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  <title>DSpace Community:</title>
  <link rel="alternate" href="http://localhost:80/xmlui/handle/123456789/185" />
  <subtitle />
  <id>http://localhost:80/xmlui/handle/123456789/185</id>
  <updated>2026-04-08T12:31:50Z</updated>
  <dc:date>2026-04-08T12:31:50Z</dc:date>
  <entry>
    <title>A molecular field approach to pressure-induced phase transitions in liquid crystals: Smectic–nematic transition</title>
    <link rel="alternate" href="http://localhost:80/xmlui/handle/123456789/193" />
    <author>
      <name>DasGupta, Sudeshna</name>
    </author>
    <id>http://localhost:80/xmlui/handle/123456789/193</id>
    <updated>2022-06-22T08:08:45Z</updated>
    <published>2021-01-01T00:00:00Z</published>
    <summary type="text">Title: A molecular field approach to pressure-induced phase transitions in liquid crystals: Smectic–nematic transition
Authors: DasGupta, Sudeshna
Abstract: Since a rigorous microscopic treatment of a nematic ﬂuid system based on a pairwise interaction potential is immensely complex, we had&#xD;
introduced a simple mean ﬁeld potential, which was a modiﬁcation of the Maier–Saupe potential in a previous paper [S. DasGupta et al.,&#xD;
“Pressure-induced phase transitions in liquid crystals: A molecular ﬁeld approach,” Phys. Rev. E 98, 022701 (2018)]. Building upon that,&#xD;
here we have modiﬁed that potential to take into account the various aspects of a smectic A–nematic phase transition. In particular, we have&#xD;
studied the dependence of the phase transition on the coupling coefﬁcient between the nematic and smectic order parameters, which in turn&#xD;
depends on the length of alkyl chain, variation of density, entropy, and speciﬁc heat. Detailed investigation on the coupling parameter shows&#xD;
the existence of a smectic A–nematic–isotropic triple point as well as a tricritical point where the smectic–nematic phase transition changes&#xD;
its nature from the second to the ﬁrst order. It is also seen that the application of pressure can result in the appearance of a nematic phase.
Description: Physics of Fluids special topic : Tribute to Frank M. White on his 88th Anniversary.</summary>
    <dc:date>2021-01-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Monte Carlo study with reweighting of uniaxial nematic liquid crystals composed of biaxial molecules</title>
    <link rel="alternate" href="http://localhost:80/xmlui/handle/123456789/192" />
    <author>
      <name>DasGupta, Sudeshna</name>
    </author>
    <id>http://localhost:80/xmlui/handle/123456789/192</id>
    <updated>2022-06-22T07:57:43Z</updated>
    <published>2019-01-01T00:00:00Z</published>
    <summary type="text">Title: Monte Carlo study with reweighting of uniaxial nematic liquid crystals composed of biaxial molecules
Authors: DasGupta, Sudeshna
Abstract: We present a high accuracy Monte Carlo simulation study of the uniaxial nematic (N U ) to isotropic (I) phase&#xD;
transition of a lattice dispersion model of uniaxial nematics composed of biaxial molecules. The N U -I coexistence&#xD;
curve terminating at the Landau critical point has been determined using the multiple histogram reweighting&#xD;
technique. A close investigation reveals a sharp departure in the nature of the N U -I coexistence curve in the&#xD;
temperature-biaxiality parameter phase diagram in comparison to the earlier theoretical (either mean-field or&#xD;
computer simulation) predictions. The coexistence curve shows a change in curvature with increasing value of&#xD;
the degree of molecular biaxiality.</summary>
    <dc:date>2019-01-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Pressure-induced phase transitions in liquid crystals: A molecular field approach</title>
    <link rel="alternate" href="http://localhost:80/xmlui/handle/123456789/191" />
    <author>
      <name>DasGupta, Sudeshna</name>
    </author>
    <id>http://localhost:80/xmlui/handle/123456789/191</id>
    <updated>2022-06-22T07:54:15Z</updated>
    <published>2018-01-01T00:00:00Z</published>
    <summary type="text">Title: Pressure-induced phase transitions in liquid crystals: A molecular field approach
Authors: DasGupta, Sudeshna
Abstract: A rigorous microscopic treatment of a nematic fluid system based on a pairwise interaction potential is&#xD;
immensely complex. For studying such systems molecular field theories are often the standard method of&#xD;
2&#xD;
 P 2  P 2 (cos ϑ ) to study&#xD;
choice. In this paper we have chosen a simple effective potential U = u v 4 4 − u v 2 2 − Au&#xD;
v 2&#xD;
an isothermal-isobaric ensemble describing a liquid crystalline system. Using this we have studied in particular&#xD;
the pressure dependence of liquid crystalline phase transitions.</summary>
    <dc:date>2018-01-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Monte Carlo investigation of critical properties of the Landau point of a biaxial liquid-crystal system</title>
    <link rel="alternate" href="http://localhost:80/xmlui/handle/123456789/190" />
    <author>
      <name>DasGupta, Sudeshna</name>
    </author>
    <id>http://localhost:80/xmlui/handle/123456789/190</id>
    <updated>2022-06-22T07:49:10Z</updated>
    <published>2016-01-01T00:00:00Z</published>
    <summary type="text">Title: Monte Carlo investigation of critical properties of the Landau point of a biaxial liquid-crystal system
Authors: DasGupta, Sudeshna
Abstract: Extensive Monte Carlo simulations are performed to investigate the critical properties of a special singular&#xD;
point usually known as the Landau point. The singular behavior is studied in the case when the order parameter is&#xD;
a tensor of rank 2. Such an order parameter is associated with a nematic-liquid-crystal phase. A three-dimensional&#xD;
lattice dispersion model that exhibits a direct biaxial nematic-to-isotropic phase transition at the Landau point&#xD;
is thus chosen for the present study. Finite-size scaling and cumulant methods are used to obtain precise&#xD;
values of the critical exponent ν = 0.713(4), the ratio γ /ν = 1.85(1), and the fourth-order critical Binder&#xD;
cumulant U ∗ = 0.6360(1). Estimated values of the exponents are in good agreement with renormalization-group&#xD;
predictions.</summary>
    <dc:date>2016-01-01T00:00:00Z</dc:date>
  </entry>
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