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    <title>NOPR Collection:</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/2242</link>
    <description />
    <items>
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        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/30661" />
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/30660" />
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/30659" />
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/30658" />
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    <dc:date>2026-10-06T19:18:20Z</dc:date>
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  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/30661">
    <title>&lt;i&gt;&lt;span style="mso-bidi-language:HI"&gt;Ab-initio &lt;/span&gt;&lt;/i&gt;&lt;span style="mso-bidi-language: HI"&gt;calculation and B&lt;sub&gt;1&lt;/sub&gt; to B&lt;sub&gt;2&lt;/sub&gt; structural phase transformation in CdO at high pressure &lt;/span&gt;</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/30661</link>
    <description>Title: &lt;i&gt;&lt;span style="mso-bidi-language:HI"&gt;Ab-initio &lt;/span&gt;&lt;/i&gt;&lt;span style="mso-bidi-language: HI"&gt;calculation and B&lt;sub&gt;1&lt;/sub&gt; to B&lt;sub&gt;2&lt;/sub&gt; structural phase transformation in CdO at high pressure &lt;/span&gt;
Authors: Srivastava, Vipul; Sanyal, Sankar P; Rajagopalan, M
Abstract: &lt;span style="mso-bidi-language:HI"&gt;The electronic and structural properties of CdO at&#xD;
high pressure have been studied by using the self-consistent tight binding&#xD;
linear muffin tin orbital method. The relative stabilities of CdO at high&#xD;
pressure in the rock salt and CsCl structures have been examined. The rock-salt&#xD;
structure is found to be the ground state structure of CdO. The phase&#xD;
transition from NaCl (B&lt;sub&gt;1&lt;/sub&gt;)- to CsCl (B&lt;sub&gt;2&lt;/sub&gt;)-type structure&#xD;
for CdO is found to occur at 81.7 GPa, which is close to experimental value&#xD;
90.6 GPa. Calculated lattice parameter and bulk modulus in both the phases are&#xD;
in good agreement with experimental results. The calculated band structure shows&#xD;
a small overlap between the conduction and valence bands with a direct band-gap&#xD;
of ~1.37 eV. A broadening of the upper Cd-4d and O-2p bands with some&#xD;
intermixing between them is observed in total DOS histogram of CdO.&#xD;
&#xD;
&lt;/span&gt;
Page(s): 75-78</description>
    <dc:date>2007-01-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/30660">
    <title>Ion beam modification and analysis of polymer composites</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/30660</link>
    <description>Title: Ion beam modification and analysis of polymer composites
Authors: Qureshi, Anjum; Singh, N L; Somani, Keyur; Rakshit, A K; Singh, F; Avasthi, D K
Abstract: &lt;span style="mso-bidi-language:HI"&gt;Thin films of ferric oxalate dispersed in&#xD;
polyvinyl chloride (PYC) were synthesized. Ferric oxalate was dispersed in PVC&#xD;
films at various concentrations. These films were irradiated with 80MeV &lt;span style="mso-bidi-font-family:Arial;mso-bidi-language:HI"&gt;O&lt;sup&gt;&lt;span style="mso-bidi-language:HI"&gt;6&lt;/span&gt;&lt;/sup&gt;&lt;sup&gt;&lt;span style="mso-bidi-font-family:&#xD;
Arial;mso-bidi-language:HI"&gt;+&lt;/span&gt;&lt;/sup&gt;&lt;span style="mso-bidi-font-family:&#xD;
Arial;mso-bidi-language:HI"&gt; &lt;span style="mso-bidi-language:HI"&gt;ions at&#xD;
a fluence of 1×10&lt;sup&gt;11&lt;/sup&gt; ions/cm&lt;sup&gt;2&lt;/sup&gt;. The radiation induced&#xD;
changes in dielectric properties, microhardness and surface roughness have been&#xD;
studied in the paper. It is observed that hardness and dielectric properties of&#xD;
the film increase with the concentration of dispersed ferric oxalate and also&#xD;
with the fluence. This suggests that ion beam irradiation promotes the metal to&#xD;
polymer adhesion, and converts the polymeric structure into hydrogen depleted&#xD;
carbon network, which make polymer harder and more conductive. Atomic force microscopy&#xD;
shows that the average roughness of the irradiated films is lower than that of&#xD;
un-irradiated films.&#xD;
&#xD;
&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Page(s): 57-61</description>
    <dc:date>2007-01-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/30659">
    <title>&lt;span style="mso-bidi-language:HI"&gt;Dielectric study of Cu&lt;sup&gt;2&lt;/sup&gt;&lt;sup&gt;&lt;span style="mso-bidi-font-family:Arial;mso-bidi-language:HI"&gt;+&lt;/span&gt;&lt;/sup&gt;&lt;span style="mso-bidi-font-family:Arial;mso-bidi-language:HI"&gt; &lt;span style="mso-bidi-language:HI"&gt;doped calcium tartrate tetrahydrate crystals &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/30659</link>
    <description>Title: &lt;span style="mso-bidi-language:HI"&gt;Dielectric study of Cu&lt;sup&gt;2&lt;/sup&gt;&lt;sup&gt;&lt;span style="mso-bidi-font-family:Arial;mso-bidi-language:HI"&gt;+&lt;/span&gt;&lt;/sup&gt;&lt;span style="mso-bidi-font-family:Arial;mso-bidi-language:HI"&gt; &lt;span style="mso-bidi-language:HI"&gt;doped calcium tartrate tetrahydrate crystals &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Authors: Suthar, S R; Joshi, S J; Parekh, B B; Joshi, M J
Abstract: &lt;span style="mso-bidi-language:HI"&gt;Calcium tartrate crystals are well-known for their&#xD;
ferroelectric properties. In the present study, copper doped calcium tartrate&#xD;
tertrahydrate crystals were grown by the single diffusion gel growth technique.&#xD;
The amount of copper doping was confirmed by Induced Condensed Plasma (ICP).&#xD;
The single phase nature was identified by powder XRD. The dielectric measurements&#xD;
were made on pelletized samples in the temperature range 40-160°C and the&#xD;
frequency range 1-500 kHz. The dielectric constant was determined from the&#xD;
value of capacitance. The copper doping showed significant influence on the&#xD;
value of dielectric constant and the transition temperature.&#xD;
&#xD;
&lt;/span&gt;
Page(s): 48-51</description>
    <dc:date>2007-01-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/30658">
    <title>&lt;span style="mso-bidi-language:HI"&gt;Transport, magnetic and thermal properties of La&lt;sub&gt;0.88&lt;/sub&gt;Ca&lt;sub&gt;0.12&lt;/sub&gt;MnO&lt;sub&gt;3 &lt;/sub&gt;single crystal &lt;/span&gt;</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/30658</link>
    <description>Title: &lt;span style="mso-bidi-language:HI"&gt;Transport, magnetic and thermal properties of La&lt;sub&gt;0.88&lt;/sub&gt;Ca&lt;sub&gt;0.12&lt;/sub&gt;MnO&lt;sub&gt;3 &lt;/sub&gt;single crystal &lt;/span&gt;
Authors: Bodhaye, Ashish; Sanyal, Sankar P; Okram, G S; Mukovskii, Y M
Abstract: &lt;span style="mso-bidi-language:HI"&gt;The transport, magnetic and thermal properties of&#xD;
La&lt;sub&gt;0.88&lt;/sub&gt;Ca&lt;sub&gt;0.12&lt;/sub&gt;MnO&lt;sub&gt;3 &lt;/sub&gt;single crystals have been&#xD;
studied using various experimental techniques. The resistivity measurement&#xD;
shows the characteristics of semiconducting behaviour having the resistivity&#xD;
6.9 MΏcm at 90K and 31.5 Ώcm at 296K. There is no resistivity peak or&#xD;
electronic transition over the whole temperature range studied. However, there&#xD;
is a notable change of resistivity at about 115 K, seemingly related to paramagnetic&#xD;
insulator to ferromagnetic insulator transition. The &lt;i&gt;ac &lt;/i&gt;susceptibility&#xD;
measurement confirms that this material shows paramagnetic insulator to ferromagnetic&#xD;
insulator transition with &lt;i&gt;&lt;span style="mso-bidi-font-family:Arial;&#xD;
mso-bidi-language:HI"&gt;T&lt;sub&gt;c&lt;/sub&gt; &lt;/span&gt;&lt;/i&gt;&lt;span style="mso-bidi-font-family:&#xD;
Arial;mso-bidi-language:HI"&gt;= &lt;span style="mso-bidi-language:HI"&gt;117.5&#xD;
K. The sharp peak around the same temperature in the heat capacity measurement&#xD;
indicates the onset of long range ordering.&#xD;
&#xD;
&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Page(s): 37-39</description>
    <dc:date>2007-01-01T00:00:00Z</dc:date>
  </item>
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