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  <title>NOPR Collection:</title>
  <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/16808" />
  <subtitle />
  <id>http://nopr.niscpr.res.in/handle/123456789/16808</id>
  <updated>2026-10-12T09:06:58Z</updated>
  <dc:date>2026-10-12T09:06:58Z</dc:date>
  <entry>
    <title>Dielectric relaxation studies of argemone-mexicana oil in pure form and in dilute solution of benzene at different temperatures</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/26414" />
    <author>
      <name>Bansal, A K</name>
    </author>
    <author>
      <name>Singh, P J</name>
    </author>
    <author>
      <name>Sharma, K S</name>
    </author>
    <author>
      <name>Kumar, Satyanshu</name>
    </author>
    <author>
      <name>Kumar, P R</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/26414</id>
    <updated>2014-02-06T16:36:26Z</updated>
    <published>2001-05-01T00:00:00Z</published>
    <summary type="text">Title: Dielectric relaxation studies of argemone-mexicana oil in pure form and in dilute solution of benzene at different temperatures
Authors: Bansal, A K; Singh, P J; Sharma, K S; Kumar, Satyanshu; Kumar, P R
Abstract: Dielectric&#xD;
properties of argemone-mexicana oil have been investigated at various&#xD;
temperatures in pure form and in dilute&#xD;
solution of benzene at 100 kHz, 8.93 GHz and optical frequency of&#xD;
sodium light. The relaxation times and&#xD;
&#xD;
&lt;span style="font-size:14.0pt;line-height:115%;font-family:" times="" new="" roman";="" mso-fareast-font-family:"times="" roman";color:black;mso-ansi-language:en-in;="" mso-fareast-language:en-in;mso-bidi-language:hi"="" lang="EN-IN"&gt;thermodynamical parameters&#xD;
have been determined from the measured data. These parameters are interpreted&#xD;
in terms of molecular and the intramolecular rotations. The present study&#xD;
suggests the existence of both the intra-molecular and overall orientations in&#xD;
the triglyceride molecule of argemone-mexicana oil under investigation. Study&#xD;
of enthalpy of activation (Δ&lt;i&gt;H&lt;/i&gt;&lt;sub&gt;ε&lt;/sub&gt;&lt;i&gt; ,Δ&lt;/i&gt;&lt;i&gt;&lt;span style="font-size:14.0pt;line-height:115%;font-family:" times="" new="" roman";="" mso-fareast-font-family:hiddenhorzocr;color:black;mso-ansi-language:en-in;="" mso-fareast-language:en-in;mso-bidi-language:hi"="" lang="EN-IN"&gt;H&lt;/span&gt;&lt;/i&gt;&lt;sub&gt;&lt;span style="font-size:14.0pt;line-height:115%;font-family:" times="" new="" roman";="" mso-fareast-font-family:hiddenhorzocr;color:black;mso-ansi-language:en-in;="" mso-fareast-language:en-in;mso-bidi-language:hi"="" lang="EN-IN"&gt;η&lt;/span&gt;&lt;/sub&gt;&lt;span style="font-size:14.0pt;line-height:115%;font-family:" times="" new="" roman";="" mso-fareast-font-family:hiddenhorzocr;color:black;mso-ansi-language:en-in;="" mso-fareast-language:en-in;mso-bidi-language:hi"="" lang="EN-IN"&gt;) &lt;span style="font-size:14.0pt;line-height:115%;font-family:" times="" new="" roman";="" mso-fareast-font-family:"times="" roman";color:black;mso-ansi-language:en-in;="" mso-fareast-language:en-in;mso-bidi-language:hi"="" lang="EN-IN"&gt;for dielectric relaxation and&#xD;
viscous flow suggests the existence of solid rotator phase in these &lt;span style="font-size:14.0pt;line-height:115%;font-family:" times="" new="" roman";="" mso-fareast-font-family:hiddenhorzocr;color:black;mso-ansi-language:en-in;="" mso-fareast-language:en-in;mso-bidi-language:hi"="" lang="EN-IN"&gt;molecules.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Page(s): 329-334</summary>
    <dc:date>2001-05-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Micro-detachment studies in paintings using sandwich hologram interferometric techniques</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/26413" />
    <author>
      <name>Kaura, Sushil K</name>
    </author>
    <author>
      <name>Chhachhia, D P</name>
    </author>
    <author>
      <name>K Aggarwal, A K</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/26413</id>
    <updated>2014-02-08T16:35:53Z</updated>
    <published>2001-05-01T00:00:00Z</published>
    <summary type="text">Title: Micro-detachment studies in paintings using sandwich hologram interferometric techniques
Authors: Kaura, Sushil K; Chhachhia, D P; K Aggarwal, A K
Abstract: &lt;span style="font-size:14.0pt;line-height:&#xD;
115%;font-family:" times="" new="" roman";mso-fareast-font-family:"times="" roman";="" color:black;mso-ansi-language:en-in;mso-fareast-language:en-in;mso-bidi-language:="" hi"="" lang="EN-IN"&gt;Hologram interferometric techniques are finding wide-range applications for&#xD;
carrying out non-destructive testing studies that are suitable in different&#xD;
situations. On account of the measuring accuracy of these techniques, they&#xD;
offer a unique application for non-destructive diagnosis of incipient faults or&#xD;
critical damages in precious and ancient artifacts, paintings, sculptures and&#xD;
monuments etc. caused due to environmental effects and aging. Investigations&#xD;
have been carried out by using sandwich hologram interferometric techniques for&#xD;
performing micro-detachment studies in paper paintings pasted and mounted on&#xD;
wooden panel boards. Experimental results achieved have been discussed.&lt;/span&gt;
Page(s): 286-290</summary>
    <dc:date>2001-05-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Singlet excitation energy transfer in tetracene-doped anthracene in thin film organic semiconductor</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/26412" />
    <author>
      <name>Prasad, B</name>
    </author>
    <author>
      <name>Mishra, P K</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/26412</id>
    <updated>2014-02-06T16:36:15Z</updated>
    <published>2001-05-01T00:00:00Z</published>
    <summary type="text">Title: Singlet excitation energy transfer in tetracene-doped anthracene in thin film organic semiconductor
Authors: Prasad, B; Mishra, P K
Abstract: &lt;span style="font-size:14.0pt;line-height:&#xD;
115%;font-family:" times="" new="" roman";mso-fareast-font-family:"times="" roman";="" color:black;mso-ansi-language:en-in;mso-fareast-language:en-in;mso-bidi-language:="" hi"="" lang="EN-IN"&gt;The electroluminescence (EL) spectra of pure and doped crystals appear to&#xD;
resemble with the spectrum in thin film form. The EL spectra of tetracene,&#xD;
anthracene and tetracene-doped ant anthracene in this film form have been&#xD;
reported. But looking at the relative intensity of undoped anthracene  and tetracene &lt;span style="font-size:14.0pt;line-height:115%;font-family:" times="" new="" roman";="" mso-fareast-font-family:hiddenhorzocr;color:black;mso-ansi-language:en-in;="" mso-fareast-language:en-in;mso-bidi-language:hi"="" lang="EN-IN"&gt;bands, it appears &lt;span style="font-size:14.0pt;line-height:115%;font-family:" times="" new="" roman";="" mso-fareast-font-family:"times="" roman";color:black;mso-ansi-language:en-in;="" mso-fareast-language:en-in;mso-bidi-language:hi"="" lang="EN-IN"&gt;that the band of higher&#xD;
intensity of anthracene (host) has been quenched by the dopant and a large part&#xD;
of doped system lies in the green region of the spectrum which is the&#xD;
characteristic emission of the dopant (guest) molecules. i.e., tetracene. The&#xD;
broadening of band for the doped molecule at 550 nm may be considered due to&#xD;
the energy transfer in this system such that the doping quenches the blue emission&#xD;
of host molecule (anthracene) and replaces it with the green emission of the&#xD;
guest molecule (tetracene).The energy band diagram and a scheme for the&#xD;
excitonic reaction kinetics, that agrees very well with experimental results&#xD;
have been constructed. It is apparent from the comparison of brightness waves&#xD;
that the structure of the doped films resembles very much with that of the&#xD;
undoped tetracene films.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Page(s): 321-328</summary>
    <dc:date>2001-05-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Structural study of 2, 4-dichlorobenzanilide-An aromatic substituted amide</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/26411" />
    <author>
      <name>Rajnikant</name>
    </author>
    <author>
      <name>Gupta, Vivek K</name>
    </author>
    <author>
      <name>Dinesh</name>
    </author>
    <author>
      <name>Goswami, B N</name>
    </author>
    <author>
      <name>Sarmah, G K</name>
    </author>
    <author>
      <name>Bhattacharyya, N K</name>
    </author>
    <author>
      <name>Gupta, Rachna</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/26411</id>
    <updated>2014-02-07T16:34:36Z</updated>
    <published>2001-05-01T00:00:00Z</published>
    <summary type="text">Title: Structural study of 2, 4-dichlorobenzanilide-An aromatic substituted amide
Authors: Rajnikant; Gupta, Vivek K; Dinesh; Goswami, B N; Sarmah, G K; Bhattacharyya, N K; Gupta, Rachna
Abstract: The crystal&#xD;
structure of the title compound (C&lt;sub&gt;13&lt;/sub&gt;H&lt;sub&gt;9&lt;/sub&gt;NOCl&lt;sub&gt;2&lt;/sub&gt;)&#xD;
has been determined by X-ray crystallographic techniques. The&#xD;
compound crystallizes in the triclinic space group Pl with unit cell&#xD;
parameters: &lt;i&gt;a &lt;/i&gt;= 9.717(3), &lt;i&gt;b &lt;/i&gt;= 10.104(3), &lt;i&gt;c =&lt;/i&gt;&#xD;
&#xD;
&lt;span style="font-size:14.0pt;line-height:115%;font-family:" times="" new="" roman";="" mso-fareast-font-family:"times="" roman";color:black;mso-ansi-language:en-in;="" mso-fareast-language:en-in;mso-bidi-language:hi"="" lang="EN-IN"&gt;13.636(3) Å, α = 80.36(2), &lt;span style="font-size:14.0pt;line-height:115%;font-family:" times="" new="" roman";="" mso-fareast-font-family:hiddenhorzocr;color:black;mso-ansi-language:en-in;="" mso-fareast-language:en-in;mso-bidi-language:hi"="" lang="EN-IN"&gt;β &lt;span style="font-size:14.0pt;line-height:115%;font-family:" times="" new="" roman";="" mso-fareast-font-family:"times="" roman";color:black;mso-ansi-language:en-in;="" mso-fareast-language:en-in;mso-bidi-language:hi"="" lang="EN-IN"&gt;= 78.20(2), γ = 70.07(2 )&lt;sup&gt;o&lt;/sup&gt;,&#xD;
Z = 4. The structure has been solved by direct methods and refined to &lt;i&gt;R &lt;/i&gt;=&#xD;
0.051 for 3310 observed reflections and &lt;i&gt;wR(F&lt;sup&gt;2&lt;/sup&gt;) &lt;/i&gt;= 0.149. There&#xD;
are two crystallographically independent molecules in the asymmetric unit. In&#xD;
both the molecules, the phenyl rings are planar. The crystal structure is&#xD;
stabilized by van der Waals forces.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Page(s): 313-315</summary>
    <dc:date>2001-05-01T00:00:00Z</dc:date>
  </entry>
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