updated>
  <dc:date>2026-10-09T10:03:36Z</dc:date>
  <entry>
    <title>X-ray diffraction studies of Ga&lt;sub&gt;2&lt;/sub&gt;Te&lt;sub&gt;3&lt;/sub&gt;</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/24369" />
    <author>
      <name>Singh, D P</name>
    </author>
    <author>
      <name>Khan, M Y</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/24369</id>
    <updated>2013-11-30T16:42:29Z</updated>
    <published>2001-02-01T00:00:00Z</published>
    <summary type="text">Title: X-ray diffraction studies of Ga&lt;sub&gt;2&lt;/sub&gt;Te&lt;sub&gt;3&lt;/sub&gt;
Authors: Singh, D P; Khan, M Y
Abstract: Compound Ga&lt;sub&gt;2&lt;/sub&gt;Te&lt;sub&gt;3&lt;/sub&gt; was&#xD;
prepared from the melt of initial elements of purity &gt; 99.999% and&#xD;
characterized by powder and single crystal techniques of X-ray diffraction&#xD;
analysis. Powder X-ray pattern was obtained up to sin θ/λ =0.634Å&lt;sup&gt;-1&lt;/sup&gt;&#xD;
and indexed. The powder data were corrected and explained on the findings of&#xD;
single crystal, obtained from the polycrystalline&#xD;
&#xD;
ingot. The studies revealed that it&#xD;
crystallized in the cubic form of zinc blende structure with a&lt;sub&gt;o&lt;/sub&gt;=5.8984A,&#xD;
Z= 1.333, space group F43m and &lt;i&gt;D&lt;/i&gt;&lt;sub&gt;x&lt;/sub&gt;&lt;i&gt;=&lt;/i&gt;5.668 g/cc&lt;i&gt;. &lt;/i&gt;Single&#xD;
crystals exhibited the property of cleavage along &lt; 1&lt;img src='http://www.niscair.res.in/jinfo/bar1.gif' border=0&gt;1&gt; and twinning a&#xD;
long &lt; 1&lt;img src='http://www.niscair.res.in/jinfo/bar1.gif' border=0&gt;0 &gt; directions.
Page(s): 46-49</summary>
    <dc:date>2001-02-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Electrical characterization of superionic materials in&lt;b&gt; &lt;/b&gt;the system (Cu&lt;sub&gt;1-x&lt;/sub&gt;Ag&lt;sub&gt;x&lt;/sub&gt;I)-(Ag&lt;sub&gt;2&lt;/sub&gt;O)(P&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;5&lt;/sub&gt;), (0.05 ≤ x ≤ 0.25) for solid state batteries</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/24338" />
    <author>
      <name>Suthanthiraraj, S Austin</name>
    </author>
    <author>
      <name>Murugesan, S</name>
    </author>
    <author>
      <name>Maruthamuthu, P</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/24338</id>
    <updated>2013-12-01T16:42:43Z</updated>
    <published>2001-02-01T00:00:00Z</published>
    <summary type="text">Title: Electrical characterization of superionic materials in&lt;b&gt; &lt;/b&gt;the system (Cu&lt;sub&gt;1-x&lt;/sub&gt;Ag&lt;sub&gt;x&lt;/sub&gt;I)-(Ag&lt;sub&gt;2&lt;/sub&gt;O)(P&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;5&lt;/sub&gt;), (0.05 ≤ x ≤ 0.25) for solid state batteries
Authors: Suthanthiraraj, S Austin; Murugesan, S; Maruthamuthu, P
Abstract: Superionic materials in the system 30(Cu&lt;sub&gt;1-x&lt;/sub&gt;Ag&lt;sub&gt;x&lt;/sub&gt;I)-46.66(Ag&lt;sub&gt;2&lt;/sub&gt;O)-23.33(P&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;5&lt;/sub&gt;),&#xD;
where x = 0.05, 0.1, 0.15, 0.2 and 0.25 respectively, were prepared using the&#xD;
melt quenching process. The electrical conductivity measurements were made in&#xD;
the temperature range 295-445 K by the complex impedance method. The room temperature&#xD;
electrical conductivity values observed for five different samples of the&#xD;
system are found to be of the order of 10&lt;sup&gt;-6&lt;/sup&gt; to 10&lt;sup&gt;-4&lt;/sup&gt; Scm&lt;sup&gt;-1&lt;/sup&gt;.&#xD;
The best conducting composition was found to exhibit an electrical conductivity&#xD;
as high as 1.15×10&lt;sup&gt;-4&lt;/sup&gt; Scm&lt;sup&gt;-1&lt;/sup&gt; at 295 K. From the&#xD;
temperature-dependent conductivity studies, the values of activation energy of&#xD;
these materials are found to be less than 0.5 eV. The ionic transport number (&lt;i&gt;t&lt;/i&gt;&lt;sub&gt;i&lt;/sub&gt;)&lt;i&gt;&#xD;
&lt;/i&gt;values for these materials are found to be greater than 0.96. These&#xD;
measurements confirm the formation of superionic materials in this system and their&#xD;
suitability for battery applications as solid electrolytes.
Page(s): 57-58</summary>
    <dc:date>2001-02-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Microwave absorption study in some iodine doped polyblends</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/24337" />
    <author>
      <name>Meghal, Priya</name>
    </author>
    <author>
      <name>Ubale, Seema</name>
    </author>
    <author>
      <name>Adgaonkar, C S</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/24337</id>
    <updated>2013-11-29T16:44:19Z</updated>
    <published>2001-02-01T00:00:00Z</published>
    <summary type="text">Title: Microwave absorption study in some iodine doped polyblends
Authors: Meghal, Priya; Ubale, Seema; Adgaonkar, C S
Abstract: Dielectric constant (ɛ&lt;i&gt;'&lt;/i&gt;) and&#xD;
dielectric loss (ɛ&lt;i&gt;"&lt;/i&gt;) were determined at a microwave frequency of&#xD;
9.586 GHz (X-band wavelength of 3cm.) for iodine doped polyblends of&#xD;
polystyrene (PS)&#xD;
&#xD;
and polymethylmetha-acrylate(PMMA). These&#xD;
values increased with iodine percentage. This can be attributed to the complex&#xD;
formation in polymer due to iodine doping.
Page(s): 55-56</summary>
    <dc:date>2001-02-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Charge decay and relaxation times in electrets</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/24336" />
    <author>
      <name>Dhaliwal, Amarjit S</name>
    </author>
    <author>
      <name>Mann, K S</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/24336</id>
    <updated>2013-12-02T16:42:19Z</updated>
    <published>2001-02-01T00:00:00Z</published>
    <summary type="text">Title: Charge decay and relaxation times in electrets
Authors: Dhaliwal, Amarjit S; Mann, K S
Abstract: In the present communication, the decay&#xD;
of surface charge density of bees wax and the role of a variety of relaxation&#xD;
times in describing the nature of charge carriers have been studied in&#xD;
&#xD;
detail. Thermo-electrets of bees wax were&#xD;
prepared under different conditions of polarizing field, temperature and time.&#xD;
The results of present investigations show that a single line does not fit the&#xD;
complete exponential decay of the surface charge. The values of decay constants&#xD;
range from 2.0×10&lt;sup&gt;2&lt;/sup&gt; sec to 1.3×10&lt;sup&gt;7&lt;/sup&gt; sec. Due to the&#xD;
presence of a large number of dipoles and ions of different kinds in bees wax,&#xD;
a number of dipole relaxation frequencies are expected.
Page(s): 53-54</summary>
    <dc:date>2001-02-01T00:00:00Z</dc:date>
  </entry>
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