<?xml version="1.0" encoding="UTF-8"?>
<rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns="http://purl.org/rss/1.0/" xmlns:taxo="http://purl.org/rss/1.0/modules/taxonomy/" xmlns:sy="http://purl.org/rss/1.0/modules/syndication/" xmlns:dc="http://purl.org/dc/elements/1.1/">
  <channel>
    <title>NISCAIR Online Periodicals Repository Collection: IJPAP Vol.48(04) [April 2010]</title>
    <link>http://nopr.niscair.res.in/handle/123456789/7627</link>
    <description />
    <items>
      <rdf:Seq>
        <rdf:li resource="http://nopr.niscair.res.in/handle/123456789/7650" />
        <rdf:li resource="http://nopr.niscair.res.in/handle/123456789/7649" />
        <rdf:li resource="http://nopr.niscair.res.in/handle/123456789/7648" />
        <rdf:li resource="http://nopr.niscair.res.in/handle/123456789/7647" />
      </rdf:Seq>
    </items>
  </channel>
  <textInput>
    <title>The Collection's search engine</title>
    <description>Search the Channel</description>
    <name>search</name>
    <link>http://nopr.niscair.res.in/simple-search</link>
  </textInput>
  <item rdf:about="http://nopr.niscair.res.in/handle/123456789/7650">
    <title>High input impedance voltage mode universal biquad filter</title>
    <link>http://nopr.niscair.res.in/handle/123456789/7650</link>
    <description>Title: High input impedance voltage mode universal biquad filter
&lt;br/&gt;
&lt;br/&gt;Authors: Kumar, K; Pal, K
&lt;br/&gt;
&lt;br/&gt;Abstract: A high input impedance voltage mode universal&#xD;
biquad filter using two operational transconductance amplifiers (OTAs), one&#xD;
current feedback amplifier (CFA), two capacitors and one grounded resistor has&#xD;
been studied. The new circuit has three inputs and single output and can&#xD;
realize all the standard filter functions, that is low pass (LP), high pass&#xD;
(HP), band pass (BP), notch (NH), and all pass (AP) filters without changing&#xD;
the circuit topology. The proposed circuit offers several advantages such as&#xD;
orthogonal controllability of the resonance frequency w&lt;sub&gt;0 &lt;/sub&gt;and quality factor &lt;i&gt;Q&lt;/i&gt;. There&#xD;
is no need of one more active element for the realization of all pass filter,&#xD;
high input impedance and low output impedance which is suitable for cascading&#xD;
for higher order filter transfer functions and low active and passive&#xD;
sensitivity performance.
&lt;br/&gt;
&lt;br/&gt;Page(s): 292-296</description>
  </item>
  <item rdf:about="http://nopr.niscair.res.in/handle/123456789/7649">
    <title>Structural and magnetic behaviour of NiFe&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;4&lt;/sub&gt; thin film grown by pulsed laser deposition</title>
    <link>http://nopr.niscair.res.in/handle/123456789/7649</link>
    <description>Title: Structural and magnetic behaviour of NiFe&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;4&lt;/sub&gt; thin film grown by pulsed laser deposition
&lt;br/&gt;
&lt;br/&gt;Authors: Dixit, Gagan; Singh, J P; Srivastava, R C; Agrawal, H M; Choudhary, R J; Gupta, Ajay
&lt;br/&gt;
&lt;br/&gt;Abstract: NiFe&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;4&lt;/sub&gt;&#xD;
thin film has been grown on Si (100) substrate by pulsed laser deposition (PLD)&#xD;
technique. The microstructure of the film was characterised by X-ray&#xD;
diffractometer (XRD) and atomic force microscopy (AFM). Magnetic&#xD;
characterisation has been done by vibrating sample magnetometer (VSM). In order&#xD;
to have comparative study, the bulk (target used for PLD) has also been&#xD;
characterised by XRD and VSM. Grazing incidence X-ray diffractometer (GIXRD)&#xD;
pattern of the film confirms the single spinel phase. Results of AFM have shown&#xD;
that the average grain size of the prepared film is of the order of 47 nm and&#xD;
surface roughness of the order of 3-4 nm. VSM measurements indicate that for&#xD;
the film, both the saturation magnetisation and the coercivity are greater than&#xD;
that of bulk.
&lt;br/&gt;
&lt;br/&gt;Page(s): 287-291</description>
  </item>
  <item rdf:about="http://nopr.niscair.res.in/handle/123456789/7648">
    <title>Modified Ghiorso equation of state for CaMgSi&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;6&lt;/sub&gt; silicate melt at 1673 K</title>
    <link>http://nopr.niscair.res.in/handle/123456789/7648</link>
    <description>Title: Modified Ghiorso equation of state for CaMgSi&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;6&lt;/sub&gt; silicate melt at 1673 K
&lt;br/&gt;
&lt;br/&gt;Authors: Kumar, M S; Sharma, B S
&lt;br/&gt;
&lt;br/&gt;Abstract: Ghiorso has recently&#xD;
developed a functional form for an equation of state (EOS) of molten silicate&#xD;
liquids. The EOS is designed for application over a wide range of melt&#xD;
compositions which can be used from reference conditions to very high&#xD;
pressures. It is emphasized here that the Ghiorso EOS does not satisfy the&#xD;
thermodynamic boundary conditions at infinite pressure. Ghiorso EOS has been&#xD;
modified to make it consistent with the Stacey thermodynamics at extreme&#xD;
compression. Various relationships between the compression ratio (&lt;i style=""&gt;V/V&lt;/i&gt;&lt;sub&gt;0&lt;/sub&gt;) and pressure &lt;i&gt;P&lt;/i&gt; have been studied for the&#xD;
silicate melt CaMgSi&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;6 &lt;/sub&gt;at 1673 K. The pressure-volume&#xD;
isothermal relationship, isothermal bulk modulus &lt;i style=""&gt;K&lt;/i&gt; and its pressure derivative have been calculated using five&#xD;
different forms of EOS viz. Birch Murnaghan third order EOS, Vinet-Rydberg EOS,&#xD;
Stacey EOS, Ghiorso EOS and the modified Ghiorso EOS. It is found that the&#xD;
modified Ghiorso EOS developed in the present study gives the satisfactory&#xD;
results which is in good agreement with the Stacey reciprocal-&lt;i&gt;K&lt;/i&gt;' EOS.
&lt;br/&gt;
&lt;br/&gt;Page(s): 282-286</description>
  </item>
  <item rdf:about="http://nopr.niscair.res.in/handle/123456789/7647">
    <title>Dependence of specific heat on electric field in Ba&lt;sub&gt;1&lt;/sub&gt;&lt;sub&gt;-x&lt;/sub&gt;Ca&lt;sub&gt;x&lt;/sub&gt;TiO&lt;sub&gt;3&lt;/sub&gt; ferroelectric perovskites</title>
    <link>http://nopr.niscair.res.in/handle/123456789/7647</link>
    <description>Title: Dependence of specific heat on electric field in Ba&lt;sub&gt;1&lt;/sub&gt;&lt;sub&gt;-x&lt;/sub&gt;Ca&lt;sub&gt;x&lt;/sub&gt;TiO&lt;sub&gt;3&lt;/sub&gt; ferroelectric perovskites
&lt;br/&gt;
&lt;br/&gt;Authors: Pradeep, Dushyant; Kumar, Ashok; Naithani, U C
&lt;br/&gt;
&lt;br/&gt;Abstract: The electric field&#xD;
dependence of the specific heat of an anharmonic Ba&lt;sub&gt;1&lt;/sub&gt;&lt;sub&gt;-x&lt;/sub&gt;Ca&lt;sub&gt;x&lt;/sub&gt;TiO&lt;sub&gt;3&lt;/sub&gt;&#xD;
ferroelectric crystal has been calculated in its paraelectric phase from&#xD;
Silverman-Joseph Hamiltonian augmented with fourth order phonon coordinates&#xD;
using double times Green’s functions. The electric field dependent soft mode&#xD;
contribution to the specific heat is described by appropriate Einstein terms.&#xD;
The variation of the specific heat with temperature and defect parameters has&#xD;
been discussed for different values of field strengths. The effect of defects&#xD;
on specific heat can be observed in the presence of anharmonicity. The specific&#xD;
heat decreases with increase in external field and increases with increase in&#xD;
temperature which is in agreement with the previous results. As the Curie&#xD;
temperature is approached, the Cochran soft mode is held to be responsible for&#xD;
the anomalous behaviour of specific heat.
&lt;br/&gt;
&lt;br/&gt;Page(s): 276-281</description>
  </item>
</rdf:RDF>

