<?xml version="1.0" encoding="UTF-8"?>
<rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns="http://purl.org/rss/1.0/" xmlns:taxo="http://purl.org/rss/1.0/modules/taxonomy/" xmlns:sy="http://purl.org/rss/1.0/modules/syndication/" xmlns:dc="http://purl.org/dc/elements/1.1/">
  <channel>
    <title>NISCAIR Online Periodicals Repository Collection: IJPAP Vol.49(05) [May 2011]</title>
    <link>http://nopr.niscair.res.in/handle/123456789/11593</link>
    <description />
    <items>
      <rdf:Seq>
        <rdf:li resource="http://nopr.niscair.res.in/handle/123456789/11606" />
        <rdf:li resource="http://nopr.niscair.res.in/handle/123456789/11605" />
        <rdf:li resource="http://nopr.niscair.res.in/handle/123456789/11604" />
        <rdf:li resource="http://nopr.niscair.res.in/handle/123456789/11603" />
      </rdf:Seq>
    </items>
  </channel>
  <textInput>
    <title>The Collection's search engine</title>
    <description>Search the Channel</description>
    <name>search</name>
    <link>http://nopr.niscair.res.in/simple-search</link>
  </textInput>
  <item rdf:about="http://nopr.niscair.res.in/handle/123456789/11606">
    <title>Effect of structural disorder on electrical and magneto transport of La&lt;sub&gt;0.5&lt;/sub&gt;Pr&lt;sub&gt;0.2&lt;/sub&gt;R&lt;sub&gt;0.3&lt;/sub&gt;MnO&lt;sub&gt;3&lt;/sub&gt; (R = Sr and Ba) manganite films</title>
    <link>http://nopr.niscair.res.in/handle/123456789/11606</link>
    <description>Title: Effect of structural disorder on electrical and magneto transport of La&lt;sub&gt;0.5&lt;/sub&gt;Pr&lt;sub&gt;0.2&lt;/sub&gt;R&lt;sub&gt;0.3&lt;/sub&gt;MnO&lt;sub&gt;3&lt;/sub&gt; (R = Sr and Ba) manganite films
&lt;br/&gt;
&lt;br/&gt;Authors: Markna, J H; Solanki, P S; Khachar, U D; Thaker, C M; Rana, D S; Kuberkar, D G
&lt;br/&gt;
&lt;br/&gt;Abstract: The manganite thin&#xD;
films La&lt;sub&gt;0.5&lt;/sub&gt;Pr&lt;sub&gt;0.2&lt;/sub&gt;R&lt;sub&gt;0.3&lt;/sub&gt;MnO&lt;sub&gt;3&lt;/sub&gt; (R = Sr&lt;sup&gt;2+&lt;/sup&gt;&#xD;
and Ba&lt;sup&gt;2+&lt;/sup&gt;) have been studied to understand the effect of A-site&#xD;
cationic size disorder (σ&lt;sub&gt;A&lt;/sub&gt;&lt;sup&gt;2&lt;/sup&gt;) on their electrical and&#xD;
magneto transport properties. Epitaxial thin films of La&lt;sub&gt;0.5&lt;/sub&gt;Pr&lt;sub&gt;0.2&lt;/sub&gt;Sr&lt;sub&gt;0.3&lt;/sub&gt;MnO&lt;sub&gt;3&lt;/sub&gt;&#xD;
(LPSMO) and La&lt;sub&gt;0.5&lt;/sub&gt;Pr&lt;sub&gt;0.2&lt;/sub&gt;Ba&lt;sub&gt;0.3&lt;/sub&gt;MnO&lt;sub&gt;3&lt;/sub&gt;&#xD;
(LPBMO) were synthesized using Pulsed Laser Deposition (PLD) technique with&#xD;
desirable thicknesses of 150 nm. In the present paper, it is shown, how Sr&lt;sup&gt;+2&lt;/sup&gt;&#xD;
and Ba&lt;sup&gt;+2&lt;/sup&gt; substitution at La-site leads to half-metallicity in LPSMO&#xD;
and low temperature resistivity minima in LPBMO films, respectively. It is&#xD;
observed that the resistivity and high field magneto resistance (HFMR) increase&#xD;
to ~ 55% in LPSMO and ~ 95% in LPBMO films with increasing size disorder. The&#xD;
increase in cation size disorder in LPBMO as compared to LPSMO, results in high&#xD;
values of positive and negative temperature coefficient of resistance (TCR) ~&#xD;
59.8%K&lt;sup&gt;−1&lt;/sup&gt; and −55.1% K&lt;sup&gt;−1&lt;/sup&gt;, respectively.
&lt;br/&gt;
&lt;br/&gt;Page(s): 354-359</description>
  </item>
  <item rdf:about="http://nopr.niscair.res.in/handle/123456789/11605">
    <title>Dielectric and electrical properties of K&lt;sub&gt;1−x&lt;/sub&gt;Na&lt;sub&gt;x&lt;/sub&gt;NbO&lt;sub&gt;3&lt;/sub&gt; system</title>
    <link>http://nopr.niscair.res.in/handle/123456789/11605</link>
    <description>Title: Dielectric and electrical properties of K&lt;sub&gt;1−x&lt;/sub&gt;Na&lt;sub&gt;x&lt;/sub&gt;NbO&lt;sub&gt;3&lt;/sub&gt; system
&lt;br/&gt;
&lt;br/&gt;Authors: Uniyal, Manish; Bhatt, S C
&lt;br/&gt;
&lt;br/&gt;Abstract: Dielectric and&#xD;
electrical properties of K&lt;sub&gt;1−x&lt;/sub&gt;Na&lt;sub&gt;x&lt;/sub&gt;NbO&lt;sub&gt;3&lt;/sub&gt; (&lt;i&gt;x&lt;/i&gt;=0,&#xD;
0.2, 0.4) ceramics have been investigated in the temperature range 35-250°C at different frequencies in the range 0.1-1 MHz. The samples have&#xD;
been prepared by the conventional solid-state reaction method and sintering&#xD;
process. It is observed that dielectric constant, loss tangent and electrical&#xD;
conductivity increase with increasing temperature. Near the transition&#xD;
temperature, dielectric constant, loss tangent and electrical conductivity of&#xD;
these samples show anomalous behaviour. All the prepared samples show&#xD;
orthorhombic structure at room temperature.
&lt;br/&gt;
&lt;br/&gt;Page(s): 350-353</description>
  </item>
  <item rdf:about="http://nopr.niscair.res.in/handle/123456789/11604">
    <title>Prediction of effective thermal conductivity of cellular and polymer composites</title>
    <link>http://nopr.niscair.res.in/handle/123456789/11604</link>
    <description>Title: Prediction of effective thermal conductivity of cellular and polymer composites
&lt;br/&gt;
&lt;br/&gt;Authors: Singh, Ramvir; Sharma, P K; Bhoopal, R S; Verma, L S
&lt;br/&gt;
&lt;br/&gt;Abstract: Theoretical&#xD;
expression has been developed to predict effective thermal conductivity (ETC)&#xD;
of cellular and polymer composites considering random flow of heat flux lines.&#xD;
The concept of averaging temperature field within different phases has been&#xD;
used. For heterogeneous materials, the parameter &lt;i style=""&gt;F&lt;/i&gt; has been introduced in place of physical porosity. Due to the&#xD;
randomness of the flux lines in heterogeneous materials, the laws of&#xD;
statistical mechanics have been used to derive the expression in terms of the&#xD;
ratio of thermal conductivity of the constituents and the physical porosity. Expression so obtained for &lt;i style=""&gt;F&lt;/i&gt; is used in the model and it has been&#xD;
found that the predicted results of effective thermal conductivity are quite close to the experimental values. A comparison&#xD;
of the proposed relation with different models has also been made.
&lt;br/&gt;
&lt;br/&gt;Page(s): 344-349</description>
  </item>
  <item rdf:about="http://nopr.niscair.res.in/handle/123456789/11603">
    <title>Synthesis, growth and characterization of copper mercury thiocyanate crystal</title>
    <link>http://nopr.niscair.res.in/handle/123456789/11603</link>
    <description>Title: Synthesis, growth and characterization of copper mercury thiocyanate crystal
&lt;br/&gt;
&lt;br/&gt;Authors: Vijayabhaskarana, B; Arivazhagan, M; Raja, C Ramachandra
&lt;br/&gt;
&lt;br/&gt;Abstract: Synthesis and growth&#xD;
of nonlinear optical copper mercury thiocyanate, CuHg(SCN)&lt;sub&gt;4&lt;/sub&gt; (CMTC)&#xD;
single crystals have been successfully carried out by slow evaporation&#xD;
technique using water and ethanol as solvents with dimensions up to &#xD;
12´8´5 mm&lt;sup&gt;3&lt;/sup&gt;. The grown single&#xD;
crystals have been studied by different characterization techniques in order to&#xD;
know their suitability for various applications. The lattice parameters of the&#xD;
crystal have been obtained by single crystal X-ray diffraction analysis. The&#xD;
presence of functional groups have been identified using FTIR analysis. The&#xD;
thermal stability and thermal decomposition of CMTC crystals have been &amp;nbsp;investigated by using thermo gravimetric&#xD;
analysis and differential thermal analysis. The CMTC crystal exhibits good&#xD;
physio-chemical stability up to 253.8°C. The&#xD;
optical transparency of the grown crystal has been studied by UV-vis-NIR&#xD;
analysis. The lower cutoff wavelength of CMTC crystal occurs at 390 nm and has&#xD;
been discovered as a non linear optical crystal material. The relative second&#xD;
harmonic generation efficiency of the CMTC crystal has been tested by Kurtz -&#xD;
Perry powder technique.
&lt;br/&gt;
&lt;br/&gt;Page(s): 340-343</description>
  </item>
</rdf:RDF>

