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<ArticleSet>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Mitigation of disruption on IR-T1 tokamak by means of low-energy neutral beam injection to control runaway electron generation</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 14 (2020)</Volume>
			<Issue>Issue 4, August 2020</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Mitigation of disruption on IR-T1 tokamak by means of low-energy neutral beam injection to control runaway electron generation</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.1007/s40094-020-00386-1</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>M.</FirstName>
				<LastName>Kafi</LastName>
				<Affiliation>Plasma Physics Research Center, Science and Research Branch, Islamic Azad University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Mahmoud</FirstName>
				<LastName>Ghoranneviss</LastName>
				<Affiliation>Plasma Physics Research Center, Science and Research Branch, Islamic Azad University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Mohammad</FirstName>
				<LastName>Reza Ghanbari</LastName>
				<Affiliation>Department of Basic Sciences, Garmsar Branch, Islamic Azad University, Garmsar, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Mohammad</FirstName>
				<LastName>Kazem Salem</LastName>
				<Affiliation>Plasma Physics Research Center, Science and Research Branch, Islamic Azad University, P.O. Box: 14665‑678, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0002-8810-1820</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>AbstractIn a tokamak, the poloidal magnetic field provided by the toroidal plasma current forms an essential part of the magnetic field confining the plasma. However, instabilities of magnetohydrodynamic equilibrium can lead to an uncontrolled sudden loss of plasma current and energy, which is called a disruption. Disruptions are of significant concern to future devices due to the large amount of energy released during the rapid quenching of the plasma. One important consequence of disruption is the generation of significant current carried in multi-MeV runaway electrons that are eventually lost into plasma components. They can damage the tokamak walls and its structure if they are not controlled. Disruption control by neutral beam injection has been performed on IR-T1 to study the effect on runaway electron generated by plasma disruptions. Noble gases are used for injection, pure Hydrogen, Helium and Argon. The use of these non-reactive gases for disruption control ensures they fast removed from the vessel after the termination of a tokamak discharge. A piezo-valve is used for injection which has the precision of 1 ms. The effect of runaway electron generation control during disruption is studied using a comparison between reference disruptive discharge and a discharge into which different impurity species are injected. The data collected can then be used to optimize the performance of these energetic electrons control generated in disruption.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Hard X</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Runaway electrons</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Ray</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Tokamak</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Enhancement of charge breeding efficiency for rare isotope beam with the control of magnetic field profile and electron beam energy in EBIS</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 14 (2020)</Volume>
			<Issue>Issue 4, August 2020</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Enhancement of charge breeding efficiency for rare isotope beam with the control of magnetic field profile and electron beam energy in EBIS</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.1007/s40094-020-00388-z</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Jong-Won</FirstName>
				<LastName>Kim</LastName>
				<Affiliation>Rare Isotope Science Project, Institute for Basic Science, Daejeon 34000, Korea</Affiliation>
				<Identifier Source="ORCID">0000-0003-3052-8482</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>AbstractThe magnetic field in the ion trap of electron beam ion source (EBIS) determines the current density of electron beam and thus the depth of trap potential, which affects the charge breeding efficiency to desired charge state. An EBIS charge breeder has been constructed to be used for the Rare Isotope Science Project in Korea. A 6 T superconducting solenoid is used for the trap, and uniform magnetic field is extended with correction coils at the ends. The effect of field uniformity on the electron current density is evaluated using TRAK, and it is shown sizable improvement in the charge breeding efficiency for rare isotope beams can be obtained by elaborate magnetic design. Furthermore, the electron beam energy affects the ionization efficiency. The electron energy is often reduced in the trap for optimal matching with charge striping cross section. However, virtual cathode formation can appear in the process of energy reduction. Maximum beam currents limited by electron energy are studied analytically and by TRAK simulation in the view of improving the charge breeding efficiency.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Charge breeding</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Electron beam ion source (EBIS)</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Rare isotope beam</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Superconducting magnet</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Virtual cathode</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Transcriptional responses following seed priming with cold plasma and electromagnetic field in Salvia nemorosa L.</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 14 (2020)</Volume>
			<Issue>Issue 4, August 2020</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Transcriptional responses following seed priming with cold plasma and electromagnetic field in Salvia nemorosa L.</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.1007/s40094-020-00387-0</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Maryam</FirstName>
				<LastName>Ghaemi</LastName>
				<Affiliation>Department of Biology, Science and Research Branch, Islamic Azad University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Ahmad</FirstName>
				<LastName>Majd</LastName>
				<Affiliation>Department of Biology, Faculty of Biological Sciences, North-Tehran Branch, Islamic Azad University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Alireza</FirstName>
				<LastName>Iranbakhsh</LastName>
				<Affiliation>Department of Biology, Science and Research Branch, Islamic Azad University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>AbstractThis study was conducted to monitor the plant responses to seed priming with electromagnetic fields (0, 4, or 6 mT) or cold plasma (0, 80, or 100 s) in Salvia nemorosa. The cold plasma or electromagnetic field treatments significantly increased shoot fresh weight (49%), root fresh weight (41%), and root length (56%). The results highlighted that seed priming with cold plasma or the electromagnetic field is an effective method to modify seedling growth. The electromagnetic field and plasma treatments upregulated the AREB1 gene (mean = 3.9-fold). Except for the electromagnetic field of 4mT, the other treatments stimulated expressions of the WRKY1 gene by an average of 6.7-fold relative to the control. The cold plasma or electromagnetic field also induced the expression of cinnamoyl-CoA reductases (CCR2) gene (mean = fourfold). These treatments also changed the expression of the rosmarinic acid synthase by an average of sixfold. These findings may improve our knowledge of plant reactions to cold plasma and electromagnetic field for possible functions in seed technology.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Applied physics</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Electromagnetic field</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Gene expression</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Cold plasma</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Seed priming</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>The effects of multiwall carbon nanotubes on the electrical characteristics of ZnO-based composites</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 14 (2020)</Volume>
			<Issue>Issue 4, August 2020</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>The effects of multiwall carbon nanotubes on the electrical characteristics of ZnO-based composites</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.1007/s40094-020-00389-y</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>N.</FirstName>
				<LastName>Asaadi</LastName>
				<Affiliation>Department of Condensed Matter Physics, Faculty of Physics, University of Tabriz, 29 Bahman Blvd., Imam St., Tabriz, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>M.</FirstName>
				<LastName>Parhizkar</LastName>
				<Affiliation>Department of Condensed Matter Physics, Faculty of Physics, University of Tabriz, 29 Bahman Blvd., Imam St., Tabriz, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0002-6847-6799</Identifier>
			</Author>
            			<Author>
                				<FirstName>H.</FirstName>
				<LastName>Bidadi</LastName>
				<Affiliation>Department of Condensed Matter Physics, Faculty of Physics, University of Tabriz, 29 Bahman Blvd., Imam St., Tabriz, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>S.</FirstName>
				<LastName>Mohammadi Aref</LastName>
				<Affiliation>Department of Condensed Matter Physics, Faculty of Physics, University of Tabriz, 29 Bahman Blvd., Imam St., Tabriz, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>M.</FirstName>
				<LastName>Ghafouri</LastName>
				<Affiliation>Department of Physics, Faculty of Physics, Shabestar Branch, Islamic Azad University, Shabestar, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>AbstractIn this experimental work, the effects of multiwall carbon nanotubes (MWCNTs) on electrical characteristics of zinc oxide–MWCNT–high-density polyethylene composite varistors have been investigated. All the samples were made at the temperature of 130 °C and pressure of 60 MPa by the hot-press method. Results show that increasing zinc oxide content in the mixture increases breakdown voltage up to 170 V, where the highest nonlinear coefficient (α ~ 13) corresponds to the samples with 95 wt% of ZnO. Results with regard to the effects of MWCNT as an additive reveal that increasing its content from 1 to 2.5% in the composites, the breakdown voltage decreases to 50 V, but the highest nonlinear coefficient (~ 14) corresponds to the sample with 1.5% of MWCNT content. It is also revealed that, heat treatment of the sample at a constant temperature of 135 °C and different time intervals from 2 to 10 h, the sample with 6 h annealing time shows maximum breakdown voltages (Vb = 140 V) with the highest nonlinear coefficient (~ 14). Investigation of the potential barrier height of samples shows a complete consistency with the breakdown voltage variations. The results have been justified regarding XRD patterns and SEM micrographs of samples.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">ZnO</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Composite varistor</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Multiwall carbon nanotube</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Nonlinear coefficient</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Fabrication of Au/ZnO/MWCNTs electrode and its characterization for electrochemical cholesterol biosensor</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 14 (2020)</Volume>
			<Issue>Issue 4, August 2020</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Fabrication of Au/ZnO/MWCNTs electrode and its characterization for electrochemical cholesterol biosensor</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.1007/s40094-020-00390-5</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Davood</FirstName>
				<LastName>Ghanei Agh Kaariz</LastName>
				<Affiliation>Department of Physics, Faculty of Sciences, Science and Research Branch, Islamic Azad University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Elham</FirstName>
				<LastName>Darabi</LastName>
				<Affiliation>Department of Physics, Faculty of Sciences, Science and Research Branch, Islamic Azad University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0001-9887-5291</Identifier>
			</Author>
            			<Author>
                				<FirstName>Seyed</FirstName>
				<LastName>Mohammad Elahi</LastName>
				<Affiliation>Department of Physics, Faculty of Sciences, Science and Research Branch, Islamic Azad University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>AbstractIn this work, a new sensitive enzyme-based electrode for electrochemical cholesterol biosensor was fabricated based on a nanocomposite of Au nanoparticles, ZnO nanoparticles and multi-wall carbon nanotubes (Au/ZnO/MWCNTs). The nanocomposite was prepared by sol–gel method and deposited on FTO substrate by dip coating, followed by cholesterol oxidase (ChOx) enzyme immobilized (ChOx/Au/ZnO/MWCNTs). Structural properties and morphology of the nanocomposite have been studied using X-ray diffraction (XRD) and Field emission scanning electron microscopy (FESEM). The sample was subjected to Fourier transform infrared spectroscopy (FTIR) to determine functional groups. Electrochemical behavior of the electrode was studied by cyclic voltammetry (CV) and differential pulse voltammetry (DPV) techniques as a function of cholesterol concentration. Electrochemical impedance spectroscopy (EIS) was also considered to study of surface modified electrodes. The ChOx/Au/ZnO/MWCNTs electrode has been found to have enhanced electron transfer and display excellent analytical linear performances. The fabricated electrode exhibited low detection limit (0.1 μM), high sensitivity (25.89 μA/μM) evaluated from DPV data in the detection range of 0.1–100 µM and high selectivity in the determination of cholesterol over glucose and uric acid. The application of the ChOx/Au/ZnO/MWCNTs electrode in detection of cholesterol in human serum was also confirmed.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Au nanoparticles</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Au/ZnO/MWCNTs nanocomposite</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Cholesterol</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Cholesterol oxidase</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Electrochemical biosensor</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Wall carbon nanotubes</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">ZnO Nanoparticles</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Multi</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Transmission of electromagnetic waves through a nonlinear over-dense plasma slab</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 14 (2020)</Volume>
			<Issue>Issue 4, August 2020</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Transmission of electromagnetic waves through a nonlinear over-dense plasma slab</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.1007/s40094-020-00391-4</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>M.</FirstName>
				<LastName>Tohfeh</LastName>
				<Affiliation>Department of Physics, North Tehran Branch, Islamic Azad University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Leila</FirstName>
				<LastName>Rajaei</LastName>
				<Affiliation>Department of Physics, Faculty of Basic Sciences, University of Qom, Qom, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0002-1303-9225</Identifier>
			</Author>
            			<Author>
                				<FirstName>Sedigheh</FirstName>
				<LastName>Miraboutalebi</LastName>
				<Affiliation>Department of Physics, North Tehran Branch, Islamic Azad University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0002-3117-3938</Identifier>
			</Author>
            			<Author>
                				<FirstName>L</FirstName>
				<LastName>Farhang Matin</LastName>
				<Affiliation>Department of Physics, North Tehran Branch, Islamic Azad University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>AbstractA study on the transmission of the electromagnetic waves from a structure consisting of an over-dense plasma layer with nonlinear effects is undertaken. The applied nonlinearity is presented due to the series expansion of the polarization in the medium. The nonlinear plasma layer is supposed to be placed between two linear dielectric layers. The transparency conditions are investigated for the p-polarized obliquely incident waves. It is shown that the formation of the surface waves can eventuate to the transmission of the incident waves. This fact has already be seen in the case of the linear over-dense plasma, but, here, it is examined in the presence of the nonlinear effects. To determine the propitious conditions for the surface wave excitation, the exact solutions of the electromagnetic field equations are used in all regions. The transmission, the reflection, and the dissipation rates of the electromagnetic waves from the entire structure are obtained, and the effects of the main parameters on them are discussed.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Reflection amplitude</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Surface wave</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Transition amplitude</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Dense plasma</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Over</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Nonlinear effect</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Terahertz emission during laser-plasma interaction: effect of electron temperature and collisions</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 14 (2020)</Volume>
			<Issue>Issue 4, August 2020</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Terahertz emission during laser-plasma interaction: effect of electron temperature and collisions</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.1007/s40094-020-00392-3</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Hitendra</FirstName>
				<LastName>K Malik</LastName>
				<Affiliation>Plasma Waves and Particle Acceleration Laboratory, Department of Physics, Indian Institute of Technology Delhi, New Delhi, India</Affiliation>
				<Identifier Source="ORCID">0000-0002-9432-8140</Identifier>
			</Author>
            			<Author>
                				<FirstName>Divya</FirstName>
				<LastName>Singh</LastName>
				<Affiliation>Rajdhani College, Delhi University, Delhi, New Delhi, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>AbstractThe electron-neutral collisions in the plasma become crucial with regard to the generation of THz radiation when thermal motion of the electrons is considerable. If we look at the mechanism of THz emission, this is only the movement/oscillations of the electrons which is responsible for the excitation of nonlinear current that generated the THz radiation. The present work aims to disclose the role of thermal motion of the plasma electrons to the resonance condition and the THz emission when two co-propagating super-Gaussian laser beams beat in the plasma. The dynamics of the plasma electrons and subsequent generation of nonlinear current are discussed in greater detail for the emission of THz radiation.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Terahertz radiation</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Laser</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Efficiency</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Ponderomotive force</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Super</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Electron temperature</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Gaussian laser</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Plasma interaction</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Tunable and reversible thermo-plasmonic hot spot imaging for temperature confinement</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 14 (2020)</Volume>
			<Issue>Issue 4, August 2020</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Tunable and reversible thermo-plasmonic hot spot imaging for temperature confinement</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.1007/s40094-020-00393-2</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>N.</FirstName>
				<LastName>S. Shnan</LastName>
				<Affiliation>Magneto‑plasmonic Lab, Laser and Plasma Research Institute, Shahid Beheshti University, Tehran, Iran

Department of Laser Physics, College of Science for Woman, University of Babylon, Babylon, Iraq</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>N.</FirstName>
				<LastName>Roostaei</LastName>
				<Affiliation>Magneto‑plasmonic Lab, Laser and Plasma Research Institute, Shahid Beheshti University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>S.</FirstName>
				<LastName>M. Hamidi</LastName>
				<Affiliation>Magneto‑plasmonic Lab, Laser and Plasma Research Institute, Shahid Beheshti University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0002-5298-2224</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>AbstractIn the present study, a novel tunable two-dimensional thermo-plasmonic grating based on gold nanorods was demonstrated by combining the plasmonic properties of the gold nanostructure and the applied external voltage. In this structure, a thin layer of the gold grating was typically deposited on a patterned polydimethylsiloxane substrate using the nanoimprint lithography method. The surface plasmon resonance of the fabricated plasmonic structure was excited by the surface plasmon imaging system based on a high numerical aperture objective lens and the charged coupled device camera. Based on the results, the number of the plasmonic hot spots due to the thermo-plasmonic effect increased by the external voltage, leading to an increase in this effect. Therefore, this reversible and tunable temperature confinement can be used as the controller of each element including cells in a defined micro-position.</Abstract>
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				<Param Name="value">2D grating</Param>
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						<Object Type="keyword">
				<Param Name="value">Nanoimprint lithography</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Plasmonic hot spot</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Plasmonic imaging system</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Temperature confinement</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Comparative study of behavior of electrical conductivity in KI‒Al2O3 and KI‒TiO2 heterostructure composites</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 14 (2020)</Volume>
			<Issue>Issue 4, August 2020</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Comparative study of behavior of electrical conductivity in KI‒Al2O3 and KI‒TiO2 heterostructure composites</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.1007/s40094-020-00394-1</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Suhail</FirstName>
				<LastName>Iqbal Wani</LastName>
				<Affiliation>Physical Chemistry Division, Department of Chemistry, Aligarh Muslim University, Aligarh 202002, Uttar Pradesh, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Nazli</FirstName>
				<LastName>Zeeshan</LastName>
				<Affiliation>Physical Chemistry Division, Department of Chemistry, Aligarh Muslim University, Aligarh 202002, Uttar Pradesh, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Rafiuddin</FirstName>
				<LastName></LastName>
				<Affiliation>Physical Chemistry Division, Department of Chemistry, Aligarh Muslim University, Aligarh 202002, Uttar Pradesh, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>AbstractThe present work reports development of binary KI–Al2O3 and KI–TiO2-based nanocomposites using simple solid-state reaction method and is characterized by X-ray diffraction, Fourier-transform infrared spectroscopy, scanning electron microscopy and impedance spectroscopy. The results show the effect of heterogeneously doped Al2O3 and TiO2 on the ionic conductivity of pure KI which is moderately conductive. The results supported the composite development in which the interface layer portrays a significant part in governing the bulk properties of the compound. Improvement in electrical conductivity is seen in the incorporation of Al2O3 and TiO2 dispersoid into the matrix of KI. With temperature, electrical conductivity increased and the activation energies were found to be decreasing. The activation energies for KI–Al2O3 and KI–TiO2 systems were 0.22 eV and 0.21 eV, respectively, in the temperature range 20‒400 °C. Dielectric constant increases with the increase in temperature in the entire temperature range studied attributed to the phenomenon of distortion of electric charges.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Dielectric constant</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Ionic conductivity</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Solid composites</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Ray diffraction</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">X</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Impedance spectroscopy</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>The effects of grounded electrode geometry on RF-driven cold atmospheric pressure plasma micro-jet</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 14 (2020)</Volume>
			<Issue>Issue 4, August 2020</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>The effects of grounded electrode geometry on RF-driven cold atmospheric pressure plasma micro-jet</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.1007/s40094-020-00395-0</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Davood</FirstName>
				<LastName>Hassanpour</LastName>
				<Affiliation>Advanced Plasma Laboratory, Faculty of Physics, University of Tabriz, Tabriz, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0003-1010-2775</Identifier>
			</Author>
            			<Author>
                				<FirstName>Sayyed‑Jalal</FirstName>
				<LastName>Pestehe</LastName>
				<Affiliation>Advanced Plasma Laboratory, Faculty of Physics, University of Tabriz, Tabriz, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0003-3224-4600</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>AbstractWith the argument that two-electrode DBD-like systems are much more operational than single-electrode systems in biomedical applications, targets sensitive to temperature and electric shock, the effects of parameters associated with the geometry of the grounded electrode such as its shape, size, and position it at the output of the atmospheric pressure RF plasma jet in two-electrode systems is investigated. By varying the position of the typical narrow ring grounded electrode on the dielectric tube toward the powered electrode, the ratio of the axial to radial electric field components depend on the externally applied potential to the plasma has been investigated and shown that the axial component of the electric field is maximized at certain position(s) of the grounded electrode. The analysis of the data indicates that there is an inverse relationship between the magnitude of the axial electric field in the plasma channel and the discharge ignition voltage, and a direct relationship with the plasma jet length. It is known that by increasing the width of the ground electrode until the full covering of dielectric, the jet length increases from the dielectric output to the neighborhood near the needle electrode, and reduces the discharge ignition threshold and consequently power consumption of the jet, but increasing its width to greater than the above values does not have a significant effect on jet output. It has also been shown that by tapering the dielectric end and fully covering it with its conical-shaped electrode, the output jet length increases and decreases its width.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Atmospheric pressure plasma jet</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">DBD</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Like)</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Electrode shape</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Grounded electrode geometry</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Jet length</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Industrial application of apodized gas sensor for on-line and in situ measurement of CO and CO2 concentration</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 14 (2020)</Volume>
			<Issue>Issue 4, August 2020</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Industrial application of apodized gas sensor for on-line and in situ measurement of CO and CO2 concentration</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.1007/s40094-020-00396-z</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Alireza</FirstName>
				<LastName>Khorsandi</LastName>
				<Affiliation>Department of Physics, University of Isfahan, Isfahan 81746‑73441, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0002-9086-718X</Identifier>
			</Author>
            			<Author>
                				<FirstName>Saeed</FirstName>
				<LastName>Ghavami Sabouri</LastName>
				<Affiliation>Department of Physics, University of Isfahan, Isfahan 81746‑73441, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0002-6200-4459</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>AbstractThe performance of an apodized gas sensor is demonstrated through simultaneous detection of CO and CO2 absorption lines around 1.57 µm in the recuperator channel of a gas-fired industrial furnace at Shahid Montazeri power plant (SMPP) industry. This led to the concentration measurement of targeted molecules as less than ~ 1% and 9.5%, respectively, at atmospheric pressure and 350 °C, indicating close consistency with the reference data reported by SMPP. A minimum detectable absorption of ~ 0.4 × 10−3, corresponding to a detection sensitivity of ~ 4.8 × 10−9 cm−1 Hz−1/2 is measured in this application.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Apodized gas sensor</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Tunable diode laser</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Wavelength modulation spectroscopy</Param>
			</Object>
					</ObjectList>
	</Article>
	</ArticleSet>
