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    <title>NISCAIR Online Periodicals Repository Collection: IJPAP Vol.44(12) [December 2006]</title>
    <link>http://nopr.niscair.res.in/handle/123456789/8227</link>
    <description />
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        <rdf:li resource="http://nopr.niscair.res.in/handle/123456789/8400" />
        <rdf:li resource="http://nopr.niscair.res.in/handle/123456789/8399" />
        <rdf:li resource="http://nopr.niscair.res.in/handle/123456789/8391" />
        <rdf:li resource="http://nopr.niscair.res.in/handle/123456789/8390" />
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  <item rdf:about="http://nopr.niscair.res.in/handle/123456789/8400">
    <title>Temperature, current and doping dependence of non-ideality factor for &lt;i style=""&gt;pnp &lt;/i&gt;and &lt;i style=""&gt;npn&lt;/i&gt; punch-through structures</title>
    <link>http://nopr.niscair.res.in/handle/123456789/8400</link>
    <description>Title: Temperature, current and doping dependence of non-ideality factor for &lt;i style=""&gt;pnp &lt;/i&gt;and &lt;i style=""&gt;npn&lt;/i&gt; punch-through structures
&lt;br/&gt;
&lt;br/&gt;Authors: Shah, Khurshed Ahmad; Islam, S S
&lt;br/&gt;
&lt;br/&gt;Abstract: The effect of punch-through in devices is of great importance in&#xD;
electronic industry. In this paper, an efficient, unconditionally stable,&#xD;
simple and accurate method has been presented for solving non-linear transport&#xD;
equations for carriers with appropriate choice of initial values of dependent&#xD;
variables. The methods are so fast that parameter dependence of non-ideality&#xD;
for punch-through structures has been incorporated easily and their specific&#xD;
effects have been determined precisely. The present study reveals that the&#xD;
non-ideality factor decreases with temperature and increases with current and&#xD;
doping concentration of the active region of the device. The relative changes&#xD;
are larger at lower temperatures and more effective at higher impurity density&#xD;
of the active region of the device. This study enables to have better understanding&#xD;
of the punch-through mechanism and design of these devices.
&lt;br/&gt;
&lt;br/&gt;Page(s): 953-958</description>
  </item>
  <item rdf:about="http://nopr.niscair.res.in/handle/123456789/8399">
    <title>Cation distribution in mixed Mg-Mn ferrite systems from X-ray diffraction technique and saturation magnetization</title>
    <link>http://nopr.niscair.res.in/handle/123456789/8399</link>
    <description>Title: Cation distribution in mixed Mg-Mn ferrite systems from X-ray diffraction technique and saturation magnetization
&lt;br/&gt;
&lt;br/&gt;Authors: Kumar, Gagan; Kanthwal, Meenakshi; Chauhan, B S; Singh, M
&lt;br/&gt;
&lt;br/&gt;Abstract: Ferrites with general formula Mg&lt;sub&gt;0.9&lt;/sub&gt; Mn&lt;sub&gt;0.1&lt;/sub&gt; Fe&lt;sub&gt;2-x&lt;/sub&gt;&#xD;
In&lt;sub&gt;x&lt;/sub&gt; O&lt;sub&gt;4&lt;/sub&gt;, Mg&lt;sub&gt;0.9&lt;/sub&gt; Mn&lt;sub&gt;0.1&lt;/sub&gt; Fe&lt;sub&gt;2-y&lt;/sub&gt;&#xD;
Al&lt;sub&gt;y&lt;/sub&gt; O&lt;sub&gt;4&lt;/sub&gt; and Mg&lt;sub&gt;0.9&lt;/sub&gt; Mn&lt;sub&gt;0.1&lt;/sub&gt; Al&lt;sub&gt;0.3&lt;/sub&gt;&#xD;
Co&lt;sub&gt;z&lt;/sub&gt; Fe&lt;sub&gt;1.7-z&lt;/sub&gt; O­&lt;sub&gt;4&lt;/sub&gt; (where &lt;i style=""&gt;x&lt;/i&gt;, &lt;i style=""&gt;y&lt;/i&gt; = 0.0, 0.1, 0.3, 0.5&#xD;
and &lt;i style=""&gt;z&lt;/i&gt;=0.3, 0.5, 0.7) were prepared by&#xD;
citrate precursor technique and studied by means of X-ray diffraction and&#xD;
saturation magnetization. The X-ray analysis confirmed the single-phase&#xD;
formation of the sample. The cation distribution is inferred from the results&#xD;
of X-ray diffraction and magnetization measurements.
&lt;br/&gt;
&lt;br/&gt;Page(s): 930-934</description>
  </item>
  <item rdf:about="http://nopr.niscair.res.in/handle/123456789/8391">
    <title>Ultrasonic velocities and refractive indices of binary mixtures of propylene carbonate + &lt;i style=""&gt;n&lt;/i&gt;-alkanols</title>
    <link>http://nopr.niscair.res.in/handle/123456789/8391</link>
    <description>Title: Ultrasonic velocities and refractive indices of binary mixtures of propylene carbonate + &lt;i style=""&gt;n&lt;/i&gt;-alkanols
&lt;br/&gt;
&lt;br/&gt;Authors: Wankhede, D S; Wankhede, N N; Lande, M K; Arbad, B R
&lt;br/&gt;
&lt;br/&gt;Abstract: The densities, ultrasonic velocities and&#xD;
refractive indices of binary mixtures of propylene carbonate + ethanol, &lt;i style=""&gt;n&lt;/i&gt;-propanol and &lt;i style=""&gt;n&lt;/i&gt;-butanol at 298.15, 303.15 and 308.15 K have been measured over&#xD;
the whole mole fraction range. Experimental data have been used to estimate the&#xD;
isentropic compressibility (&lt;i style=""&gt;K&lt;sub&gt;s&lt;/sub&gt;&lt;/i&gt;),&#xD;
intermolecular free length (&lt;i style=""&gt;L&lt;sub&gt;f&lt;/sub&gt;&lt;/i&gt;),&#xD;
specific acoustic impedance (&lt;i style=""&gt;Z&lt;/i&gt;),&#xD;
polarizability (&lt;img src='/image/spc_char/alpha.gif' border=0&gt; ) and their deviations excess isentropic compressibility (&lt;i style=""&gt;K&lt;sub&gt;s&lt;/sub&gt;&lt;sup&gt;E&lt;/sup&gt;&lt;/i&gt;), excess&#xD;
intermolecular free length (&lt;i style=""&gt;L&lt;sub&gt;f&lt;/sub&gt;&lt;sup&gt;E&lt;/sup&gt;&lt;/i&gt;),&#xD;
excess acoustic impedance (&lt;i style=""&gt;Z&lt;sup&gt;E&lt;/sup&gt;&lt;/i&gt;)&#xD;
and excess refractive index (&lt;i style=""&gt;&lt;img src='/image/spc_char/delta.gif' border=0&gt;n&lt;sub&gt;D&lt;/sub&gt;&lt;/i&gt;). The results have been fitted to Redlich-Kister equation and&#xD;
discussed in terms of molecular interactions.
&lt;br/&gt;
&lt;br/&gt;Page(s): 909-916</description>
  </item>
  <item rdf:about="http://nopr.niscair.res.in/handle/123456789/8390">
    <title>Compensation effect of &lt;i style=""&gt;ac &lt;/i&gt;conduction in Se&lt;sub&gt;80&lt;/sub&gt;Te&lt;sub&gt;20 &lt;/sub&gt;and Se&lt;sub&gt;80&lt;/sub&gt;Te&lt;sub&gt;10&lt;/sub&gt;M&lt;sub&gt;10&lt;/sub&gt; (M = Cd, In, Sb) chalcogenide glasses</title>
    <link>http://nopr.niscair.res.in/handle/123456789/8390</link>
    <description>Title: Compensation effect of &lt;i style=""&gt;ac &lt;/i&gt;conduction in Se&lt;sub&gt;80&lt;/sub&gt;Te&lt;sub&gt;20 &lt;/sub&gt;and Se&lt;sub&gt;80&lt;/sub&gt;Te&lt;sub&gt;10&lt;/sub&gt;M&lt;sub&gt;10&lt;/sub&gt; (M = Cd, In, Sb) chalcogenide glasses
&lt;br/&gt;
&lt;br/&gt;Authors: Mehta, N; Kumar, D; Kumar, A
&lt;br/&gt;
&lt;br/&gt;Abstract: In many amorphous&#xD;
and liquid semiconductors and other class of materials, Meyer-Neldel rule is&#xD;
observed in the &lt;i style=""&gt;dc&lt;/i&gt; conductivity,&#xD;
where the pre-exponential factor (σ&lt;sub&gt;0&lt;/sub&gt;) is found to increase exponentially with the activation energy (Δ&lt;i style=""&gt;E&lt;/i&gt;). In the present paper, the observation of Meyer- Neldel rule in&#xD;
case of &lt;i style=""&gt;ac&lt;/i&gt; conductivity near the room&#xD;
temperature in bulk samples of Se&lt;sub&gt;80&lt;/sub&gt;Te&lt;sub&gt;20&lt;/sub&gt; and Se&lt;sub&gt;80&lt;/sub&gt;Te&lt;sub&gt;10&lt;/sub&gt;M&lt;sub&gt;10&lt;b style=""&gt; &lt;/b&gt;&lt;/sub&gt;(M = Cd, In, Sb) chalcogenide&#xD;
glasses has been reported.
&lt;br/&gt;
&lt;br/&gt;Page(s): 935-938</description>
  </item>
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