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    <title>NOPR Collection:</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/14703</link>
    <description />
    <items>
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        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/14782" />
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/14781" />
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/14780" />
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/14779" />
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    <dc:date>2026-10-12T18:44:43Z</dc:date>
  </channel>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/14782">
    <title>Nanosize dependent electrical and magnetic properties of NiFe&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;4&lt;/sub&gt; ferrite</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/14782</link>
    <description>Title: Nanosize dependent electrical and magnetic properties of NiFe&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;4&lt;/sub&gt; ferrite
Authors: Singh, Sukhdeep; Ralhan, N K; Kotnala, R K; Verma, Kuldeep Chand
Abstract: The effect of&#xD;
nanosize particles on dielectric and magnetic properties of NiFe&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;4&lt;/sub&gt;&#xD;
(NF) ferrite has been studied. NF nanoferrites were prepared by a chemical&#xD;
combustion route followed by annealing temperatures from 400&lt;span style="font-family:Symbol;mso-ascii-font-family:" times="" new="" roman";="" mso-hansi-font-family:"times="" roman";mso-char-type:symbol;mso-symbol-font-family:="" symbol"="" lang="EN-GB"&gt;° to 700&lt;span style="font-family:Symbol;mso-ascii-font-family:&#xD;
" times="" new="" roman";mso-hansi-font-family:"times="" roman";mso-char-type:symbol;="" mso-symbol-font-family:symbol"="" lang="EN-GB"&gt;°C. The &#xD;
X-ray diffraction (XRD) shows minor amorphous behaviour of NF at 400&lt;span style="font-family:Symbol;mso-ascii-font-family:" times="" new="" roman";="" mso-hansi-font-family:"times="" roman";mso-char-type:symbol;mso-symbol-font-family:="" symbol"="" lang="EN-GB"&gt;°C. However, spinel ferrite structure has been observed with higher&#xD;
annealing in the temperature range 500-700&lt;span style="font-family:Symbol;mso-ascii-font-family:" times="" new="" roman";mso-hansi-font-family:="" "times="" roman";mso-char-type:symbol;mso-symbol-font-family:symbol"="" lang="EN-GB"&gt;°C. The average particles size is measured using Debye-Scherer’s&#xD;
relation. The particle's size is also measured by transmission electron&#xD;
microscopy and the average value is at nm scale. Room temperature dielectric&#xD;
properties viz.; dielectric constant (ε) and loss (tanδ) for all the specimens&#xD;
have been studied as a function of applied frequency in the range 100 Hz-20&#xD;
MHz. These studies indicate that the values of &lt;i style="mso-bidi-font-style:&#xD;
normal"&gt;ε&lt;/i&gt; and tanδ depend on the size of particles. The cole-cole plot of&#xD;
impedance spectroscopy has been used to find the grain size and boundary effect&#xD;
on electrical properties of NF nanograins. The magnetic measurements show the&#xD;
value of saturation magnetization (&lt;i style="mso-bidi-font-style:normal"&gt;M&lt;sub&gt;s&lt;/sub&gt;&lt;/i&gt;)&#xD;
is 0.003, 44.95, 38.83, 45.26 emu/g, respectively, observed at 400&lt;span style="font-family:Symbol;mso-ascii-font-family:" times="" new="" roman";="" mso-hansi-font-family:"times="" roman";mso-char-type:symbol;mso-symbol-font-family:="" symbol"="" lang="EN-GB"&gt;°, 500&lt;span style="font-family:Symbol;mso-ascii-font-family:&#xD;
" times="" new="" roman";mso-hansi-font-family:"times="" roman";mso-char-type:symbol;="" mso-symbol-font-family:symbol"="" lang="EN-GB"&gt;°, 600&lt;span style="font-family:Symbol;mso-ascii-font-family:" times="" new="" roman";mso-hansi-font-family:="" "times="" roman";mso-char-type:symbol;mso-symbol-font-family:symbol"="" lang="EN-GB"&gt;° and 700&lt;span style="font-family:Symbol;&#xD;
mso-ascii-font-family:" times="" new="" roman";mso-hansi-font-family:"times="" roman";="" mso-char-type:symbol;mso-symbol-font-family:symbol"="" lang="EN-GB"&gt;°C. &#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;
Page(s): 739-743</description>
    <dc:date>2012-10-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/14781">
    <title>Pressure derivatives of bulk modulus for materials at extreme compression</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/14781</link>
    <description>Title: Pressure derivatives of bulk modulus for materials at extreme compression
Authors: Singh, P K; Dwivedi, A
Abstract: The method based on&#xD;
the calculus of indeterminates for demonstrating that all the physically&#xD;
acceptable equations of state satisfy the identities for the pressure&#xD;
derivatives of bulk modulus of materials at extreme compression, has been&#xD;
developed. The specific examples of the Birch-Murnaghan finite strain equation,&#xD;
the Poirier-Tarantola logarithmic equation, the Rydberg-Vinet potential energy&#xD;
equation, the Keane K-primed equation and the Stacey reciprocal K-primed&#xD;
equation, have been considered. Expressions for the bulk modulus and its&#xD;
pressure derivatives have been derived and reduced to the limit of infinite&#xD;
pressure. The expressions thus obtained are useful for further analysis of&#xD;
higher derivative thermoelastic properties.
Page(s): 734-738</description>
    <dc:date>2012-10-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/14780">
    <title>Interdependence of nano grain size, alloying effects and  magnetic properties of Ni-Cu-Al alloys</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/14780</link>
    <description>Title: Interdependence of nano grain size, alloying effects and  magnetic properties of Ni-Cu-Al alloys
Authors: Karar, N; Srivastava, A K; Kotnala, R K
Abstract: The remarkable&#xD;
modification in physical and magnetic properties of ternary Ni, Cu and Al based&#xD;
ensemble of ball milled nanoparticle alloys and their crystalline shape with&#xD;
grain size and composition has been studied in the present paper. The onset of&#xD;
crystalline changes have been correlated to grain size and alloying content. A&#xD;
sharp decrease in ferromagnetism maintaining the cubic symmetry with grain size&#xD;
and alloying was also revealed. These alloys show two phase transitions, one&#xD;
near room temperature and the other near 80&lt;span style="font-family:Symbol;mso-ascii-font-family:" times="" new="" roman";mso-hansi-font-family:="" "times="" roman";mso-char-type:symbol;mso-symbol-font-family:symbol"="" lang="EN-GB"&gt;°C compared to 200&lt;span style="font-family:Symbol;&#xD;
mso-ascii-font-family:" times="" new="" roman";mso-hansi-font-family:"times="" roman";="" mso-char-type:symbol;mso-symbol-font-family:symbol"="" lang="EN-GB"&gt;°C for&#xD;
similar bulk compositions. Such observations have been explained and their&#xD;
possible usage is being explored.&#xD;
&#xD;
&lt;/span&gt;&lt;/span&gt;
Page(s): 727-733</description>
    <dc:date>2012-10-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/14779">
    <title>&lt;span style="font-size:10.0pt;font-family: "Times New Roman";mso-fareast-font-family:"Times New Roman";mso-bidi-font-family: Mangal;mso-ansi-language:EN-US;mso-fareast-language:EN-US;mso-bidi-language: HI" lang="EN-US"&gt;Molecular structure, vibrational spectra and theoretical NBO, HOMO-LUMO analysis of &lt;i&gt;&lt;span style="font-size:10.0pt;font-family: "Times New Roman";mso-fareast-font-family:OneGulliver-ItalicA;mso-bidi-font-family: Mangal;mso-ansi-language:EN-US;mso-fareast-language:EN-US;mso-bidi-language: HI" lang="EN-US"&gt;N&lt;/span&gt;&lt;/i&gt;&lt;span style="font-size:10.0pt;font-family:"Times New Roman"; mso-fareast-font-family:OneGulliverA;mso-bidi-font-family:Mangal;mso-ansi-language: EN-US;mso-fareast-language:EN-US;mso-bidi-language:HI" lang="EN-US"&gt;-benzoyl glycine&lt;span style="font-size:10.0pt;font-family:"Times New Roman";mso-fareast-font-family: "Times New Roman";mso-bidi-font-family:Mangal;mso-ansi-language:EN-US; mso-fareast-language:EN-US;mso-bidi-language:HI" lang="EN-US"&gt; by DFT and &lt;i style="mso-bidi-font-style:normal"&gt;ab-initio&lt;/i&gt; HF methods&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/14779</link>
    <description>Title: &lt;span style="font-size:10.0pt;font-family: "Times New Roman";mso-fareast-font-family:"Times New Roman";mso-bidi-font-family: Mangal;mso-ansi-language:EN-US;mso-fareast-language:EN-US;mso-bidi-language: HI" lang="EN-US"&gt;Molecular structure, vibrational spectra and theoretical NBO, HOMO-LUMO analysis of &lt;i&gt;&lt;span style="font-size:10.0pt;font-family: "Times New Roman";mso-fareast-font-family:OneGulliver-ItalicA;mso-bidi-font-family: Mangal;mso-ansi-language:EN-US;mso-fareast-language:EN-US;mso-bidi-language: HI" lang="EN-US"&gt;N&lt;/span&gt;&lt;/i&gt;&lt;span style="font-size:10.0pt;font-family:"Times New Roman"; mso-fareast-font-family:OneGulliverA;mso-bidi-font-family:Mangal;mso-ansi-language: EN-US;mso-fareast-language:EN-US;mso-bidi-language:HI" lang="EN-US"&gt;-benzoyl glycine&lt;span style="font-size:10.0pt;font-family:"Times New Roman";mso-fareast-font-family: "Times New Roman";mso-bidi-font-family:Mangal;mso-ansi-language:EN-US; mso-fareast-language:EN-US;mso-bidi-language:HI" lang="EN-US"&gt; by DFT and &lt;i style="mso-bidi-font-style:normal"&gt;ab-initio&lt;/i&gt; HF methods&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Authors: Rui-Zhou, Zhang; Xiao-Hong, Li; Xian-Zhou, Zhang
Abstract: The vibrational&#xD;
frequencies of &lt;span style="mso-fareast-font-family:OneGulliver-ItalicA;&#xD;
mso-bidi-font-style:italic" lang="EN-GB"&gt;N-benzoyl glycine in the ground state have been calculated using&#xD;
density functional method (B3LYP) by using 6-311++G(d,p) basis set. Theoretical vibrational spectra have been interpreted by means of&#xD;
potential energy distribution (PEDs) using MOLVIB program. The equilibrium&#xD;
geometry and the thermodynamic functions of the title compound have been&#xD;
performed at HF/6-31G(d,p)/6-311++G(d,p)&#xD;
and B3LYP/6-31G(d,p)/&#xD;
6-311++G(d,p) levels of theory. A detailed interpretation of the infrared&#xD;
spectra is reported. The theoretical spectrograms for IR and Raman spectra have&#xD;
been constructed. The natural bond orbital analysis has&#xD;
been carried out to explain the charge transfer or delocalization of charge due&#xD;
to the intra-molecular interactions. Energies of the highest occupied molecular&#xD;
orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) have been&#xD;
predicted.&#xD;
&#xD;
&lt;/span&gt;
Page(s): 719-726</description>
    <dc:date>2012-10-01T00:00:00Z</dc:date>
  </item>
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