<?xml version="1.0" encoding="UTF-8"?>
<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/123456789/16806" />
  <subtitle />
  <id>http://nopr.niscpr.res.in/handle/123456789/16806</id>
  <updated>2026-10-11T07:47:09Z</updated>
  <dc:date>2026-10-11T07:47:09Z</dc:date>
  <entry>
    <title>Conductance of ballistic superlattice in transverse magnetic field</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/26291" />
    <author>
      <name>Ghosh, P K</name>
    </author>
    <author>
      <name>Mitra, B</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/26291</id>
    <updated>2014-02-10T16:33:33Z</updated>
    <published>2001-03-01T00:00:00Z</published>
    <summary type="text">Title: Conductance of ballistic superlattice in transverse magnetic field
Authors: Ghosh, P K; Mitra, B
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 electronic transport of the ballistic superlattice in the presence of a&#xD;
transverse magnetic field within the constriction has been studied, where the&#xD;
wells have equal length across the constriction and the barriers are arranged&#xD;
in a manner either periodic or quasi-periodic· The conductance exhibits strong&#xD;
transmission resonances which drastically affected the quantized conductance, &amp;nbsp;plateaus of the ideal unmodulated constriction.&#xD;
The magnetic field produces an overall rightward shift of the conductance. When&#xD;
the field increases, the peaks in the group of resonances are depressed progressively&#xD;
in the region of a given plateau and finally disappear in a stronger magnetic field.&lt;/span&gt;
Page(s): 170-175</summary>
    <dc:date>2001-03-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>&lt;span style="font-size:14.0pt;line-height: 115%;font-family:"Times New Roman";mso-fareast-font-family:"Times New Roman"; color:black;mso-ansi-language:EN-IN;mso-fareast-language:EN-IN;mso-bidi-language: HI" lang="EN-IN"&gt;Investigations on sandwich &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;structures &lt;span style="font-size:14.0pt;line-height: 115%;font-family:"Times New Roman";mso-fareast-font-family:"Times New Roman"; color:black;mso-ansi-language:EN-IN;mso-fareast-language:EN-IN;mso-bidi-language: HI" lang="EN-IN"&gt;of metal-free p&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;hthalocyanine  &lt;span style="font-size:14.0pt;line-height:115%;font-family:"Times New Roman"; mso-fareast-font-family:"Times New Roman";color:black;mso-ansi-language:EN-IN; mso-fareast-language:EN-IN;mso-bidi-language:HI" lang="EN-IN"&gt;(H&lt;sub&gt;2&lt;/sub&gt;PC) thin film using gold electrodes&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/26290" />
    <author>
      <name>Unni, K N Narayanan</name>
    </author>
    <author>
      <name>Menon, C S</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/26290</id>
    <updated>2014-02-03T16:33:37Z</updated>
    <published>2001-03-01T00:00:00Z</published>
    <summary type="text">Title: &lt;span style="font-size:14.0pt;line-height: 115%;font-family:"Times New Roman";mso-fareast-font-family:"Times New Roman"; color:black;mso-ansi-language:EN-IN;mso-fareast-language:EN-IN;mso-bidi-language: HI" lang="EN-IN"&gt;Investigations on sandwich &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;structures &lt;span style="font-size:14.0pt;line-height: 115%;font-family:"Times New Roman";mso-fareast-font-family:"Times New Roman"; color:black;mso-ansi-language:EN-IN;mso-fareast-language:EN-IN;mso-bidi-language: HI" lang="EN-IN"&gt;of metal-free p&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;hthalocyanine  &lt;span style="font-size:14.0pt;line-height:115%;font-family:"Times New Roman"; mso-fareast-font-family:"Times New Roman";color:black;mso-ansi-language:EN-IN; mso-fareast-language:EN-IN;mso-bidi-language:HI" lang="EN-IN"&gt;(H&lt;sub&gt;2&lt;/sub&gt;PC) thin film using gold electrodes&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Authors: Unni, K N Narayanan; Menon, C S
Abstract: &lt;span style="font-size:&#xD;
 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;Sandwich&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; structures of metal-free&#xD;
phthalocyanine (H&lt;sub&gt;2&lt;/sub&gt;Pc) thin films using gold electrodes have been&#xD;
prepared by thermal evaporation. The &lt;i&gt;J-V&lt;/i&gt; characteristics are determined&#xD;
for films exposed to air and for films annealed in air at 523K. The temperature&#xD;
dependence of current density is studied for both ohmic and space charge&#xD;
limited conduction (SCLC). The effect of incorporation of oxygen into the&#xD;
structure in both cases is &lt;span style="font-size:14.0pt;&#xD;
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;investigated.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Page(s): 159-162</summary>
    <dc:date>2001-03-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Effect of charge fluctuation on current pulses and instability in a plasma produced in admixture of gases subjected to dc corona discharge</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/26289" />
    <author>
      <name>Pimpale, Sushama S</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/26289</id>
    <updated>2014-01-31T16:33:22Z</updated>
    <published>2001-03-01T00:00:00Z</published>
    <summary type="text">Title: Effect of charge fluctuation on current pulses and instability in a plasma produced in admixture of gases subjected to dc corona discharge
Authors: Pimpale, Sushama S
Abstract: The effect&#xD;
of time of&amp;nbsp; exposure to electrodeless&#xD;
discharge on emission of counts for a temperature of 50°C in a fresh vessel&#xD;
under de excitation has been studied by exposing air at a pressure of 10 torr&#xD;
to a potential of 1.5 kV and to a bias of 5&#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;V. The change of current&#xD;
pulses which is composed of the basic charging equation and fluctuations in the&#xD;
plasma has been discussed on the basis of charge equality and inequality in the&#xD;
plasma bounded by two concentric glass tubes.&lt;/span&gt;
Page(s): 155-158</summary>
    <dc:date>2001-03-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Growth and electrical transport properties of dithallium selenide single crystal</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/26264" />
    <author>
      <name>Rahman, M Abdel</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/26264</id>
    <updated>2014-01-29T16:42:58Z</updated>
    <published>2001-03-01T00:00:00Z</published>
    <summary type="text">Title: Growth and electrical transport properties of dithallium selenide single crystal
Authors: Rahman, M Abdel
Abstract: &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;Crystals&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; of the Tl&lt;sub&gt;2&lt;/sub&gt;Se were synthesized&#xD;
with the aid of locally designed simple new growth technique. This technique is&#xD;
based on Bridgman growth method. Electrical conductivity, Hall effect and Hall&#xD;
mobility were investigated as a function of temperature in the range 225-500K,&#xD;
on  &lt;i&gt;p&lt;/i&gt;-type single&#xD;
crystals.Measurements were crried out perpendicular to the &lt;i&gt;c&lt;/i&gt;-axix.&#xD;
Variation of the charge carriers against temperatures was discussed. The energy&#xD;
gap width as well as the ionozation energy was computed. At room temperature&#xD;
the Hall mobility was found to be μ=500cm&lt;sup&gt;2&lt;/sup&gt;/V.&lt;/span&gt;&lt;/span&gt;
Page(s): 176-179</summary>
    <dc:date>2001-03-01T00:00:00Z</dc:date>
  </entry>
</feed>

