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<feed xmlns="http://www.w3.org/2005/Atom" xmlns:dc="http://purl.org/dc/elements/1.1/">
  <title>NOPR Collection:</title>
  <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/24327" />
  <subtitle />
  <id>http://nopr.niscpr.res.in/handle/123456789/24327</id>
  <updated>2026-10-09T16:20:17Z</updated>
  <dc:date>2026-10-09T16:20:17Z</dc:date>
  <entry>
    <title>Magnetic properties of Cd and Al substituted cobalt ferrite</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/24471" />
    <author>
      <name>Shitre, A R</name>
    </author>
    <author>
      <name>Devatwal, U N</name>
    </author>
    <author>
      <name>Birajdar, D S</name>
    </author>
    <author>
      <name>Jadhav, K M</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/24471</id>
    <updated>2013-12-10T16:38:17Z</updated>
    <published>2000-10-01T00:00:00Z</published>
    <summary type="text">Title: Magnetic properties of Cd and Al substituted cobalt ferrite
Authors: Shitre, A R; Devatwal, U N; Birajdar, D S; Jadhav, K M
Abstract: &lt;span style="font-size:&#xD;
16.0pt;mso-bidi-font-size:9.0pt;font-family:" times="" new="" roman","serif""=""&gt;The&#xD;
crystal structure and magnetic properties of simultaneously substituted cadmium&#xD;
and aluminium spinel series Co&lt;sub&gt;1-x&lt;/sub&gt;Cd&lt;sub&gt;x&lt;/sub&gt;Fe&lt;sub&gt;2-x&lt;/sub&gt;Al&lt;sub&gt;x&lt;/sub&gt;O&lt;sub&gt;4&lt;/sub&gt;&#xD;
with x=0.0, 0.1, 0.2, 0.3, 0.4 and &lt;i&gt;0.5, &lt;/i&gt;are studied by X-ray diffraction&#xD;
and saturation magnetization measurements. The single phase fcc spinel&#xD;
structure of all the samples was confirmed by X-ray diffraction. X-ray analysis&#xD;
showed that the latticc parameter &lt;i&gt;&lt;span style="font-size:14.5pt;&#xD;
mso-bidi-font-size:7.5pt;font-family:" arial","sans-serif""=""&gt;'a', &lt;/span&gt;&lt;/i&gt;&lt;span style="font-size:16.0pt;mso-bidi-font-size:9.0pt;font-family:" times="" new="" roman","serif""=""&gt;increases&#xD;
with increasing x. The apparent density and X-ray density exhibit similar behaviour.&#xD;
The Bragg peaks of XRD patterns were used to determine the possible cation&#xD;
distribution among the tetrahedral (A) and octahedral rB] sites. X-ray&#xD;
intensity calculations indicate that Cd&lt;sup&gt;&lt;span style="font-size:13.5pt;&#xD;
mso-bidi-font-size:6.5pt;font-family:" times="" new="" roman","serif""=""&gt;2&lt;/span&gt;&lt;/sup&gt;&lt;sup&gt;&lt;span style="font-size:13.0pt;mso-bidi-font-size:6.0pt;font-family:" arial","sans-serif""=""&gt;+&lt;/span&gt;&lt;/sup&gt;&lt;span style="font-size:13.0pt;mso-bidi-font-size:6.0pt;font-family:" arial","sans-serif""=""&gt;&#xD;
&lt;span style="font-size:16.0pt;mso-bidi-font-size:9.0pt;font-family:" times="" new="" roman","serif""=""&gt;and&#xD;
Al&lt;sup&gt;&lt;span style="font-size:13.5pt;mso-bidi-font-size:6.5pt;&#xD;
font-family:" times="" new="" roman","serif""=""&gt;3&lt;/span&gt;&lt;/sup&gt;&lt;sup&gt;&lt;span style="font-size:13.0pt;mso-bidi-font-size:6.0pt;font-family:" arial","sans-serif""=""&gt;+&lt;/span&gt;&lt;/sup&gt;&lt;span style="font-size:13.0pt;mso-bidi-font-size:6.0pt;font-family:" arial","sans-serif""=""&gt;&#xD;
&lt;span style="font-size:16.0pt;mso-bidi-font-size:9.0pt;font-family:" times="" new="" roman","serif""=""&gt;ions&#xD;
occupy tetrahedral (A) and octahedral [B] sites respectively, while Fe&lt;sup&gt;&lt;span style="font-size:13.0pt;mso-bidi-font-size:6.0pt;font-family:" times="" new="" roman","serif""=""&gt;3&lt;/span&gt;&lt;/sup&gt;&lt;sup&gt;&lt;span style="font-size:13.5pt;mso-bidi-font-size:6.5pt;font-family:" arial","sans-serif""=""&gt;+&lt;/span&gt;&lt;/sup&gt;&lt;span style="font-size:13.5pt;mso-bidi-font-size:6.5pt;font-family:" arial","sans-serif""=""&gt;&#xD;
&lt;span style="font-size:16.0pt;mso-bidi-font-size:9.0pt;font-family:" times="" new="" roman","serif""=""&gt;ions&#xD;
occupy both tetrahedral (A) and octahedral [B] sites.&#xD;
&#xD;
&lt;span style="font-size:&#xD;
16.0pt;mso-bidi-font-size:9.0pt;font-family:" times="" new="" roman","serif""=""&gt;&amp;nbsp; The saturation magnetization ‘&lt;span style="font-size:19.0pt;mso-bidi-font-size:12.0pt;font-family:" times="" new="" roman","serif";="" mso-bidi-font-style:italic"=""&gt;σ&lt;sub&gt;s&lt;/sub&gt;’&lt;span style="font-size:16.0pt;&#xD;
mso-bidi-font-size:9.0pt;font-family:" times="" new="" roman","serif""=""&gt;and magneton&#xD;
number 'n&lt;sub&gt;B&lt;/sub&gt;' (the saturation magnetization per formula unit) measured&#xD;
at 300 K using high field hysteresis loop technique decrease with increasing x,&#xD;
suggesting decrease in ferrimagneric behaviour. Neel's two sublattice model is&#xD;
applicable up to x≤ 0.2 while Y-K three sublattice model is applicable for x≥&#xD;
0.2. The cation distribution obtained from magnetization data is in good&#xD;
agreement with the cation distribution estimated from X-ray intensity&#xD;
calculations. The Neel temperature &lt;i&gt;&lt;span style="font-size:15.5pt;&#xD;
mso-bidi-font-size:8.5pt;font-family:" arial","sans-serif""=""&gt;T&lt;sub&gt;N&lt;/sub&gt; &lt;/span&gt;&lt;/i&gt;&lt;span style="font-size:16.0pt;mso-bidi-font-size:9.0pt;font-family:" times="" new="" roman","serif""=""&gt;deduced&#xD;
from a.c. susceptibility data decreases with x, suggesting a decrease in&#xD;
ferrimagnetic behaviour.&lt;span style="font-size:25.0pt;mso-bidi-font-size:&#xD;
11.0pt"&gt;&#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;&lt;/span&gt;&lt;/span&gt;
Page(s): 464-468</summary>
    <dc:date>2000-10-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Life-time measurements of doped zinc sulphide under nitrogen laser excitation</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/24469" />
    <author>
      <name>Bhatti, H S</name>
    </author>
    <author>
      <name>Verma, N K</name>
    </author>
    <author>
      <name>Kumar, Sunil</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/24469</id>
    <updated>2013-12-03T16:39:48Z</updated>
    <published>2000-10-01T00:00:00Z</published>
    <summary type="text">Title: Life-time measurements of doped zinc sulphide under nitrogen laser excitation
Authors: Bhatti, H S; Verma, N K; Kumar, Sunil
Abstract: &lt;span style="font-size:&#xD;
15.0pt;mso-bidi-font-size:8.0pt;font-family:" times="" new="" roman","serif""=""&gt;Excited&#xD;
state lifetime measurements have been carried out for zinc sulphide doped with&#xD;
copper and silver activators having doping concentrations 0.03 to 0.40% by&#xD;
weight using nitrogen laser as the excitation source having pulse-width (10&#xD;
ns), energy per pulse (2 mJ), and pulse repetition rate (50 Hz). The effect of&#xD;
dopant-concentration has been studied at room temperature as well as at liquid&#xD;
nitrogen temperature; the lifetimes are found to remain more or less constant&#xD;
except at room temperature. The decrease in temperature of the sample is found&#xD;
to make its decay faster. &#xD;
&#xD;
&lt;/span&gt;
Page(s): 461-463</summary>
    <dc:date>2000-10-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>&lt;span style="font-size: 21.0pt;mso-bidi-font-size:14.0pt;font-family:"Times New Roman","serif""&gt;Chemical and electronic spectral studies of ullmannite (Ni&lt;sub&gt;&lt;span style="font-size:16.0pt;mso-bidi-font-size:9.0pt;font-family:"Times New Roman","serif""&gt;4&lt;/span&gt;&lt;/sub&gt;&lt;span style="font-size:21.0pt;mso-bidi-font-size:14.0pt;font-family:"Times New Roman","serif""&gt;Sb&lt;sub&gt;&lt;span style="font-size:16.0pt;mso-bidi-font-size:9.0pt;font-family:"Times New Roman","serif""&gt;4&lt;/span&gt;&lt;/sub&gt;&lt;span style="font-size:21.0pt;mso-bidi-font-size:14.0pt;font-family:"Times New Roman","serif""&gt;S&lt;sub&gt;&lt;span style="font-size:16.0pt;mso-bidi-font-size:9.0pt;font-family:"Times New Roman","serif""&gt;4&lt;/span&gt;&lt;/sub&gt;&lt;span style="font-size:16.0pt;mso-bidi-font-size:9.0pt;font-family:"Times New Roman","serif""&gt;) &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/24467" />
    <author>
      <name>Reddy, S N</name>
    </author>
    <author>
      <name>Ravikumar, R V S S N</name>
    </author>
    <author>
      <name>Reddy, B J</name>
    </author>
    <author>
      <name>Reddy, Y P</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/24467</id>
    <updated>2013-12-03T16:39:43Z</updated>
    <published>2000-10-01T00:00:00Z</published>
    <summary type="text">Title: &lt;span style="font-size: 21.0pt;mso-bidi-font-size:14.0pt;font-family:"Times New Roman","serif""&gt;Chemical and electronic spectral studies of ullmannite (Ni&lt;sub&gt;&lt;span style="font-size:16.0pt;mso-bidi-font-size:9.0pt;font-family:"Times New Roman","serif""&gt;4&lt;/span&gt;&lt;/sub&gt;&lt;span style="font-size:21.0pt;mso-bidi-font-size:14.0pt;font-family:"Times New Roman","serif""&gt;Sb&lt;sub&gt;&lt;span style="font-size:16.0pt;mso-bidi-font-size:9.0pt;font-family:"Times New Roman","serif""&gt;4&lt;/span&gt;&lt;/sub&gt;&lt;span style="font-size:21.0pt;mso-bidi-font-size:14.0pt;font-family:"Times New Roman","serif""&gt;S&lt;sub&gt;&lt;span style="font-size:16.0pt;mso-bidi-font-size:9.0pt;font-family:"Times New Roman","serif""&gt;4&lt;/span&gt;&lt;/sub&gt;&lt;span style="font-size:16.0pt;mso-bidi-font-size:9.0pt;font-family:"Times New Roman","serif""&gt;) &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Authors: Reddy, S N; Ravikumar, R V S S N; Reddy, B J; Reddy, Y P
Abstract: &lt;span style="font-size:&#xD;
15.5pt;mso-bidi-font-size:8.5pt;font-family:" times="" new="" roman","serif""=""&gt;The&#xD;
streak grayish black coloured and almost opaque mineral ullmannite belonging to&#xD;
France received from Musee De Mineralogie, Ecole Natle, Supre Des Mines, Paris,&#xD;
France, has been investigated by atomic absorption spectroscopy (AAS) and&#xD;
optical absorption spectroscopy. The AAS analysis shows that the mineral&#xD;
contains the transition elements nickel (1. 14%), iron (0.29%), cobalt&#xD;
(0.073%), copper (0.013%), and manganese (0.003 1 %). The bands observed at&#xD;
25967, 24993, &#xD;
&#xD;
&lt;span style="font-size:&#xD;
15.5pt;mso-bidi-font-size:8.5pt;font-family:" times="" new="" roman","serif""=""&gt;21546,&#xD;
14966, 12252 and 861 8 cm&lt;sup&gt;-1&lt;/sup&gt; in the optical absorption spectrum&#xD;
recorded at room temperature are assigned to different transitions of Ni(lI)&#xD;
ion. The following crystal field parameters are evaluated: &lt;i&gt;&lt;span style="font-size:16.0pt;mso-bidi-font-size:9.0pt;font-family:" times="" new="" roman","serif""=""&gt;Dq&#xD;
&lt;/span&gt;&lt;/i&gt;&lt;span style="font-size:19.5pt;mso-bidi-font-size:12.5pt;font-family:&#xD;
" times="" new="" roman","serif""=""&gt;= &lt;span style="font-size:15.5pt;mso-bidi-font-size:&#xD;
8.5pt;font-family:" times="" new="" roman","serif""=""&gt;860 cm&lt;sup&gt;-1&lt;/sup&gt;, &lt;i&gt;&lt;span style="font-size:16.0pt;mso-bidi-font-size:9.0pt;font-family:" times="" new="" roman","serif""=""&gt;B&#xD;
&lt;/span&gt;&lt;/i&gt;&lt;span style="font-size:19.5pt;mso-bidi-font-size:12.5pt;font-family:&#xD;
" times="" new="" roman","serif""=""&gt;= &lt;span style="font-size:15.5pt;mso-bidi-font-size:&#xD;
8.5pt;font-family:" times="" new="" roman","serif""=""&gt;840 cm&lt;sup&gt;-1&lt;/sup&gt;, and C= 3350&#xD;
cm&lt;sup&gt;-1&lt;/sup&gt;, respectively. These values confirm the octahedral symmetry for&#xD;
Ni(II) in the mineral ullmannite.&#xD;
&#xD;
&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Page(s): 459-460</summary>
    <dc:date>2000-10-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Conductivity and DSC studies of poly(ethylene glycol) and its salt complexes</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/24466" />
    <author>
      <name>Murugendrappa, M V</name>
    </author>
    <author>
      <name>Khasim, Syed</name>
    </author>
    <author>
      <name>Prasad, M V N Ambika</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/24466</id>
    <updated>2013-12-03T16:39:28Z</updated>
    <published>2000-10-01T00:00:00Z</published>
    <summary type="text">Title: Conductivity and DSC studies of poly(ethylene glycol) and its salt complexes
Authors: Murugendrappa, M V; Khasim, Syed; Prasad, M V N Ambika
Abstract: &lt;span style="font-size:&#xD;
15.0pt;mso-bidi-font-size:8.0pt;font-family:" times="" new="" roman","serif""=""&gt;The&#xD;
temperature response of conductivity of poly(ethylene glycol) (PEG) and its&#xD;
salt complexes like KCI, KBr and KI has been studied in the temperature range&#xD;
299 to 331 K. Doping of PEG with KCI and KBr increased the conductivity by about&#xD;
2.5 times for KCI and about 6.25 times for KBr, while doping with KI reduced&#xD;
the conductivity to about 0.05 times its pure component value. This may be due&#xD;
to the presence of dissolved salt in the solid, or alternatively may be due to&#xD;
the changes in the structure of PEG induced by the presence of salt. DSC&#xD;
studies on the samples were carried out wherein a beautiful peak was observed&#xD;
near the melting point. Analysis of DSC results confirms that the reaction is&#xD;
endothermic and the peak shifts towards higher value for different salts as&#xD;
compared to pure PEG.&#xD;
&#xD;
&lt;/span&gt;
Page(s): 456-458</summary>
    <dc:date>2000-10-01T00:00:00Z</dc:date>
  </entry>
</feed>

