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    <title>NOPR Community:</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/8604</link>
    <description />
    <pubDate>Tue, 06 Oct 2026 19:15:41 GMT</pubDate>
    <dc:date>2026-10-06T19:15:41Z</dc:date>
    <item>
      <title>Electrical conduction in potassium boro-vanadate iron glass</title>
      <link>http://nopr.niscpr.res.in/handle/123456789/30650</link>
      <description>Title: Electrical conduction in potassium boro-vanadate iron glass
Authors: Panchal, Harshvadan R; Kanchan, Dinesh K
Abstract: &lt;span style="mso-bidi-language:HI"&gt;The conduction mechanism of &lt;i&gt;&lt;span style="mso-bidi-font-family:Arial;mso-bidi-language:HI"&gt;x&lt;/span&gt;&lt;/i&gt;&lt;span style="mso-bidi-font-family:Arial;mso-bidi-language:HI"&gt;K&lt;sub&gt;2&lt;/sub&gt;O:(100-&lt;i&gt;x&lt;/i&gt;-&lt;i&gt;y&lt;/i&gt;)[(1+&lt;i&gt;n&lt;/i&gt;)V&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;5&lt;/sub&gt;:B&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;3&lt;/sub&gt;&lt;i&gt;&#xD;
&lt;/i&gt;&lt;span style="mso-bidi-language:HI"&gt;where &lt;i&gt;&lt;span style="mso-bidi-font-family:Arial;mso-bidi-language:HI"&gt;x &lt;/span&gt;&lt;/i&gt;&lt;span style="mso-bidi-language:HI"&gt;= 0,5,10,15, 20, &lt;i&gt;&lt;span style="mso-bidi-font-family:&#xD;
Arial;mso-bidi-language:HI"&gt;y &lt;/span&gt;&lt;/i&gt;&lt;span style="mso-bidi-language:HI"&gt;=&#xD;
5, 7.5, 10, 12.5 and 15 and &lt;i&gt;n &lt;/i&gt;= 0.2 to 1 in step of 0.2 had been&#xD;
explained on the basis of Mott's theory. The de conductivity of the present glass&#xD;
system was measured in the temperature range 315-435 K for all the different&#xD;
glass compositions. The decrease of conductivity and increase in activation&#xD;
energy had been observed with the increase of Fe&lt;sub&gt;&lt;span style="mso-bidi-font-family:Arial;mso-bidi-language:HI"&gt;2&lt;/span&gt;&lt;/sub&gt;&lt;span style="mso-bidi-font-family:Arial;mso-bidi-language:HI"&gt;O&lt;sub&gt;3&lt;/sub&gt;&lt;span style="mso-bidi-language:HI"&gt; concentration. Estimated small polaron radius is&#xD;
found to be smaller than the atomic site spacing (V-V spacing) and greater than&#xD;
the radius of iron on which the electron is localized. The present glass system&#xD;
shows a semiconducting adiabatic hopping due to a small polaron.&#xD;
&#xD;
&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Page(s): 137-141</description>
      <pubDate>Tue, 01 Feb 2005 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://nopr.niscpr.res.in/handle/123456789/30650</guid>
      <dc:date>2005-02-01T00:00:00Z</dc:date>
    </item>
    <item>
      <title>Development of a large area telescopic detector system for elastic and transfer reaction angular distribution measurements</title>
      <link>http://nopr.niscpr.res.in/handle/123456789/30648</link>
      <description>Title: Development of a large area telescopic detector system for elastic and transfer reaction angular distribution measurements
Authors: Kalita, K; Jhingan, A; Barua, S; Das, J J; Varughese, T; Sugathan, P; Madhavan, N; Nath, S; Verma, S; Singh, R
Abstract: &lt;span style="mso-bidi-language:HI"&gt;A large area telescopic detector set-up (Δ&lt;i&gt;E-E&lt;/i&gt;)&lt;i&gt;&#xD;
&lt;/i&gt;has been developed for elastic scattering and transfer reaction measurements&#xD;
involving low intensity radioactive ion beam (RIB) at Nuclear Science Centre&#xD;
(NSC), New Delhi.&#xD;
The detector system consists of a transmission type gas ionization chamber (Δ&lt;i&gt;E-E&lt;/i&gt;)&lt;i&gt;&#xD;
&lt;/i&gt;with axial field geometry followed by &lt;i&gt;E-&lt;/i&gt;two-two-dimensional position&#xD;
sensitive silicon detectors (2D-PSSD) placed side by side (50 mm &lt;span style="mso-bidi-font-family:Arial;mso-bidi-language:HI"&gt;× &lt;span style="mso-bidi-language:HI"&gt;50 mm each) for the residual-energy&#xD;
&#xD;
&lt;span style="mso-bidi-language:HI"&gt;measurements. The gas ionization chamber (IC)&#xD;
gives the energy loss of the particles for Z-identification whereas the silicon&#xD;
detectors give their energy as well as the position. The responses of the IC&#xD;
with alpha and fission sources, and of the&#xD;
&#xD;
&lt;span style="mso-bidi-language:HI"&gt;entire detector system with &lt;sup&gt;7&lt;/sup&gt;Be beam&#xD;
are presented which demonstrate the overall performance.&#xD;
&#xD;
&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Page(s): 567-572</description>
      <pubDate>Mon, 01 Aug 2005 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://nopr.niscpr.res.in/handle/123456789/30648</guid>
      <dc:date>2005-08-01T00:00:00Z</dc:date>
    </item>
    <item>
      <title>Effect of metallic substitution on the optical, mechanical and photoconducting properties of L-arginium diphosphate single crystals</title>
      <link>http://nopr.niscpr.res.in/handle/123456789/30647</link>
      <description>Title: Effect of metallic substitution on the optical, mechanical and photoconducting properties of L-arginium diphosphate single crystals
Authors: Pragasam, A Joseph Ami; Selvakumar, S; Madhavan, J; Anand, D Prem; Sagayaraj, P
Abstract: &lt;span style="mso-bidi-language:HI"&gt;L-arginium diphosphate (LADP) is one of the&#xD;
important analogs of LAP crystal. LADP has excellent optical, thermal and&#xD;
mechanical properties, which make it a potential candidate for photonics device&#xD;
fabrication. The present work deals&#xD;
&#xD;
&lt;span style="mso-bidi-language:HI"&gt;with the growth and characterization of metal (Cu&lt;sup&gt;&lt;span style="mso-bidi-font-family:Arial;mso-bidi-language:HI"&gt;2+&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;and Mg&lt;sup&gt;&lt;span style="mso-bidi-font-family:&#xD;
Arial;mso-bidi-language:HI"&gt;2+&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;substituted&#xD;
single crystals of LADP. The grown crystals are subjected to single crystal&#xD;
XRD, AAS, FTIR, DRS spectra and microhardness studies. Microhardness studies&#xD;
indicate that&#xD;
&#xD;
&lt;span style="mso-bidi-language:HI"&gt;the presence of dopant has enhanced the hardness&#xD;
of the material. The photoconductivity study reveals the positive photoconducting&#xD;
nature of both pure and doped crystals.&#xD;
&#xD;
&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Page(s): 463-468</description>
      <pubDate>Wed, 01 Jun 2005 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://nopr.niscpr.res.in/handle/123456789/30647</guid>
      <dc:date>2005-06-01T00:00:00Z</dc:date>
    </item>
    <item>
      <title>Adaptive optics and its applications</title>
      <link>http://nopr.niscpr.res.in/handle/123456789/30645</link>
      <description>Title: Adaptive optics and its applications
Authors: Mohan, D; Mishra, S K; Saha, S K
Abstract: &lt;span style="mso-bidi-language:HI"&gt;The adaptive optics (AO) system combines&#xD;
technologies that enable corrections in real time for the deleterious effects&#xD;
of the atmosphere allowing terrestrial telescopes to achieve their near&#xD;
diffraction-limit. Such a system introduces controllable&#xD;
&#xD;
&lt;span style="mso-bidi-language:HI"&gt;counter wavefront distortions, which both&#xD;
spatially and temporally follow that of the atmosphere. AO system has&#xD;
advantages over post-detection image restoration techniques that are limited by&#xD;
noise and recovers near diffraction-limited images and&#xD;
&#xD;
&lt;span style="mso-bidi-language:HI"&gt;improves the point source sensitivity. This system&#xD;
may become standard tool for the new generation large optical imaging systems.&#xD;
Development of such a technique was made possible due to the significant&#xD;
improvements in technological innovation over the past few decades. After a&#xD;
brief introduction on the deleterious effects of the atmosphere on the image, this&#xD;
article discusses in detail about required components in order to develop the&#xD;
AO system and its applications in various fields, particularly in observational&#xD;
astronomy.&#xD;
&#xD;
&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Page(s): 399-414</description>
      <pubDate>Wed, 01 Jun 2005 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://nopr.niscpr.res.in/handle/123456789/30645</guid>
      <dc:date>2005-06-01T00:00:00Z</dc:date>
    </item>
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