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    <title>NOPR Community:</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/9010</link>
    <description />
    <pubDate>Mon, 05 Oct 2026 10:52:19 GMT</pubDate>
    <dc:date>2026-10-05T10:52:19Z</dc:date>
    <item>
      <title>Spectroscopic studies of molluscan shells</title>
      <link>http://nopr.niscpr.res.in/handle/123456789/30639</link>
      <description>Title: Spectroscopic studies of molluscan shells
Authors: Konwar, R; Changmai, R; Baruah, G D
Abstract: &lt;span style="mso-bidi-language:HI"&gt;The spectral characteristics of few naturally&#xD;
occurring molluscan shells have been investigated with the help of laser induced&#xD;
fluorescence, X-Rays, absorption and FTIR spectroscopic techniques. The laser&#xD;
induced fluorescence (LIF) or the&#xD;
&#xD;
&lt;span style="mso-bidi-language:HI"&gt;stimulated laser induced fluorescence from&#xD;
molluscan shells exhibits diffuse bands in the region 5860-6350 Ǻ and some discrete&#xD;
bands in the region 5000-5400Ǻ. The fluorescence spectra of different shells&#xD;
are found to be different. The FTlR&#xD;
&#xD;
&lt;span style="mso-bidi-language:HI"&gt;spectra show predominantly the vibrational bands&#xD;
of CaCO&lt;sub&gt;3&lt;/sub&gt;. But there are additional bands, which are not&#xD;
characteristic of CaCO&lt;sub&gt;3&lt;/sub&gt;. The X-ray photograph and iridescence&#xD;
pattern of few shells are presented.&#xD;
&#xD;
&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Page(s): 812-815</description>
      <pubDate>Mon, 01 Nov 2004 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://nopr.niscpr.res.in/handle/123456789/30639</guid>
      <dc:date>2004-11-01T00:00:00Z</dc:date>
    </item>
    <item>
      <title>Blue electroluminescence in organic semiconductors</title>
      <link>http://nopr.niscpr.res.in/handle/123456789/30636</link>
      <description>Title: Blue electroluminescence in organic semiconductors
Authors: Misra, Aparna; Kumar, Lokendra; Kumar, Pankaj; Dhawan, S K; Kamalasanan, M N; Chandra, Subhas
Abstract: &lt;span style="mso-bidi-language:HI"&gt;Light emitting diodes based on organic materials&#xD;
are of considerable interest owing to their attractive characteristics and&#xD;
potential applications in flat panel displays. This paper focuses on some&#xD;
important blue light emitting organic materials.&#xD;
&#xD;
&lt;span style="mso-bidi-language:HI"&gt;Particularly the attention has been paid to the&#xD;
absorption, photoluminescence (PL), electroluminescence (EL) spectra, current-voltage&#xD;
&lt;span style="mso-bidi-font-family:Arial;mso-bidi-language:HI"&gt;(&lt;i&gt;1-&lt;/i&gt;&lt;i&gt;&lt;span style="mso-bidi-language:HI"&gt;V)&lt;/span&gt;&lt;/i&gt;&lt;span style="mso-bidi-language:HI"&gt;&#xD;
and luminescence-voltage &lt;span style="mso-bidi-font-family:Arial;&#xD;
mso-bidi-language:HI"&gt;(&lt;i&gt;L- &lt;/i&gt;&lt;i&gt;&lt;span style="mso-bidi-language:HI"&gt;V&lt;/span&gt;&lt;/i&gt;&lt;span style="mso-bidi-language:HI"&gt;) characteristics of blue light emitting organic&#xD;
semiconductors, as well&#xD;
&#xD;
&lt;span style="mso-bidi-language:HI"&gt;as those of the para-hexaphenyl (PHP). Syntheses&#xD;
of some important blue light emitting materials have also been discussed. Para hexaphenyl (PHP), which was synthesized by the&#xD;
conventional Kovacic method, is one of the important blue light&#xD;
&#xD;
&lt;span style="mso-bidi-language:HI"&gt;emitting π-conjugated oligomers. OLEDs fabricated,&#xD;
using PHP as an emitter, TPD and PBD as the hole transport layer and electron&#xD;
transport layer respectively, gave efficient blue electroluminescence. The&#xD;
photoluminescence (PL) and&#xD;
&#xD;
&lt;span style="mso-bidi-language:HI"&gt;electrolurninescence (EL) of PHP occur at 423 nm,&#xD;
indicating PHP as an excellent blue emitter. This oligomer showed strong&#xD;
absorption peaks at 297 and 318 nm. The devices showed non-linear electrical&#xD;
properties and bright electroluminescence with low turn on voltages (9V). Some&#xD;
of &lt;span style="mso-bidi-font-family:Arial;mso-bidi-language:HI"&gt;our &lt;span style="mso-bidi-language:HI"&gt;most recent work in the development of a variety of&#xD;
blue light emitting devices has been included and discussed in detail.&#xD;
&#xD;
&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Page(s): 793-805</description>
      <pubDate>Mon, 01 Nov 2004 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://nopr.niscpr.res.in/handle/123456789/30636</guid>
      <dc:date>2004-11-01T00:00:00Z</dc:date>
    </item>
    <item>
      <title>Analysis of coupling characteristics of rectangular core optical waveguide coupler</title>
      <link>http://nopr.niscpr.res.in/handle/123456789/30635</link>
      <description>Title: Analysis of coupling characteristics of rectangular core optical waveguide coupler
Authors: Engles, D; Malik, S S
Abstract: &lt;span style="mso-bidi-language:HI"&gt;A theoretical formulism based on the boundary&#xD;
matching technique has been proposed to study the systematic of an asymmetric&#xD;
waveguide coupler. Same formulism is applicable to a symmetric coupler. The&#xD;
equivalent parallel coupling length to account for the coupling in the two&#xD;
S-shaped regions in the input and the output of the coupler is obtained from&#xD;
the coupler geometry and is dealt with more accurately and sensitively in our&#xD;
calculations. No fitting parameter is required for our&#xD;
&#xD;
&lt;span style="mso-bidi-language:HI"&gt;calculation. The calculated characteristics of the&#xD;
asymmetric coupler are very close to those of experimental ones. Our model can&#xD;
aid in the design of diffused channel single mode rectangular core optical&#xD;
waveguide couplers.&#xD;
&#xD;
&lt;/span&gt;&lt;/span&gt;
Page(s): 674-683</description>
      <pubDate>Wed, 01 Sep 2004 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://nopr.niscpr.res.in/handle/123456789/30635</guid>
      <dc:date>2004-09-01T00:00:00Z</dc:date>
    </item>
    <item>
      <title>Crystal and molecular structure of antimony thiourea bromide</title>
      <link>http://nopr.niscpr.res.in/handle/123456789/30633</link>
      <description>Title: Crystal and molecular structure of antimony thiourea bromide
Authors: Shettigar, V; Bhat, S G; Dharmaprakash, S M
Abstract: &lt;span style="mso-bidi-language:HI"&gt;The structure of antimony thiourea bromide hydrate&#xD;
(ATB) with molecular formula Sb[SC(NH&lt;sub&gt;2&lt;/sub&gt;)&lt;sub&gt; 2&lt;/sub&gt;]Br&lt;sub&gt;3&lt;/sub&gt;.H&lt;sub&gt;2&lt;/sub&gt;O&#xD;
has been determined by X-ray single crystal diffraction. ATB crystallizes in&#xD;
the orthorhombic system with the lattice parameters &lt;i&gt;a &lt;/i&gt;= 12.272(3)Ǻ; &lt;i&gt;&lt;span style="mso-bidi-font-family:Arial;mso-bidi-language:HI"&gt;b &lt;/span&gt;&lt;/i&gt;&lt;span style="mso-bidi-language:HI"&gt;=11.675(4)Ǻ; c =18.617(5)Ǻ; the space group is &lt;i&gt;C&lt;/i&gt;mc2&lt;sub&gt;&lt;span style="mso-bidi-font-family:Arial;mso-bidi-language:HI"&gt;1&lt;/span&gt;&lt;/sub&gt;&lt;span style="mso-bidi-font-family:Arial;mso-bidi-language:HI"&gt;, &lt;span style="mso-bidi-language:HI"&gt;Z = 8, and &lt;i&gt;&lt;span style="mso-bidi-font-family:&#xD;
Arial;mso-bidi-language:HI"&gt;D&lt;/span&gt;&lt;/i&gt;&lt;sub&gt;&lt;span style="mso-bidi-font-family:&#xD;
Arial;mso-bidi-language:HI"&gt;c&lt;/span&gt;&lt;/sub&gt;&lt;i&gt;&lt;span style="mso-bidi-font-family:&#xD;
Arial;mso-bidi-language:HI"&gt; &lt;/span&gt;&lt;/i&gt;&lt;span style="mso-bidi-language:HI"&gt;= 2.648Mg/m&lt;sup&gt;3&lt;/sup&gt;&lt;i&gt;.&#xD;
&lt;/i&gt;The final &lt;i&gt;R &lt;/i&gt;= 0.0366 &lt;span style="mso-bidi-font-family:Arial;&#xD;
mso-bidi-language:HI"&gt;(wR = &lt;span style="mso-bidi-language:HI"&gt;0.0914)&#xD;
for 1273 reflections. The asymmetric unit consists of two symmetrically&#xD;
independent halves of a complex Sb[SC(NH&lt;sub&gt;2&lt;/sub&gt;)&lt;sub&gt;2&lt;/sub&gt;]Br&lt;sub&gt;3&lt;/sub&gt;]&#xD;
and one crystal water molecule, which are completed to a complex dimer by the&#xD;
mirror plane of the space group. The whole crystal is found packed in mm2 point&#xD;
group, which is non-centrosymmetric arrangement of atoms. &#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): 581-584</description>
      <pubDate>Sun, 01 Aug 2004 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://nopr.niscpr.res.in/handle/123456789/30633</guid>
      <dc:date>2004-08-01T00:00:00Z</dc:date>
    </item>
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