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<ArticleSet>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Low-frequency electrostatic waves and chaotic motions in collisional superthermal plasmas</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 4, September &amp; October 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Low-frequency electrostatic waves and chaotic motions in collisional superthermal plasmas</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1704.45</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Mostafa</FirstName>
				<LastName>Mehdipoor</LastName>
				<Affiliation>Department of Physics, Faculty of Science, Gonbad Kavous University, Gonbad Kavous, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0001-8524-8248</Identifier>
			</Author>
            			<Author>
                				<FirstName>Yaghoob</FirstName>
				<LastName>Mohammadmoradi</LastName>
				<Affiliation>Department of physics, Aliabad Katoul Branch, Islamic Azad University, Aliabad Katoul, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0001-6462-0653</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 work, the dynamics and chaotic behavior of ion-acoustic (IA) traveling waves in a collisional plasma consisting of cold ions, superthermal electrons, and immobile neutral particles are studied. The effect of ion-neutral collisions is also considered here. Using the reductive perturbation technique, a forced modified Korteweg-de Vries (FMK-dV) equation is obtained in the presence of an externally applied force. The periodic, quasi-periodic, and chaotic motions of IA waves are investigated by considering three-dimensional phase portraits and time-series analysis. It is noted that ion-neutral collisional frequency, strength, and frequency of the external periodic force play an important role in controlling the dynamic motion of ion-acoustic waves. Moreover, it is found that the strength of the external perturbation can be considered as the main parameter for the transition from quasi-periodic motion to chaotic motion.</Abstract>
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            			<Object Type="keyword">
				<Param Name="value">Chaotic motions</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Collisional plasmas</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Forced modified K-dV equation</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Ion-acoustic waves</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Traveling waves</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Exploring elastic mechanics and radiation shielding efficacy in neodymium(III)-enhanced zinc tellurite glasses: A theoretical and applied physics perspective</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 4, September &amp; October 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Exploring elastic mechanics and radiation shielding efficacy in neodymium(III)-enhanced zinc tellurite glasses: A theoretical and applied physics perspective</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1704.44</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Hesham</FirstName>
				<LastName>M. H. Zakaly</LastName>
				<Affiliation>Department of Physics, Faculty of Science, Menoufia University, Shebin El Koom, Egypt

Istinye University, Faculty of Engineering and Natural Sciences, Computer Engineering Department, Istanbul, Turkey

Institute of Physics and Technology, Ural Federal University, Yekaterinburg, Russia</Affiliation>
				<Identifier Source="ORCID">0000-0002-7645-9964</Identifier>
			</Author>
            			<Author>
                				<FirstName>Yasser</FirstName>
				<LastName>S. Rammah</LastName>
				<Affiliation>Department of Physics, College of Science, Princess Nourah bint Abdulrahman University, Riyadh, Saudi Arabia.</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Shams</FirstName>
				<LastName>A. M. Issa</LastName>
				<Affiliation>Department of Basic and Applied Science, Collage of Engineering and Technology, Arab Academy of Science, Technology and Maritime Transport, Smart Village, Giza, Egypt.</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Nouf</FirstName>
				<LastName>Almousa</LastName>
				<Affiliation>Physics and Mathematical Engineering Department, Faculty of Electronic Engineering, Menoufia University, Menouf, Egypt.</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Adel</FirstName>
				<LastName>M. El-Refaey</LastName>
				<Affiliation>Department of Basic and Applied Science, College of Engineering and Technology, Arab Academy of Science,  Technology and Maritime Transport, Smart Village, Giza, Egypt</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Mohamed</FirstName>
				<LastName>Said Shams</LastName>
				<Affiliation>Physics and Mathematical Engineering Department, Faculty of Electronic Engineering, Menoufia University, Menouf, Egypt</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 work scrutinizes the radiation protection features and mechanical characteristics of neodymium zinc-tellurite of composition [(TeO2)70-(ZnO)30]1-x –(Nd2O3)x: x= 0-5 mol% in steps of 1 (TZNd1 – 5). The Makishima–Mackenzie&#039;s model was adopted for the computation of the Poisson&#039;s ratio (PR) and elastic moduli. WinXcom and EXABCal software&#039;s were performed to evaluate the radiation shielding parameters and buildup factors, respectively of TZNd-glasses. Results revealed that the increasing of Nd2O3 concentration in TZNd-glasses from 1 to 5 mol% had a positive effect on their elastic parameters: Young&#039;s modulus increased from 53.13 to 54.81GPa, bulk modulus changed from 31.95-33.65 GPa, and the PR varied from 0.222 to 0.228 for TZNd1 to TZNd5. There was a small increase in the Z/A as the Nd content increased, which leads to slight increase in TMSP of the particles. The mass attenuation coefficient increased in the order TZNd1&lt; TZNd2&lt; TZNd3 &lt; TZNd4 &lt; TZNd5. The maximum value of LAC obtained at 15 keV were 246, 249, 253, 257, and 260 cm-1 for TZNd1, TZNd2, TZNd3, TZNd4, and TZNd5, respectively. The HVT varies inversely with the linear attenuation coefficient. Throughout the considered energy spectrum the range of   for the glasses varied from 22.65 – 40.22, 22.64 – 40.25, 22.64 – 40.29, 22.63 – 40.32, and 22.63 – 40.36 for TZNd1, TZNd2, TZNd3, TZNd4, and TZNd5, respectively. The values of fast neutron removal cross section  showed a steady increase as the partial densities of Nd and oxygen of the TZNd-glass systems increased. Generally, one can conclude that the additive of Nd2O3 to TeO2-ZnO glasses leads to enhance their mechanical properties and increase their ability to absorb neutron and photon to apply in nuclear medicine applications.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Radiation protection</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">WinXcom</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Tellurite</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">EXABCal code</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Mechanical features</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Role of dust on the gradient driven instability in an E×B plasma</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 4, September &amp; October 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Role of dust on the gradient driven instability in an E×B plasma</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1704.43</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Munish</FirstName>
				<LastName>Munish</LastName>
				<Affiliation>Department of Physics, Gargi College, University of Delhi, Delhi, India

Plasma Science and Technology Laboratory, Department of Physics, Indian Institute of Technology Delhi, New Delhi 110016, India</Affiliation>
				<Identifier Source="ORCID">0000-0003-4258-5222</Identifier>
			</Author>
            			<Author>
                				<FirstName>Dimple</FirstName>
				<LastName>Sharma</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>Babu</FirstName>
				<LastName>Lal</LastName>
				<Affiliation>Department of Physics, Swami Sharaddhanand College Alipur, University of Delhi, India.</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Sukhmander</FirstName>
				<LastName>Singh</LastName>
				<Affiliation>Plasma Waves and Electric Propulsion Laboratory, Department of Physics, Central University of Rajasthan, Ajmer, Kishangarh- 305817, India</Affiliation>
				<Identifier Source="ORCID">0000-0002-6761-1303</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>The E*B plasma systems play an important role in the technologies like electric space propulsion and magnetized plasma sources used in plasma material interaction / surface processing. However, due to the gradient in plasma density, collisions and external fields such systems become prone to the instabilities and also dust particles are generated during the plasma processing. Hence, this article discusses the growth of gradient driven instability in a cross-field plasma, where both the ions and the electrons are magnetized and dust particles also exist. Using the fluid approach, we write basic equations and then derive an equation in terms of perturbed potential. The unperturbed part of this equation leads to the dispersion equation which is solved numerically for obtaining the growth rate of the instability. The normalized form of the growth rate is investigated in greater detail under the effect of dust density, dust mass, dust temperature, external magnetic field, ion temperature and ion temperature gradient.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Dust particles</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Film deposition</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Plasma processing</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Dust mass</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Gradient driven instability</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Space propulsion</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Temperature gradient</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Phase transformation; structural and optical properties of two dimensional MoO3</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 4, September &amp; October 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Phase transformation; structural and optical properties of two dimensional MoO3</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1704.42</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Mohammad</FirstName>
				<LastName>Reza Khanlary</LastName>
				<Affiliation>Department of Physics, Imam Khomeini International University, Qazvin, Iran.</Affiliation>
				<Identifier Source="ORCID">0000-0003-1499-853X</Identifier>
			</Author>
            			<Author>
                				<FirstName>Azita</FirstName>
				<LastName>Keshavarz</LastName>
				<Affiliation>Department of Physics, Imam Khomeini International University, Qazvin, Iran.</Affiliation>
				<Identifier Source="ORCID">0000-0003-1607-6037</Identifier>
			</Author>
            			<Author>
                				<FirstName>Reza</FirstName>
				<LastName>Shakouri</LastName>
				<Affiliation>Department of Physics, Imam Khomeini International University, Qazvin, Iran.</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Milad</FirstName>
				<LastName>Parhizkari</LastName>
				<Affiliation>Department of Physics, Imam Khomeini International University, Qazvin, Iran.</Affiliation>
				<Identifier Source="ORCID">0000-0003-4599-3846</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>Thin-layered materials from transition-metal dichalcogenides family and their preforms such as molybdenum three oxides (MoO3) exhibit great potential as active material in optoelectronics. Stable materials of few atoms thick have shown emerging capabilities in this area. In this article, we report the synthesis of MoO3 nanostructures by spray pyrolysis method. We will, perhaps for the first time, show that by varying the hot plate temperature from 350 to 4400C, a phase transformation reveal from h-MoO3 to α-MoO3. By annealing the prepared α-MoO3 sample a preferential orientation of (002) crystal plane is induced. A large band gap of 2.8 eV for the prepared MoO3 film was obtained from the transmission spectra. The Raman vibrational modes were investigated for excitation wavelength at 532 nm using MoO3 films and for a heterostructured MoO3/MoS2 film .Better crystallinity and decrease in defects intensity, as an advantage of MoO3 hybridization can be achieved by proper fabricating the heterostructure sample.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Thin Film</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Band gap</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Heterostructure</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Raman spectra</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Approximate solutions of the Dirac equation with Deformed Woods-Saxon potential including a Hellmann like tensor interaction</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 4, September &amp; October 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Approximate solutions of the Dirac equation with Deformed Woods-Saxon potential including a Hellmann like tensor interaction</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1704.41</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Uduakobong</FirstName>
				<LastName>S. Okorie</LastName>
				<Affiliation>Department of Physics, Akwa Ibom State University, Ikot Akpaden, Nigeria</Affiliation>
				<Identifier Source="ORCID">0000-0002-5660-0289</Identifier>
			</Author>
            			<Author>
                				<FirstName>Akpan</FirstName>
				<LastName>N. Ikot</LastName>
				<Affiliation>Department of Physics, Theoretical Physics Group, University of Port Harcourt, Choba, Nigeria</Affiliation>
				<Identifier Source="ORCID">0000-0002-1078-262X</Identifier>
			</Author>
            			<Author>
                				<FirstName>Monday</FirstName>
				<LastName>E. Udoh</LastName>
				<Affiliation>Department of Physics, University of Uyo, Uyo. Nigeria.</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Sylvester</FirstName>
				<LastName>A. Ekong</LastName>
				<Affiliation>Department of Physics, Akwa Ibom State University, Ikot Akpaden, Nigeria</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Collins</FirstName>
				<LastName>O. Edet</LastName>
				<Affiliation>Department of Physics, Cross River University of Technology, Calabar, Nigeria</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Ridha</FirstName>
				<LastName>Horchani</LastName>
				<Affiliation>Department of Physics, College of Science, Sultan Qaboos University, Al-Khod, Muscat, Sultanate of Oman</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Gaotsiwe</FirstName>
				<LastName>J Rampho</LastName>
				<Affiliation>Department of Physics, University of South Africa, Florida 1710, Johannesburg, South Africa</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>An Approximate bound state solutions of the Dirac equation under the spin and pseudospin symmetries for the deformed Woods-Saxon potential with a Hellmann-like tensor interaction was examined. With the help of the Nikiforov-Uvarov functional analysis (NUFA) method and an approximation scheme, the analytical and numerical energies of the combined potential were obtained for both symmetries, for different quantum numbers. Degeneracies were observed in the energy values in the absence of the tensor interaction and these degeneracies were removed with the help of the Hellmann-like tensor interaction. The variations of the energies for spin and pseudospin symmetries were studied for various values of the quantum numbers and deformation parameters. Our study shows that the relativistic energies obtained are very sensitive to the quantum numbers and the deformation parameter.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Dirac equation</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Bound state</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">NUFA method</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Potential function</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Tensor interaction</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Quantum mechanical treatment of Shannon entropy measure and energy spectra of selected diatomic molecules with the modified Kratzer plus generalized inverse quadratic Yukawa potential model</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 4, September &amp; October 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Quantum mechanical treatment of Shannon entropy measure and energy spectra of selected diatomic molecules with the modified Kratzer plus generalized inverse quadratic Yukawa potential model</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1704.40</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<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>Fina</FirstName>
				<LastName>O. Faithpraise</LastName>
				<Affiliation>Department of Physics, University of Calabar, Calabar, Nigeria.</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Eddy</FirstName>
				<LastName>S. William</LastName>
				<Affiliation>Theoretical Physics Group, Department of Physics, School of Pure and Applied Sciences, Federal University of Technology, Ikot Abasi, Nigeria.</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Peter</FirstName>
				<LastName>O. Okoi</LastName>
				<Affiliation>Department of Physics, University of Calabar, Calabar, Nigeria.</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Efiong</FirstName>
				<LastName>A. Ibanga</LastName>
				<Affiliation>Department of Physics, National Open University of Nigeria, Jabi, Abuja, 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 research, we have obtained the energy eigenvalues and the corresponding normalized eigenfunction for the linear combination of the modified Kratzer and generalized inverse quadratic Yukawa potential using two different analytical methods: the exact quantization rule and the formula method respectively. The obtained normalized wave function is used to study the Shannon entropy in position and momentum spaces for the ground and first excited states. It was observed that the Shannon entropy in position space decreases as the screening parameter is increased and also increases in momentum space as the screening parameter is increased in such a way that their sum satisfies the Bialynicki-Birula-Mycielski (BBM) inequality that stipulated lower bound state of Sr+Sp&gt;D(l+In(pi)) . Numerical results were generated for some selected diatomic molecules such as N2, CO, NO, and CH which agreed with other works in the literature. The content of this research finds application in atomic and molecular physics, quantum chemistry, and physics.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Schrödinger equation</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Bialynicki-Birula-Mycielski inequality</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Energy spectra</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Shannon Entropy</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Wave function</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Investigation of MHD instabilities in tokamak plasmas Using biorthogonal decomposition of Mirnov coil data</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 4, September &amp; October 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Investigation of MHD instabilities in tokamak plasmas Using biorthogonal decomposition of Mirnov coil data</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1704.39</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Habib</FirstName>
				<LastName>Mehrniya</LastName>
				<Affiliation>Plasma Physics Research Center, Science and Research Branch, Islamic Azad University, P.O. Box: 14665‑678, Tehran, 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>
            			<Author>
                				<FirstName>Ahmad</FirstName>
				<LastName>Salar Elahi</LastName>
				<Affiliation>Plasma Physics Research Center, Science and Research Branch, Islamic Azad University, P.O. Box: 14665‑678, 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>Spatiotemporal signal analysis is essential in investigating magnetic fluctuations of tokamak plasmas. Signal analysis of Mirnov coils through biorthogonal decomposition (BD) can reveal the spatial structure and time evolution of magnetohydrodynamic (MHD) instabilities in a tokamak. This technique is comparable to singular value decomposition in terms of formulation. The present study calculates the probability of instability modes&#039; presence and identifies the dominant modes using the method above. Moreover, the relationship between the singular value entropy as a signal characteristic and magnetic field oscillations of Mirnov coils in the IR-T1 tokamak is investigated. This study evaluated the presence of active modes with and without applying a resonant helical field. The results indicate that when L=2 and L=3 are applied independently, the probability of m=2 &amp; 3 active modes is greater than when the resonant helical field is absent. In contrast, by combining these two, the likelihood of the presence of these modes is reduced.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Instability indicators</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Principal axes</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Singular values entropy</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Biorthogonal decomposition</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Optical imaging and magnetic field simulation of a DC circular planar magnetron sputtering discharge</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 4, September &amp; October 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Optical imaging and magnetic field simulation of a DC circular planar magnetron sputtering discharge</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1704.38</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Ahmad</FirstName>
				<LastName>Reza Rastkar</LastName>
				<Affiliation>Laser and Plasma Research Institute, Shahid Beheshti University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Ali</FirstName>
				<LastName>Reza Niknam</LastName>
				<Affiliation>Laser and Plasma Research Institute, Shahid Beheshti University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0002-1460-7677</Identifier>
			</Author>
            			<Author>
                				<FirstName>Mostafa</FirstName>
				<LastName>Salahshoor</LastName>
				<Affiliation>School of Physics, Iran University of Science and Technology, 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>In this paper, the optical images of glow discharge plasma and the finite element method simulation of the magnetic field strength in a balanced and two types of unbalanced DC circular planar magnetron sputtering sources are presented. The investigation showed that wherever the magnetic field strength is stronger, the intensity of light and the ionization are greater and consequently, the deposition is higher. The comparison of recorded optical images with the finite element simulation results of the magnetic field strength indicated the correlation between regions of high magnetic field strength and high light emission.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Magnetron sputtering</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Glow discharge plasma</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Finite element method</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Magnetic field distribu tion</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>Characterization of RF-driven atmospheric pressure plasma micro-jet plume</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 4, September &amp; October 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Characterization of RF-driven atmospheric pressure plasma micro-jet plume</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1704.37</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>The plasma parameters of an RF-driven plasma microjet in different applied RF powers, different positions from the outlet nozzle, and various argon flow rates are investigated. A double Langmuir probe is designed and constructed, then, the electron temperature, ion density, and saturation currents along the microjet axis at different positions such as top, mid, end and out of the microjet are measured. To avoid the collision, sparking, and corrosion effects, in high pressure plasmas, on the characteristic curve, the double Langmuir probe was reciprocated linearly perpendicular to the plasma jet with a frequency of 20 Hz. The four frequently used methods of the direct fitting of the theoretically obtained formula, double slope, turning point or Dote, and cutting or intercept method are explained and used to determine the electron excitation temperature from the experimental data and shown that they lead to similar results, so, the averaged value of these results used in the evaluations of plasma densities. The plasma number density and electron temperature were measured using DLP in the jet at different axial locations. The results for the electron excitation temperature from the DLP is compared with that of obtained from the emission spectrum of the plasma jet. It has been shown that the averaged electron excitation temperature obtained using optical emission spectroscopy (1.58eV) is within the 25% of that measured by the double Langmuir probe which is same as the early reported value by other researches.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Atmospheric pressure cold plasma microjet</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Electron temperature</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Langmuir double probe</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">RF microjet</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Optical emission spectroscopy</Param>
			</Object>
					</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>Journal of Theoretical and Applied Physics (JTAP)</PublisherName>
			<JournalTitle>The quantum fluctuations of charge and current in a driven nonlinear LC-circuit with a linear capacitor and a nonlinear inductor</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 17 (2023) JTAP</Volume>
			<Issue>Issue 4, September &amp; October 2023</Issue>
			<PubDate PubStatus="epublish">
                <Year>2023</Year>
                <Month>11</Month>
                <Day>17</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>The quantum fluctuations of charge and current in a driven nonlinear LC-circuit with a linear capacitor and a nonlinear inductor</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.57647/J.JTAP.2023.1704.36</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Ameneh</FirstName>
				<LastName>Zamani</LastName>
				<Affiliation>Department of Physics, University of Qom, Qom, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Hasan</FirstName>
				<LastName>Pahlavani</LastName>
				<Affiliation>Department of Physics, University of Qom, Qom, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0002-8784-3240</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2023</Year>
				<Month>11</Month>
				<Day>17</Day>
			</PubDate>
		</History>
		<Abstract>A nonlinear soft-core ferrite (ferromagnetic material) inductor that obeys of a polynomial current-magnetic flux relationship (typically a power series in the magnetic flux) is introduced. The quantum Hamiltonian of a nonlinear LC-circuit consisting of a linear capacitor and a nonlinear inductor under the inﬂuence of an external field is found. The energy spectrum is obtained and the quantum behavior of the nonlinear coefficients is studied numerically. The quantum fluctuations of electric charge and current are obtained as a function of the characteristic parameters then the time-dependent of the characteristic parameters and the digger squeezing is analyzed by numerical approach.</Abstract>
		<ObjectList>
            			<Object Type="keyword">
				<Param Name="value">Numerical Solution</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Duﬃng’ s electrical oscillator</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Nonlinear inductor</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Quantum fluctuation</Param>
			</Object>
						<Object Type="keyword">
				<Param Name="value">Quantum LC-circuit</Param>
			</Object>
					</ObjectList>
	</Article>
	</ArticleSet>
