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    <title>NOPR Community:</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/63</link>
    <description />
    <pubDate>Mon, 05 Oct 2026 09:41:39 GMT</pubDate>
    <dc:date>2026-10-05T09:41:39Z</dc:date>
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      <title>NOPR Community:</title>
      <url>https://http://nopr.niscpr.res.in:443/retrieve/200086/IJPAP 64(05) Cover Page.png</url>
      <link>http://nopr.niscpr.res.in/handle/123456789/63</link>
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    <item>
      <title>Odd-Even Staggering in Gamma Vibrational Bands of Deformed Nuclei Insights from Collective Models and Machine Learning Approaches</title>
      <link>http://nopr.niscpr.res.in/handle/123456789/68440</link>
      <description>Title: Odd-Even Staggering in Gamma Vibrational Bands of Deformed Nuclei Insights from Collective Models and Machine Learning Approaches
Authors: Sharma, Pooja; Bindra, Amit
Abstract: The odd-even spin staggering of gamma-vibrational bands is examined for even-even Gd isotopes in the rare-earth region. The&#xD;
work uses experimental gamma-band energies, the empirical staggering index S(J), the energy ratio R4/2, and the asymmetry&#xD;
parameter gamma0 to follow the evolution from gamma-soft behaviour toward more axially deformed rotational structures. The&#xD;
analysis is framed by collective-model ideas, especially the interacting boson model and the triaxial rotor picture, because both&#xD;
connect gamma-band level splitting with the softness or rigidity of the nuclear shape. A LightGBM regression procedure is further&#xD;
used only as a data-support tool for the missing S(7) and S(8) entries at N = 94. The imputed values are inserted with uncertainty&#xD;
estimates so that the observed trend of the Gd chain can be discussed without leaving artificial gaps in the systematics. The results&#xD;
show strong staggering near the transitional neutron numbers and a close relation between S(J), R4/2 and asymmetry&#xD;
parameter 𝛾􀬴. These observations support the view that gamma-band staggering is a sensitive indicator of triaxial effects,&#xD;
shape evolution and symmetry changes in deformed nuclei.
Page(s): 955-960</description>
      <pubDate>Tue, 01 Sep 2026 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://nopr.niscpr.res.in/handle/123456789/68440</guid>
      <dc:date>2026-09-01T00:00:00Z</dc:date>
    </item>
    <item>
      <title>Harmonic Minimization using a Cascaded Multilevel Converter for a Standalone Renewable Energy System</title>
      <link>http://nopr.niscpr.res.in/handle/123456789/68439</link>
      <description>Title: Harmonic Minimization using a Cascaded Multilevel Converter for a Standalone Renewable Energy System
Authors: Gupta, Ranitesh; Sahay, Kuldeep
Abstract: Effective power conversion is necessary when integrating photovoltaic (PV) systems into the electrical grid to manage&#xD;
high voltages, minimize switch stress, and improve power quality while reducing the need for intensive filtering.&#xD;
The advantages of multilevel inverters (MLIs), especially cascaded H-Bridge (CHB) designs, in lowering electromagnetic&#xD;
interference (EMI) and increasing efficiency have made them essential for renewable energy systems. This work proposes a&#xD;
DC-AC-DC-AC converter system with seven-level and thirteen-level topologies. The seven-level converter system is&#xD;
designed and simulated in MATLAB/Simulink using phase-shifted pulse-width modulation (PSPWM) and level-shifted&#xD;
pulse-width modulation (LSPWM) to analyze total harmonic distortion (THD) and determine the best modulation technique&#xD;
for a grid-connected standalone system. The study finds that the thirteen-level converter showed improved power quality&#xD;
and system efficiency, with a significant decrease in THD to 0.43 % after filtering. Real-time simulation on the OPAL-RT&#xD;
platform confirms the adaptability and efficacy of the presented approach in real-world situations. Furthermore,&#xD;
incorporating more reliable and compact medium-frequency transformers supports environmental sustainability by&#xD;
enhancing energy efficiency, reducing material consumption, and supporting modularity for easier maintenance.
Page(s): 961-971</description>
      <pubDate>Tue, 01 Sep 2026 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://nopr.niscpr.res.in/handle/123456789/68439</guid>
      <dc:date>2026-09-01T00:00:00Z</dc:date>
    </item>
    <item>
      <title>Adaptive Metaheuristic Optimization of Frequency-Selective Multi-band Antennas for Enhanced Electromagnetic Performance</title>
      <link>http://nopr.niscpr.res.in/handle/123456789/68438</link>
      <description>Title: Adaptive Metaheuristic Optimization of Frequency-Selective Multi-band Antennas for Enhanced Electromagnetic Performance
Authors: Palanisamy, SatheeshKumar; Sathishkumar, N; Mahapatra, Sheila; Kandasamy, Jeevitha
Abstract: With advanced wireless systems gaining market traction, there is a need for small, high-performance antennas. Design&#xD;
strategies must be efficient and accurate so antennas can operate across multiple bands with good gain and impedance&#xD;
matching. This study presents a flexible metaheuristic optimization methodology for designing a multi-band antenna with&#xD;
Frequency Selective Surfaces (FSS). The design process involves the step-by-step evolution of its FSS unit cell, starting&#xD;
from a circular structure followed by an annular ring and an adyne triangular protrusion to enhance resonance characteristics&#xD;
and surface current distribution. The rectangular patch with its rectangular protrusions forms the key radiating component of&#xD;
the antenna at the end. An evolved frequency-selective surface (FSS) cell improves frequency selectivity and gain. The&#xD;
Adaptive Enhanced Diversified Hiking Optimization Algorithm (AEDHOA) achieves a good trade-off between exploration&#xD;
and exploitation, with accelerated convergence and improved optimization accuracy. Simulations and experiments both&#xD;
show that far-field radiation performance improves significantly when FSS elements are added to the radiating surface. At&#xD;
3.8 GHz, the antenna with FSS under the patch achieves a return loss of −53 dB, a VSWR of 1.3, and a gain of 4.01 dBi.&#xD;
Compared with traditional methods, the AEDHOA reduces computation iterations by 35 % and increases the fitness value&#xD;
by 27 %. This work demonstrates a scalable and computationally efficient design approach for multi-band antennas suitable&#xD;
for next-gen wireless, IoT, and radar applications.
Page(s): 972-983</description>
      <pubDate>Tue, 01 Sep 2026 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://nopr.niscpr.res.in/handle/123456789/68438</guid>
      <dc:date>2026-09-01T00:00:00Z</dc:date>
    </item>
    <item>
      <title>Polar Resistors Asymmetric Semiconductor Structures as Linear Resistors with Different Resistances for Opposite Polarities</title>
      <link>http://nopr.niscpr.res.in/handle/123456789/68437</link>
      <description>Title: Polar Resistors Asymmetric Semiconductor Structures as Linear Resistors with Different Resistances for Opposite Polarities
Authors: N Roy Choudhury, Aditya
Abstract: Passive, two-terminal resistors, with linear current voltage relationships, but exhibiting different resistances for opposite&#xD;
polarities are introduced in this paper. Such resistors change their resistance when current direction through them changes.&#xD;
These are named polar resistors. Such polar resistance is observed in asymmetric semiconductor INI structures, where I is an&#xD;
abbreviation for intrinsic, and N is for n-type doped. Polar resistance is not material specific. Both Silicon and Gallium&#xD;
Arsenide polar resistors were simulated in this work. In a three-layered INI structure, for certain thicknesses of the intrinsic&#xD;
layers, it is observed that for positive voltage, voltage drops significantly across one intrinsic layer, and for negative voltage,&#xD;
voltage drops significantly across the other intrinsic layer. With different I-layer thicknesses polar resistance is achieved.&#xD;
A background mobile electronic concentration of 1011/cc and 1012/cc were assumed for Si, due to background doping, and&#xD;
107/cc and 108/cc were assumed for GaAs. Metallic ohmic contacts to semiconductor intrinsic layers are difficult to&#xD;
fabricate. So doped n-type CdS and SnO2 were used as contact enabling layers to Si and GaAs respectively. This implies the&#xD;
structure is NININ; i.e. N-CdS/I-Si/N-Si/I-Si/N-CdS and N-SnO2/I-GaAs/N-GaAs/I-GaAs/N-SnO2. In such devices,&#xD;
between -1V and +1V, polar resistance is observed and a rectification ratio up to 10 are demonstrated. The roles of the&#xD;
middle N layer and the n-type contact enabling layers are also discussed.
Page(s): 984-997</description>
      <pubDate>Tue, 01 Sep 2026 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://nopr.niscpr.res.in/handle/123456789/68437</guid>
      <dc:date>2026-09-01T00:00:00Z</dc:date>
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