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    <title>DSpace Community: PHD</title>
    <link>http://202.45.146.37:8080/jspui/handle/123456789/445</link>
    <description>PHD</description>
    <pubDate>Thu, 27 Aug 2026 00:34:57 GMT</pubDate>
    <dc:date>2026-08-27T00:34:57Z</dc:date>
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      <title>FIRST-PRINCIPLES STUDY OF MECHANICAL, ELECTRONIC, MAGNETIC AND OPTICAL PROPERTIES OF SELECTED SINGLE AND  DOUBLE PEROVSKITES</title>
      <link>http://202.45.146.37:8080/jspui/handle/123456789/447</link>
      <description>Title: FIRST-PRINCIPLES STUDY OF MECHANICAL, ELECTRONIC, MAGNETIC AND OPTICAL PROPERTIES OF SELECTED SINGLE AND  DOUBLE PEROVSKITES
Authors: POKHAREL, PESHAL
Abstract: Perovskites are crystalline materials represented by the general formula ABX3. Their&#xD;
simple crystal structure leads to a broad range of electrical, catalytic, optical, magnetic,&#xD;
piezoelectric, dielectric, and magnetoresistive properties. Due to their remarkable&#xD;
properties, perovskites have been widely utilized in thin-film capacitors, optoelectronic&#xD;
devices, non-volatile memory, solar cells, data storage technologies, spintronic devices,&#xD;
lasers, sensors, high-temperature coatings, and frequency filters. In the present work,&#xD;
&#xD;
we investigate the mechanical, electronic, magnetic, and optical properties of zirco-&#xD;
nium silicate (ZrSiO3) perovskite (under different hydrostatic pressures, surface termi-&#xD;
nations, different layer configurations, and its monolayer form); europium (Eu)– and&#xD;
&#xD;
yttrium (Y)–doped samarium manganite (SmMnO3); and the double perovskite stron-&#xD;
tium zirconium molybdate (Sr2ZrMoO6) using first-principles density functional theory&#xD;
&#xD;
(DFT) calculations. For bulk calculations, the Perdew–Burke–Ernzerhof (PBE–GGA)&#xD;
exchange–correlation functional was used, whereas the Perdew–Burke–Ernzerhof for&#xD;
solids (PBEsol) functional was employed for surface and layered structures. Ultrasoft&#xD;
Vanderbilt pseudopotentials (USPPs) were adopted with plane-wave cutoff of 70 Ry&#xD;
for the wavefunctions and 560 Ry for the charge density. Brillouin zone sampling was&#xD;
performed using Monkhorst–Pack grids of 14 × 14 × 14 for bulk property calculations&#xD;
and 14 × 14 × 1 for the monolayer. Convergence thresholds were set to 10−6 eV for the&#xD;
total energy and 10−3 eV/Å for the atomic forces. The elastic constants were calculated&#xD;
using the stress–strain method. The present study shows that the bulk ZrSiO3 is an&#xD;
indirect band gap semiconductor. Its band gap value increases with rise in pressure and&#xD;
decreases with the increasing number of layers. The termination model has a smaller&#xD;
band gap (2.585 eV for ZrO– and 1.639 eV for SiO2– termination model) than the bulk&#xD;
model. Electronic band gap of ZrSiO3 monolayer increases under compressive strain&#xD;
and decreases under tensile strain. Pristine SmMnO3 shows ferromagnetic half–metallic&#xD;
&#xD;
behaviour, and has the band gap of 2.72 eV. Its value substantially reduces with the in-&#xD;
troduction of Eu and Y dopants. The Sr2ZrMoO6 double perovskite exhibits an indirect&#xD;
&#xD;
band gap semiconductor with ferromagnetic behaviour. Elastic property calculations&#xD;
confirmed the mechanical stability and ductility of bulk ZrSiO3 up to 100 GPa. Both&#xD;
ZrO– and SiO2–terminated models of ZrSiO3 are also mechanically stable and ductile.&#xD;
The ZrSiO3 monolayer exhibits mechanical stability and ductility from -6% to +6%&#xD;
strain values. The pristine and Eu– and Y– doped SmMnO3, the material preserves&#xD;
its mechanical stability and ductility, even at a 25% substitution level. The stiffness of&#xD;
pristine SmMnO3 decreases with Eu– doping and increases with Y– doping. Elastic&#xD;
calculations of double perovskite Sr2ZrMoO6 under isotropic pressures from 0 to 80&#xD;
GPa reveal significant elastic anisotropy, with distinct pressure–dependent behaviors.&#xD;
&#xD;
ix&#xD;
&#xD;
Magnetic analysis reveals that the magnetic moment of SmMnO3 increases with Eu–&#xD;
doping, whereas Y– doping leads to a reduction. Curie temperature of pristine SmMnO3&#xD;
raises with Eu– doping, whereas lowers with Y– doping. The real and imaginary parts&#xD;
of dielectric function of ZrSiO3 increase with pressure, with absorption edges and sharp&#xD;
peaks shift to higher energies as pressure increases from 0 to 100 GPa. The refractive&#xD;
index and reflectivity of SmMnO3 decreases with Eu– and Y– dopings. The tunable&#xD;
electronic and optical properties of ZrSiO3 under pressure, mechanical strain, surface&#xD;
termination and 2D form indicated the material is suitable for flexible electronic devices&#xD;
and nano–electronics. The enhanced magnetic and electronic properties of Eu–and Y–&#xD;
doping on SmMnO3 indicate its application in magnetic sensors and data storage devices.
Description: FOR THE AWARD OF&#xD;
DOCTOR OF PHILOSOPHY&#xD;
&#xD;
IN PHYSICS</description>
      <pubDate>Wed, 01 Jul 2026 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://202.45.146.37:8080/jspui/handle/123456789/447</guid>
      <dc:date>2026-07-01T00:00:00Z</dc:date>
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