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  <title>NOPR Collection:</title>
  <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/12586" />
  <subtitle />
  <id>http://nopr.niscpr.res.in/handle/123456789/12586</id>
  <updated>2026-10-12T21:24:15Z</updated>
  <dc:date>2026-10-12T21:24:15Z</dc:date>
  <entry>
    <title>Temperature dependence of antiferroeletric mode frequency, dielectric constant and loss tangent in deuterated squaric acid crystal</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/12595" />
    <author>
      <name>Upadhyay, Trilok Chandra</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/12595</id>
    <updated>2016-07-20T05:09:29Z</updated>
    <published>2011-09-01T00:00:00Z</published>
    <summary type="text">Title: Temperature dependence of antiferroeletric mode frequency, dielectric constant and loss tangent in deuterated squaric acid crystal
Authors: Upadhyay, Trilok Chandra
Abstract: By fitting model&#xD;
values of physical quantities for deuterated SQA crystal in theoretically&#xD;
derived expression for AFE mode frequency, dielectric entrant and loss tangent&#xD;
in my earlier paper [&lt;i&gt;Indian J Pure &amp;amp; Appl Phys, &lt;/i&gt;47 (2009) 119]&#xD;
temperature dependence of these quantities have been calculated and compared&#xD;
with experimental data of Maier &lt;i&gt;et al., &lt;/i&gt;&lt;i style=""&gt;Phys Status Solidi (b), &lt;/i&gt;89 (1978) 578 and Semmingsen, D&lt;i style=""&gt;, Acta Chem Scand&lt;/i&gt;, 27 (1977) 3961, which&#xD;
show a good agreement.
Page(s): 633-636</summary>
    <dc:date>2011-09-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Specific heat jump and transition temperature &lt;i&gt;T&lt;/i&gt;&lt;sub&gt;C &lt;/sub&gt;for La&lt;sub&gt;2&lt;/sub&gt;&lt;sub&gt;-x&lt;/sub&gt;Ba&lt;sub&gt;x&lt;/sub&gt;CuO&lt;sub&gt;4&lt;/sub&gt;, Bi&lt;sub&gt;2&lt;/sub&gt;Ca&lt;sub&gt;n&lt;/sub&gt;&lt;sub&gt;-1&lt;/sub&gt;Sr&lt;sub&gt;n&lt;/sub&gt;Cu&lt;sub&gt;n&lt;/sub&gt;O&lt;sub&gt;2n+3 &lt;/sub&gt;and Tl&lt;sub&gt;2&lt;/sub&gt;Ca&lt;sub&gt;n&lt;/sub&gt;&lt;sub&gt;-1&lt;/sub&gt;Ba&lt;sub&gt;2&lt;/sub&gt;Cu&lt;sub&gt;n&lt;/sub&gt;O&lt;sub&gt;2n+3(2n+4)&lt;/sub&gt; superconductors</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/12594" />
    <author>
      <name>Nyawere, P W Otieno</name>
    </author>
    <author>
      <name>Khanna, KM</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/12594</id>
    <updated>2016-07-20T05:08:33Z</updated>
    <published>2011-09-01T00:00:00Z</published>
    <summary type="text">Title: Specific heat jump and transition temperature &lt;i&gt;T&lt;/i&gt;&lt;sub&gt;C &lt;/sub&gt;for La&lt;sub&gt;2&lt;/sub&gt;&lt;sub&gt;-x&lt;/sub&gt;Ba&lt;sub&gt;x&lt;/sub&gt;CuO&lt;sub&gt;4&lt;/sub&gt;, Bi&lt;sub&gt;2&lt;/sub&gt;Ca&lt;sub&gt;n&lt;/sub&gt;&lt;sub&gt;-1&lt;/sub&gt;Sr&lt;sub&gt;n&lt;/sub&gt;Cu&lt;sub&gt;n&lt;/sub&gt;O&lt;sub&gt;2n+3 &lt;/sub&gt;and Tl&lt;sub&gt;2&lt;/sub&gt;Ca&lt;sub&gt;n&lt;/sub&gt;&lt;sub&gt;-1&lt;/sub&gt;Ba&lt;sub&gt;2&lt;/sub&gt;Cu&lt;sub&gt;n&lt;/sub&gt;O&lt;sub&gt;2n+3(2n+4)&lt;/sub&gt; superconductors
Authors: Nyawere, P W Otieno; Khanna, KM
Abstract: The transition&#xD;
temperature &lt;i style=""&gt;T&lt;/i&gt;&lt;sub&gt;C&lt;/sub&gt; and the&#xD;
specific heat jump ∆&lt;i style=""&gt;C&lt;/i&gt;/&lt;i style=""&gt;T&lt;sub&gt;C&lt;/sub&gt;&lt;/i&gt; in La&lt;sub&gt;2&lt;/sub&gt;&lt;sub&gt;-x&lt;/sub&gt;Ba&lt;sub&gt;x&lt;/sub&gt;CuO&lt;sub&gt;4, &lt;/sub&gt;Bi&lt;sub&gt;2&lt;/sub&gt;Ca&lt;sub&gt;n&lt;/sub&gt;&lt;sub&gt;-1&lt;/sub&gt;Sr&lt;sub&gt;n&lt;/sub&gt;Cu&lt;sub&gt;n&lt;/sub&gt;O&lt;sub&gt;2n+4&lt;/sub&gt;&#xD;
and Tl&lt;sub&gt;2&lt;/sub&gt;Ca&lt;sub&gt;n&lt;/sub&gt;&lt;sub&gt;-1&lt;/sub&gt;Ba&lt;sub&gt;2&lt;/sub&gt;Cu&lt;sub&gt;n&lt;/sub&gt;O&lt;sub&gt;2n+3(2n+4)&lt;/sub&gt; are calculated&#xD;
using exotic pairing model. These values are calculated at both buckling mode&#xD;
and breathing mode. The values calculated are compared with known experimental&#xD;
values. If ∆ is the gap in the allowed energy states, then the jump in the&#xD;
specific heat is C&lt;sub&gt;S&lt;/sub&gt;-C&lt;sub&gt;n&lt;/sub&gt;.&#xD;
These results show that the calculated values of the ratios and &lt;i style=""&gt;T&lt;/i&gt;&lt;sub&gt;C&lt;/sub&gt; compare well with&#xD;
experimental values.
Page(s): 627-632</summary>
    <dc:date>2011-09-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Study of electronic and optical properties of Sc-, Y-, Ti-doped transparent conducting oxide</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/12593" />
    <author>
      <name>Sharma, Yamini</name>
    </author>
    <author>
      <name>Srivastava, Pankaj</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/12593</id>
    <updated>2016-07-20T05:14:08Z</updated>
    <published>2011-09-01T00:00:00Z</published>
    <summary type="text">Title: Study of electronic and optical properties of Sc-, Y-, Ti-doped transparent conducting oxide
Authors: Sharma, Yamini; Srivastava, Pankaj
Abstract: Transparent&#xD;
conducting oxides have important applications as optoelectronic devices. First&#xD;
principles calculations have been performed to study the electronic and optical&#xD;
properties of Sc-, Y- and Ti-doped transparent conducting oxide (TCO) material CdO. The dielectric functions,&#xD;
absorption coefficients and transmittance spectra have been computed to study&#xD;
the effect of doping. The density of states have also been investigated to&#xD;
interpret the calculated optical spectra in terms of inter band transitions.&#xD;
The valence electron charge density is plotted to understand the redistribution&#xD;
of charges on introduction of transition metal ions. The electrical conductivity&#xD;
and Hall coefficient have also been calculated. The calculated band gap for&#xD;
pure CdO which is 0.51 eV increases significantly with doping. The band gaps&#xD;
for Sc-, Y- and Ti- doped CdO are 2.67, 2.83 and 2.53 eV, respectively, which are&#xD;
in good agreement with experimental measurements.
Page(s): 619-626</summary>
    <dc:date>2011-09-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Characterization of cold atomic cloud in a magneto-optical trap</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/12592" />
    <author>
      <name>Arora, Poonam</name>
    </author>
    <author>
      <name>Chowdhury, Swatilekha</name>
    </author>
    <author>
      <name>Agarwal, Ashish</name>
    </author>
    <author>
      <name>Pant, Kavindra</name>
    </author>
    <author>
      <name>Gupta, Amitava Sen</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/12592</id>
    <updated>2016-07-20T05:09:28Z</updated>
    <published>2011-09-01T00:00:00Z</published>
    <summary type="text">Title: Characterization of cold atomic cloud in a magneto-optical trap
Authors: Arora, Poonam; Chowdhury, Swatilekha; Agarwal, Ashish; Pant, Kavindra; Gupta, Amitava Sen
Abstract: The results of&#xD;
characterization of cold cloud of cesium (Cs) atoms trapped in a&#xD;
magneto-optical trap (MOT) have been presented. The MOT is a part of the&#xD;
Physics package of the Cs Fountain Clock being developed at National Physical&#xD;
Laboratory (NPL), India.&#xD;
The number of atoms, size and temperature of the cloud have been measured and&#xD;
calculated. It is also been investigated how the number of trapped atoms&#xD;
changes with the trapping laser’s beam intensity, detuning and magnetic-field&#xD;
gradient of the trap.
Page(s): 590-595</summary>
    <dc:date>2011-09-01T00:00:00Z</dc:date>
  </entry>
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