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<ArticleSet>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Electrodeposition of cobalt oxide thin films for potential applications</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 2, May &amp; June 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Electrodeposition of cobalt oxide thin films for potential applications</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1702.25</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Sandra</FirstName>
				<LastName>Augustine</LastName>
				<Affiliation>Department of Physics and Industrial Physics, Nnamdi Azikiwe University, Awka, Nigeria</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Azubike</FirstName>
				<LastName>Josiah Ekpunobi</LastName>
				<Affiliation>Department of Physics and Industrial Physics, Nnamdi Azikiwe University, Awka, Nigeria</Affiliation>
				<Identifier Source="ORCID">0000-0002-5111-7298</Identifier>
			</Author>
            			<Author>
                				<FirstName>Diemiruaye</FirstName>
				<LastName>Mimi Jeroh</LastName>
				<Affiliation>Department of Physics and Industrial Physics, Nnamdi Azikiwe University, Awka, Nigeria</Affiliation>
				<Identifier Source="ORCID">0000-0002-1622-0337</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>Cobalt oxide thin films at varied molar concentrations were prepared by electrodeposition technique. Ultraviolet-Visible (UV/VIS) analysis conducted on the grown films revealed blue shift in the absorption edge at increased molar concentrations, which is a consequence of band gap widening. The band gap values (3.65 eV to 3.85 eV) in this research are greater than the value (2.4 eV) for the bulk phase of cobalt oxide. This increase in band gap can be likened to higher concentration effect and quantum-size phenomenon. Scanning Electron Microscopy (SEM) analysis indicated a porous nature for the material, suggesting its ability in absorbing ultraviolet (UV) radiation, thus confirming its use as an absorber material for solar cells fabrication. Energy Dispersive X-ray (EDX) study confirmed the growth of cobalt oxide. X-ray diffraction (XRD) analysis confirms the crystalline nature of the films with grain sizes within the range of 0.7 nm to 1 nm for varied molar concentrations. Electrical studies reveal a linear relationship of resistivity values with molar concentrations, while the conductivity values reveal inverse relationship with molar concentration.</Abstract>
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            			<Object Type="keyword">
				<Param Name="value">Blue-shift</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Cobalt oxide</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Crystalline</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Molar concentrations</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Band widening</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Excitation of R- and L-waves by laser propagation through over-dense magnetized plasma and their verification</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 2, May &amp; June 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Excitation of R- and L-waves by laser propagation through over-dense magnetized plasma and their verification</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1702.24</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Gaurav</FirstName>
				<LastName>Kumar</LastName>
				<Affiliation>Department of Physics, Indian Institute of Technology, New Delhi, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Hitendra</FirstName>
				<LastName>K. Malik</LastName>
				<Affiliation>Plasma Science and Technology Laboratory, Department of Physics, Indian Institute of Technology Delhi, New Delhi 110016, India</Affiliation>
				<Identifier Source="ORCID">0000-0002-9432-8140</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>Laser-plasma interaction is a fascinating subject in view of its various applications in wave generation, particle acceleration, radiation generation, etc. The laser beam gets reflected at the vacuum-plasma interface if the plasma density is equal or larger than the critical density. However, in the presence of strong magnetic field in the order of kilo Tesla, the beam can travel some distance through over-dense plasma. Here E×B heating and pondermotive force play role for the laser beams to propagate through the over-dense plasma. In the present article, taking the external magnetic field along the propagation direction of the laser beam we have observed the R- and L- waves to be excited. The applied magnetic field is chosen in such way that the laser frequency 𝜔𝑙 falls between the electron cyclotron frequency 𝜔𝑐𝑒 and ion cyclotron frequency 𝜔𝑐𝑖. Under this situation, it generates only an R-wave. If the laser frequency is considered to be less than the ion cyclotron frequency ( 𝜔𝑙𝑎𝑠𝑒𝑟&lt;𝜔𝑐𝑖) then an L-wave is additionally generated. In both the cases, an electrostatic disturbance is also formed with different but significant electric field amplitudes. We simulate these R- and L-waves in 1-D by using Particle-in-Cell (PIC) simulation using the EPOCH-4.17.10. Specifically, the electric and magnetic fields are studied that are associated with these waves, and the waves are verified based on the dispersion relation and the polarization studies.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Electron cyclotron frequency</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Ion cyclotron frequency</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">L-wave</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Particle in cell</Param>
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						<Object Type="keyword">
				<Param Name="value">R-wave</Param>
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	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Enhancement of Seebeck coefficient with full spin polarization of CsMgN2 Thin Films: A DFT Study</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 2, May &amp; June 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Enhancement of Seebeck coefficient with full spin polarization of CsMgN2 Thin Films: A DFT Study</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1702.23</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Rohangiz</FirstName>
				<LastName>Ashtari Faregh</LastName>
				<Affiliation>Department of Physics, Hamedan Branch, Islamic Azad University, Hamedan, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Arash</FirstName>
				<LastName>Boochani</LastName>
				<Affiliation>Department o Physics, Kermanshah Branch, Islamic Azad University, Kermanshah, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0002-2383-4169</Identifier>
			</Author>
            			<Author>
                				<FirstName>Seyedeh</FirstName>
				<LastName>Razyeh Masharian</LastName>
				<Affiliation>Department of Physics, Hamedan Branch, Islamic Azad University, Hamedan, 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>Structural, electronic, and thermoelectric properties of the CsMgN2 compound with its thin film films of Cs-Mg and Mg-N terminations have been studied in a First-Principles study. The total energy changes (E-V) versus the unit cell volume of bulk show better stability in the ferromagnetic than the non-magnetic phase. The E-V diagrams of film Cs-Mg and Mg-N terminations have the ground state points at the ferromagnetic phase. The derivative bulk modulus of Cs-Mg termination is like the bulk phase, which refers to the ionic bonds between atoms.

The magnetic moment of the bulk and two mentioned terminations have the integers of 3µB, 10 µB, and 13 µB, respectively. The DOS and bandstructure diagrams by the mBJ and GGA approximations confirm the half-metallic behavior of the bulk and the mentioned terminations. The energy gaps of their semiconductor phase are 1.40eV, 0.64eV, and 0.20eV, for the bulk, Cs-Mg, and Mg-N terminations, respectively. The Seebeck coefficient of Cs-Mg termination in 200K temperature is much higher than the bulk case. The merit figure of coefficient (ZT) shows that bulk and mentioned terminations have high thermoelectric quality at up spin.</Abstract>
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            			<Object Type="keyword">
				<Param Name="value">Electronic</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Thermoelectric</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">DFT</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">CsMgN2</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Dopant and milling time effect on impedance and electrical properties of perovskite ceramics</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 2, May &amp; June 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Dopant and milling time effect on impedance and electrical properties of perovskite ceramics</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1702.22</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Shristi</FirstName>
				<LastName>Chaudhary</LastName>
				<Affiliation>Chandigarh University Gharuan Mohali Punjab, India</Affiliation>
				<Identifier Source="ORCID">0000000188642830</Identifier>
			</Author>
            			<Author>
                				<FirstName>Mikanshi</FirstName>
				<LastName>Chaudhary</LastName>
				<Affiliation>Chandigarh University Gharuan Mohali Punjab, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Sheela</FirstName>
				<LastName>Devi</LastName>
				<Affiliation>Chandigarh University Gharuan Mohali Punjab, India</Affiliation>
				<Identifier Source="ORCID">0000000291830290</Identifier>
			</Author>
            			<Author>
                				<FirstName>Shilpi</FirstName>
				<LastName>Jindal</LastName>
				<Affiliation>Chandigarh University Gharuan Mohali Punjab, India</Affiliation>
				<Identifier Source="ORCID">0000000172956739</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>Tungsten doped Barium Titanate (BT) with composition BaW0.05Ti0.95O3 (BWT) were prepared by using ball milling technique for different hours (10h, 20h and 30h). In the present paper, the microstructural, dielectric and impedance studies are discussed. The microstructural studies using XRD data reveals the formation of single phased tetragonal structure and perovskite structure. The dielectric properties of BT nanoceramics were significantly enhanced by the partial replacement of W (at B site) showing the diffuse phase transition at 80°C. Dielectric loss rises as the temperature rises. There is increase in charge carrier mobility which results in increased polarization and significant dielectric loss. Additionally, compared to the un-milled BWT ceramic sample, the 30h milled had superior dielectric characteristics with high dielectric constant and reduced loss. The nature of the phase transition was confirmed by the Curie-Weiss law and the ferroelectric analysis was carried by well-established P-E loops. The impedance studies were carried out by plotting Nyquist plots. The ac conductivity plot follows Arrhenius relation and the calculated activation energy confirms the negative temperature coefficient of resistance (NTCR) behavior of the material.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">SEM</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">XRD</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Barium titanate</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Ferroelectrics</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">PE</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Numerical investigations of electron-self-injection in different shaped bubbles in wakefield acceleration</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 2, May &amp; June 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Numerical investigations of electron-self-injection in different shaped bubbles in wakefield acceleration</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1702.21</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Sonu</FirstName>
				<LastName>Kumar</LastName>
				<Affiliation>Department of Physics, Indian Institute of Technology Delhi, New Delhi - 110016, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Dhananjay</FirstName>
				<LastName>K Singh</LastName>
				<Affiliation>Department of Physics, PKRM College, Dhanbad - 826004, Jharkhand, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Hitendra</FirstName>
				<LastName>K. Malik</LastName>
				<Affiliation>Plasma Science and Technology Laboratory, Department of Physics, Indian Institute of Technology Delhi, New Delhi 110016, India</Affiliation>
				<Identifier Source="ORCID">0000-0002-9432-8140</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>Electron-self-injection in bubble wakefield acceleration is the new concept for acceleration of electrons inside bubble. In this technique, self-injected plasma electrons have been used for acceleration whose advantage is that there is no need of external source of electrons. In our case, we have carried out numerical investigations of self-injected plasma electrons in different shaped bubbles such as spherical, longitudinal ellipsoid and transverse ellipsoid bubble. For these numerical investigations, by carrying out relativistic Hamiltonian analysis of plasma electrons, we have used 4th order Runge-Kutta (RK) method by employing MATLAB ode45, a nonstiff differential equations solver. We have discussed different parameters such as impact parameter, radius of bubble, bubble velocity for their effect on the formation of bubbles with different shapes and self-injection of the electrons.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Energy gain</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Self-injection</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Bubble shape</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Bubble wakefield acceleration</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Structural and electronic properties of Li_n, B_n, N_n and O_n (n=1-4) clustering on graphene: Density functional theory calculations with dispersive forces correction</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 2, May &amp; June 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Structural and electronic properties of Li_n, B_n, N_n and O_n (n=1-4) clustering on graphene: Density functional theory calculations with dispersive forces correction</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1702.20</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Malika</FirstName>
				<LastName>Gallouze</LastName>
				<Affiliation>Department of Theoretical Physics, Physics Faculty, University of Science and Technologie Houari Boumediene</Affiliation>
				<Identifier Source="ORCID">0000-0003-1745-5514</Identifier>
			</Author>
            			<Author>
                				<FirstName>Mahrez</FirstName>
				<LastName>Drir</LastName>
				<Affiliation>Department of Theoretical Physics, Physics Faculty, University of Science and Technologie Houari Boumediene</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Abdelhafid</FirstName>
				<LastName>Kellou</LastName>
				<Affiliation>Department of Theoretical Physics, Physics Faculty, University of Science and Technologie Houari Boumediene</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>We have performed density functional theory calculations to study the adsorption of Li, B, N, and O clusters on graphene to clarify the interaction of these atoms with a graphene sheet. The stable structure, the adsorption energy, and the density of states (DOS) of atom-graphene systems are calculated. The obtained results of the structural, adsorption and interaction energies show that light atoms on graphene show physisorption/chemisorption mechanisms with and without clusteringoccurrence. More interestingly, the formation of diatomic molecules is noticed. For example, Li atoms prefer to be physisorbed where as B atoms prefer the clustering configuration on the graphene sheet. For N and O atoms, the results show that the formation of molecules on a graphene sheet is preferred. The densities of states calculations have been performed to study the electronic properties of the studied systems. The results show that electronic structures are affected by the increasing concentration and the nature of adsorbed light atoms.</Abstract>
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				<Param Name="value">DFT</Param>
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				<Param Name="value">Adsorption</Param>
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						<Object Type="keyword">
				<Param Name="value">Physical properties</Param>
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						<Object Type="keyword">
				<Param Name="value">Van de Waals</Param>
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	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Investigation of plasma-activated water effects on preservation and physicochemical properties of Petroselinum crispum and Lepidium sativum</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 2, May &amp; June 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Investigation of plasma-activated water effects on preservation and physicochemical properties of Petroselinum crispum and Lepidium sativum</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1702.19</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Meysam</FirstName>
				<LastName>Nikpour</LastName>
				<Affiliation>Plasma Technology Research Core, Faculty of Science, University of Mazandaran, Babolsar, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0002-0046-4775</Identifier>
			</Author>
            			<Author>
                				<FirstName>Farshad</FirstName>
				<LastName>Sohbatzadeh</LastName>
				<Affiliation>Department of Atomic and Molecular Physics, Faculty of Basic Sciences, University of Mazandaran, Babolsar, Mazandaran 47416‑95447, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Ehsan</FirstName>
				<LastName>Nazifi</LastName>
				<Affiliation>Department of Atomic and Molecular Physics, Faculty of Basic Sciences, University of Mazandaran, Babolsar, Mazandaran 47416‑95447, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Saeed</FirstName>
				<LastName>Mirzanejhad</LastName>
				<Affiliation>Department of Atomic and Molecular Physics, Science Faculty, University of Mazandaran, Babolsar, 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>The present study aims at highlighting plasma, plasma-activated water (PAW) in particular, as a means of alternative, an innovative and unique method for its application in different aspects of food and vegetable processing and preservation. To investigate the effect of PAW on nutrient retention in vegetables, an experimental set was used to produce PAW that processes deionized water (DI). The concentrations of reactive species in PAW were calculated to compare their effect on nutrient retention. Then, the vegetables were washed with DI and PAW for 20 minutes. The samples were stored at 4 ° C for 14 days. Immediately after washing and on the seventh and fourteenth days, nutrient content levels were measured. The results showed that using PAW causes the nutrients to remain in the vegetables for a longer time. We show that nutrient persistence in vegetables depends on the concentration and the type of reactive species in PAW.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Plasma-activated water (PAW)</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Preservation</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Fresh vegetables</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Physicochemical properties</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Magnetic susceptibility and Magnetocaloric effect of Frost-Musulin potential subjected to Magnetic and Aharonov-Bohm (Flux) fields for CO and NO diatomic molecules</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 2, May &amp; June 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Magnetic susceptibility and Magnetocaloric effect of Frost-Musulin potential subjected to Magnetic and Aharonov-Bohm (Flux) fields for CO and NO diatomic molecules</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1702.18</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Eddy</FirstName>
				<LastName>Sunday William</LastName>
				<Affiliation>Department of Physics, Faculty of Physical sciences, University of Calabar, Calabar, Nigeria</Affiliation>
				<Identifier Source="ORCID">0000-0002-5247-5281</Identifier>
			</Author>
            			<Author>
                				<FirstName>Stanley</FirstName>
				<LastName>C. Onye</LastName>
				<Affiliation>Department of Computer Science, Faculty of Computing, Air Force Institute of Technology, Kaduna, Nigeria</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Akpan</FirstName>
				<LastName>Ndem Ikot</LastName>
				<Affiliation>Theoretical Physics Group, Department of Physics, University of Uyo, Uyo, Nigeria</Affiliation>
				<Identifier Source="ORCID">0000-0002-1078-262X</Identifier>
			</Author>
            			<Author>
                				<FirstName>Arthur</FirstName>
				<LastName>N. Nwachukwu</LastName>
				<Affiliation>Department of Physics, Alex Ekwueme Federal University Ndufu-Alike, Ebonyi State, Nigeria</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Etido</FirstName>
				<LastName>P Inyang</LastName>
				<Affiliation>Department of Physics, National Open University of Nigeria, Jabi, Abuja, Nigeria</Affiliation>
				<Identifier Source="ORCID">0000-0002-5031-3297</Identifier>
			</Author>
            			<Author>
                				<FirstName>Ituen</FirstName>
				<LastName>B. Okon</LastName>
				<Affiliation>Department of Physics, University of Uyo, Uyo, Nigeria</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Ita</FirstName>
				<LastName>Okon Akpan</LastName>
				<Affiliation>Department of Physics, Faculty of Physical sciences, University of Calabar, Calabar, Nigeria</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Benedict</FirstName>
				<LastName>I. Ita</LastName>
				<Affiliation>Department of Pure and Applied Chemistry, University of Calabar, Calabar, Nigeria</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>In this paper, we perform a nonrelativistic study of Frost-Musulin potential (FMP) impacted by the external magnetic and AB flux fields for the CO and NO diatomic molecules using the Nikiforov-Uvarov method with the Greene-Aldrich approximation to the centrifugal barrier. The numerical computation of the proposed potential reveals that the combined impact of the magnetic and AB flux fields completely removes the degeneracy of the energy spectra and controls the behavior of the magnetocaloric effect (MCE) by acting as a regulating factor to cool or heat the MCE. Also, the thermomagnetic plots obtained for the analyzed dimer molecules agreed perfectly with previous work. This research has the potential to be applied in molecular physics and MCE studies for a variety of molecules.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Schrödinger equation</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Nikiforov-Uvarov method</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Thermomagnetic properties</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Theoretical study of ISB conduction optical absorption and impurity binding energy associated with lowest excited states in QW with a new modulated potential</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 2, May &amp; June 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Theoretical study of ISB conduction optical absorption and impurity binding energy associated with lowest excited states in QW with a new modulated potential</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1702.17</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Redouane</FirstName>
				<LastName>En-nadir</LastName>
				<Affiliation>Le Mans Université, Faculty of sciences, University of Sidi Mohamed Ben Abdullah, Fez, Morocco</Affiliation>
				<Identifier Source="ORCID">0000-0002-5064-0028</Identifier>
			</Author>
            			<Author>
                				<FirstName>Haddou</FirstName>
				<LastName>El-ghazi</LastName>
				<Affiliation>Le Mans Université, Faculty of sciences, University of Sidi Mohamed Ben Abdullah, Fez, Morocco

ENSAM, Hassan-II University, Casablanca, Morocco</Affiliation>
				<Identifier Source="ORCID">0000-0002-2139-2360</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>This paper provides a theoretical investigation of the ground and first excited-states donor impurity binding energy and the linear and nonlinear optical absorption coefficients in quantum well with novel modulated potential called Redouane-Haddou potential (RHP). Within the effective-mass theory, the Schrödinger equation has been calculated numerically using the finite element method. The analytical expressions of the optical absorption coefficients are obtained within compact density matrix theory. Our results reveal that the A-parameter has a significant influence on the confinement profile and electron states, therefore, the binding energy as well as the optical properties of the investigated system. It increases the binding energy and redshift (blueshift) associated with drop (improvement) of the linear and nonlinear optical absorption coefficients related to 2p→1s,2p→2s, and 3s→2p transitions. Moreover, it is noticed that with an appropriate choice of the A-parameter and structure dimension, the optical response of the investigated system can be tailored in a controllable manner.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Optical absorption</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Quantum well</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">RHP potential</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Binding energy</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Effect of collisions, ionisation and non-extensivity on sheath formation in an electronegative warm plasma under electron emission from the wall</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 2, May &amp; June 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Effect of collisions, ionisation and non-extensivity on sheath formation in an electronegative warm plasma under electron emission from the wall</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1702.16</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Yetendra</FirstName>
				<LastName>Prasad Jha</LastName>
				<Affiliation>Plasma Science and Technology Laboratory, Department of Physics, Indian Institute of Technology Delhi, New Delhi 110016, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Mayank</FirstName>
				<LastName>Kumar</LastName>
				<Affiliation>Department of Mechanical Engineering, Indian Institute of Technology Delhi, New Delhi, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Hitendra</FirstName>
				<LastName>K. Malik</LastName>
				<Affiliation>Plasma Science and Technology Laboratory, Department of Physics, Indian Institute of Technology Delhi, New Delhi 110016, India</Affiliation>
				<Identifier Source="ORCID">0000-0002-9432-8140</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>The effect of collisions, ionisation and non-extensivity is studied numerically in an electronegative warm plasma associated with electron emission from the wall. Electrostatic potential, space charge density, net negative charge density and emitted electron beam density are plotted with the normalised distance to see the effects of aforesaid parameters The negative ion is described with fluid equations to see it’s effect of the mass ratio (negative ion to positive ion) on emitted electron beam density inside the sheath. The three types of electronegative plasma taken are CF_4, O_2 and C_60. The emitted beam electron density is more in number at the wall for higher collisional and ionisation case and less in higher mass ratio. For super-extensive case the emitted beam electrons is lesser than compared to the Boltzmann distributed electrons. The sheath thickness is found to be more in higher mass ratio, emitted beam electrons and super -extensive case while for higher collisional and ionisation case the sheath thickness is less.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Electric potential</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Plasma-material interaction</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Secondary electron emission</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Sheath thickness</Param>
			</Object>
					</ObjectList>
	</Article>
	</ArticleSet>
