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<ArticleSet>
		<Article>
		<Journal>
			<PublisherName>OICC PRESS</PublisherName>
			<JournalTitle>Effects of mixed electric field on characterization of electrohydrodynamics drying system</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 16 (2022)</Volume>
			<Issue>Issue 1, March 2022</Issue>
			<PubDate PubStatus="epublish">
                <Year>2022</Year>
                <Month>12</Month>
                <Day>11</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Effects of mixed electric field on characterization of electrohydrodynamics drying system</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.30495/jtap.162201</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Amir</FirstName>
				<LastName>Abbas Heidari</LastName>
				<Affiliation>Laser and Plasma Research Institute, Shahid Beheshti University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0001-9802-7487</Identifier>
			</Author>
            			<Author>
                				<FirstName>Pourya</FirstName>
				<LastName>Seyfi</LastName>
				<Affiliation>Laser and Plasma Research Institute, Shahid Beheshti University, Evin, Tehran 1983963113, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Ahmad</FirstName>
				<LastName>Khademi</LastName>
				<Affiliation>Laser and Plasma research institute, Shahid Beheshti University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0002-0411-6444</Identifier>
			</Author>
            			<Author>
                				<FirstName>Hamid</FirstName>
				<LastName>Ghomi</LastName>
				<Affiliation>Laser and Plasma Research Institute, Shahid Beheshti University, Evin, Tehran 1983963113, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0003-2203-5194</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2022</Year>
				<Month>12</Month>
				<Day>11</Day>
			</PubDate>
		</History>
		<Abstract>In this paper, we present a new structure of applying two electrical power supplies to generate ionic wind. In
this configuration, two power supplies were applied simultaneously with a modulated voltage to an electrohydrodynamic
(EHD) system then corona discharge parameters and EHD thrust characterization was investigated
by a corona dryer mechanism. The EHD thrust experiments were performed with a pin to plate and SDBD
arrangements. The results show that with the simultaneous application of two power supplies the drying rate
in a drop of water as a standard sample was greatly enhanced and the drying time was reduced. Thus, the
total evaporation was occurred in 1 minute in the SDBD structure with a power of 7 watts and in 1.5 minutes in
pin to plate structure with a power of 2.5 watts. Eventually, it was observed that the use of mixed electric fields
enhances the ionic wind, hence increases the non-thermal evaporation process significantly. Furthermore, the
drying rate has grown notably In SDBD configuration.</Abstract>
		<ObjectList>
            		</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>OICC PRESS</PublisherName>
			<JournalTitle>Synthesis structural and anti-microbial characterization of nanostructured doped tin oxide</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 16 (2022)</Volume>
			<Issue>Issue 1, March 2022</Issue>
			<PubDate PubStatus="epublish">
                <Year>2022</Year>
                <Month>12</Month>
                <Day>09</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Synthesis structural and anti-microbial characterization of nanostructured doped tin oxide</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.30495/jtap.162202</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>A.M.</FirstName>
				<LastName>Roychaudhury</LastName>
				<Affiliation>Department of Chemistry, Raiganj University, Raiganj, Uttar Dinajpur 733134, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Utsa</FirstName>
				<LastName>Debnath</LastName>
				<Affiliation>Department of Chemistry, Raiganj University, Raiganj, Uttar Dinajpur 733134, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Sujay</FirstName>
				<LastName>Munshi</LastName>
				<Affiliation>Department of Physics, Raiganj University, Raiganj, Uttar Dinajpur 733134, India.</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Goutam</FirstName>
				<LastName>Kumar Basak</LastName>
				<Affiliation>Department of Microbiology, Raiganj University, Raiganj, Uttar Dinajpur 733134, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Abhigyan</FirstName>
				<LastName>Dutta</LastName>
				<Affiliation>Department of Physics, University of Burdwan, Burdwan, 713 104, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>S.</FirstName>
				<LastName>Masanta</LastName>
				<Affiliation>Department of Physics, Bose Institute, 93/1, APC Road, Kolkata 700009, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Achintya</FirstName>
				<LastName>Singha</LastName>
				<Affiliation>Department of Physics, Bose Institute, 93/1, APC Road, Kolkata 700009, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Aritra</FirstName>
				<LastName>Banerjee</LastName>
				<Affiliation>Department of Physics, University of Calcutta, 92 A P C Road, Kolkata-700 009, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Debtanu</FirstName>
				<LastName>Ghosh</LastName>
				<Affiliation>Department of Physics, Vivekananda Mahavidyalaya, Haripal, Hooghly 712405, India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Partha</FirstName>
				<LastName>Chatterjee</LastName>
				<Affiliation>Department of Physics, Vivekananda Mahavidyalaya, Haripal, Hooghly 712405, India</Affiliation>
				<Identifier Source="ORCID">0000-0002-7049-3934</Identifier>
			</Author>
            			<Author>
                				<FirstName>Apurba</FirstName>
				<LastName>Kanti Deb</LastName>
				<Affiliation>Department of Physics, Raiganj University, Raiganj, Uttar Dinajpur 733134, India</Affiliation>
				<Identifier Source="ORCID">0000-0001-7033-3044</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2022</Year>
				<Month>12</Month>
				<Day>09</Day>
			</PubDate>
		</History>
		<Abstract>Nanocrystalline boron doped tin oxide and boron and silver co-doped SnO2 was successfully prepared by using
simple sol-gel method. The structural property of as-prepared nanocrystalline materials was investigated by
using X-ray powder diffraction, Raman spectroscopy, Fourier transform infrared spectroscopy and scanning
electron microscopy. The infrared spectra of the prepared samples showed an incorporation of B and Ag in the
SnO2 nanocrystals. The X-ray powder diffraction pattern of the as prepared sample demonstrated the formation
of a rutile structure of SnO2 nanocrystallites with particle size of 35 nm and 98 nm for boron doped and co-doped
samples respectively. The two different Sn-O bond distances are found to be varying in a different manner for the
doped samples unlike pristine samples. A significant lattice microstrain was observed for co-doped samples
indicating local lattice distortion. The prepared samples showed significant anti-microbial activities against some
Gram-Positive &amp; Gram-Negative</Abstract>
		<ObjectList>
            		</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>OICC PRESS</PublisherName>
			<JournalTitle>Investigation of the Poynting flux ratio in the helix traveling wave tube</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 16 (2022)</Volume>
			<Issue>Issue 1, March 2022</Issue>
			<PubDate PubStatus="epublish">
                <Year>2022</Year>
                <Month>12</Month>
                <Day>11</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Investigation of the Poynting flux ratio in the helix traveling wave tube</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.30495/jtap.162203</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Mona</FirstName>
				<LastName>Mehranfar</LastName>
				<Affiliation>Plasma Physics Research Centre, Science and Research Branch, Islamic Azad University, Tehran, Iran.</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName></FirstName>
				<LastName></LastName>
				<Affiliation></Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Davoud</FirstName>
				<LastName>Dorranian</LastName>
				<Affiliation>Plasma Physics Research Centre, Science and Research Branch, Islamic Azad University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0001-8855-7425</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2022</Year>
				<Month>12</Month>
				<Day>11</Day>
			</PubDate>
		</History>
		<Abstract>The study deals with amplification of a propagating slow wave interacting with an annular hollow electron beam
in a helix slow wave structure (SWS). The role of thermal plasma density in a ratio of the axial pointing flux in the
plasma region is also investigated. This ratio is small for lower plasma densities. The effects of the variations of
the hollow electron beam velocity on the normalized growth rate and the poynting flux ratio at the hybrid mode
frequency are presented. The maximum gain is obtained in the frequency of hybrid mode and the poynting flux
ratio reaches its maximum value at the hybrid mode frequency. Also is analyzed the trend of changes for the
normalized growth rate for a different beam velocities. The results show that for all beam velocities the maximum
growth rate is for hybrid mode frequencies. The numerical method used in this paper is complex transcendental.</Abstract>
		<ObjectList>
            		</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>OICC PRESS</PublisherName>
			<JournalTitle>The interface of FeCrP film with graphene-like BN: electronic, band alignment, and thermoelectric properties</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 16 (2022)</Volume>
			<Issue>Issue 1, March 2022</Issue>
			<PubDate PubStatus="epublish">
                <Year>2022</Year>
                <Month>12</Month>
                <Day>11</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>The interface of FeCrP film with graphene-like BN: electronic, band alignment, and thermoelectric properties</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.30495/jtap.162204</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Mansoure</FirstName>
				<LastName>Ilkhani</LastName>
				<Affiliation>Department of Physics, Shahr-e-Qods Branch, Islamic Azad University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0002-6830-3169</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2022</Year>
				<Month>12</Month>
				<Day>11</Day>
			</PubDate>
		</History>
		<Abstract>Based on the Density Functional Theory (DFT) and Generalized Gradient Approximation (GGA), the structural,
electronic, and band alignment properties of the interface of FeCrP film with graphene-like BN (g-BN) were
studied. These properties have been investigated at three different distances between FeCrP film and g-BN. In
all three mentioned distances, the ground state point and the bulk modulus show that these compounds have the
necessary strength to form, and at the distance of 2.7628 ˚A, the compound is more stable than the other two
distances. At this interface, the bulk modulus is greater than its values for the pure FeCrP and also the g-BN
compounds. In addition, at the FeCrP-BN interface, the emergence of a large magnetic moment of 13.995 μB is
found. Based on the mBJ approximation, this interface has a half-metallic characteristic and in the minority spin,
it has a direct bandgap of 0.41 eV spin flip. At this interface, the Schottky height was obtained to be about 1.89
eV. It is found that the BN electronic structure is n-type and the ECNLs appearing in this band alignment are close
to the Fermi level as donor-like.</Abstract>
		<ObjectList>
            		</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>OICC PRESS</PublisherName>
			<JournalTitle>Impact of silica seeding and discharge voltage on plasma parameters at atmospheric pressure</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 16 (2022)</Volume>
			<Issue>Issue 1, March 2022</Issue>
			<PubDate PubStatus="epublish">
                <Year>2022</Year>
                <Month>12</Month>
                <Day>11</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Impact of silica seeding and discharge voltage on plasma parameters at atmospheric pressure</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.30495/jtap.162205</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Vijay</FirstName>
				<LastName>Kumar Jha</LastName>
				<Affiliation>Central Department of Physics, Kirtipur (Tribhuvan University, Kathmandu), Nepal</Affiliation>
				<Identifier Source="ORCID">0000-0001-7310-1177</Identifier>
			</Author>
            			<Author>
                				<FirstName>Lekha</FirstName>
				<LastName>Nath Mishra</LastName>
				<Affiliation>Patan Multiple Campus, Patandhoka, Lalitpur (Tribhuvan University, Kathmandu), Nepal</Affiliation>
				<Identifier Source="ORCID">0000-0002-3892-4570</Identifier>
			</Author>
            			<Author>
                				<FirstName>Bijoyendra</FirstName>
				<LastName>Narayan</LastName>
				<Affiliation>J. L. College, Hajipur, Vaishali (B. R. A. Bihar University, Muzaffarpur), India</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2022</Year>
				<Month>12</Month>
				<Day>11</Day>
			</PubDate>
		</History>
		<Abstract>The interaction of cold plasma with heterogeneous catalysts has led to some peculiar behavior, especially with
silica (SiO2) seeding in presence of 2% alumina (Al2O3). In this paper, we have measured plasma parameters in
low temperature arc plasma. I - V characteristics of Langmuir probes are plotted using the data obtained from
the experimental set up for single probe method in arc plasma at atmospheric pressure. It is revealed that the
used seed modifies the electron temperature of the plasma appreciably while the temperature of the gas in the
surrounding remains almost unchanged. The single probe characteristics have been utilized to measure the
electron temperature, floating potential, Debye length and electron density. It is found that electron temperature
decreases whereas electron density increases appreciably after seeding the arc plasma. The decrease in
electron temperature and increase in electron density to 99.9% are observed after seeding the arc plasma
with silica mixture as compared to those before seeding. Variations in plasma parameters such as electron
temperature, electron density, plasma frequency and Debye length with discharge voltage are also plotted for the
silica seeded arc plasma.</Abstract>
		<ObjectList>
            		</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>OICC PRESS</PublisherName>
			<JournalTitle>The generalized representation of Dirac equation in two dimensions</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 16 (2022)</Volume>
			<Issue>Issue 1, March 2022</Issue>
			<PubDate PubStatus="epublish">
                <Year>2022</Year>
                <Month>12</Month>
                <Day>11</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>The generalized representation of Dirac equation in two dimensions</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.30495/jtap.162206</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Hamze</FirstName>
				<LastName>Moayeri</LastName>
				<Affiliation>Physics Department, Science Faculty, Jundi-Shapur University of Technology, Dezful, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0001-5199-4349</Identifier>
			</Author>
            			<Author>
                				<FirstName>Ali</FirstName>
				<LastName>Chenani</LastName>
				<Affiliation>Physics Department, Science Faculty, Jundi-Shapur University of Technology, Dezful, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Alireza</FirstName>
				<LastName>Hakimifard</LastName>
				<Affiliation>Physics Department, Science Faculty, Jundi-Shapur University of Technology, Dezful, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Nemat</FirstName>
				<LastName>Tahmasebi</LastName>
				<Affiliation>Physics Department, Science Faculty, Jundi-Shapur University of Technology, Dezful, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0002-7214-1684</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2022</Year>
				<Month>12</Month>
				<Day>11</Day>
			</PubDate>
		</History>
		<Abstract>Since the discovery of the Dirac equation, much research has been done on the construction of various sets
consisting of Dirac matrices that all of which follow the Cliford Algebra. But there is never notice to the relationship
between the internal elements of these matrices. In this work, the general form of 2×2 Dirac matrices for
2+1 dimension is found. In order to find this general representation, all relations among the elements of the
matrices are found, and the generalized Lorentz transform matrix is also found under the effect of the general
representation of Dirac matrices. As we know, the well known equation of Dirac, (iγμ∂μ −m) Ψ = 0, is consist of
matrices of even dimension known as the Dirac matrices. Our motivation for this study was lack of the general
representation of these matrices despite the fact that more than nine decades have been passed since the
discovery of this well known equation. Everyone has used a specific representation of this equation according to
their need; such as the standard representation known as Dirac-Pauli Representation, Weyl Representation or
Majorana representation. In this work, the general form which these matrices can have is found once for all.</Abstract>
		<ObjectList>
            		</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>OICC PRESS</PublisherName>
			<JournalTitle>The Cairns-Tsallis model for ion acoustic cnoidal (periodic) waves</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 16 (2022)</Volume>
			<Issue>Issue 1, March 2022</Issue>
			<PubDate PubStatus="epublish">
                <Year>2022</Year>
                <Month>12</Month>
                <Day>11</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>The Cairns-Tsallis model for ion acoustic cnoidal (periodic) waves</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.30495/jtap.162207</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Forough</FirstName>
				<LastName>Farhadkiyaei</LastName>
				<Affiliation>Physics Department, Islamic Azad Uni., Aligudarz Branch, Aligudarz, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0001-5401-406X</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2022</Year>
				<Month>12</Month>
				<Day>11</Day>
			</PubDate>
		</History>
		<Abstract>In this paper, considering the importance of ion acoustic waves in nonlinear phenomena of plasma, the combined
effects of nonextensivity and nonthermality parameters on the ion acoustic cnoidal nonlinear waves studied. In
this regard, the hybrid Cairns-Tsallis distribution function used to describe the electrons and positrons. Conditions
of formation of nonlinear ion acoustic waves and permissible values of nonextensivity (Q) and nonthermality
(α) parameters were determined and the behavior of these waves with changes in these parameters in this
type of plasma have been studied. For this purpose, we have used the reductive perturbation method (RPM)
to derive the corresponding KdV equation for the ion acoustic wave, then considering the Sagdeev potential,
the conditions for the generation of ion acoustic waves in the cnoidal and soliton form discussed. The effect of
nonextensivity (Q) and nonthermality (α) parameters on the Sagdeev potential (potential well width and depth),
wave amplitude and frequency investigated. The results show that for all of the acceptable values of Q and α the
cnoidal ion acoustic wave is compressive.</Abstract>
		<ObjectList>
            		</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>OICC PRESS</PublisherName>
			<JournalTitle>Investigation of the effects of pulse repetition frequency in a mixed electric field on a SDBD-like plasma jet</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 16 (2022)</Volume>
			<Issue>Issue 1, March 2022</Issue>
			<PubDate PubStatus="epublish">
                <Year>2022</Year>
                <Month>12</Month>
                <Day>11</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Investigation of the effects of pulse repetition frequency in a mixed electric field on a SDBD-like plasma jet</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.30495/jtap.162208</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Amir</FirstName>
				<LastName>Abbas Heidari</LastName>
				<Affiliation>Laser and Plasma Research Institute, Shahid Beheshti University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0001-9802-7487</Identifier>
			</Author>
            			<Author>
                				<FirstName>Pourya</FirstName>
				<LastName>Seyfi</LastName>
				<Affiliation>Laser and Plasma Research Institute, Shahid Beheshti University, Evin, Tehran 1983963113, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Ahmad</FirstName>
				<LastName>Khademi</LastName>
				<Affiliation>Laser and Plasma research institute, Shahid Beheshti University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0002-0411-6444</Identifier>
			</Author>
            			<Author>
                				<FirstName>Hamid</FirstName>
				<LastName>Ghomi</LastName>
				<Affiliation>Laser and Plasma Research Institute, Shahid Beheshti University, Evin, Tehran 1983963113, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0003-2203-5194</Identifier>
			</Author>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2022</Year>
				<Month>12</Month>
				<Day>11</Day>
			</PubDate>
		</History>
		<Abstract>In this paper, the design, performance and characterization of a low temperature argon plasma jet with a Surface
Dielectric Barrier Discharge (SDBD)-like structure are presented. Based on this structure, the argon plasma
jet is generated in a SDBD-like structure with a mixed electric field. SDBD-like structure, refers to the plasma
jet generated by the surface dielectric barrier discharge. The effects of high frequency electric pulse as the
main igniter for plasma jet generation and low frequency sinusoidal electric field in order to modify the dynamic
behavior of plasma jet are investigated in this paper. The effect of these variations on the plasma jet along with
the decrease in pulse repetition frequency were recorded by Schlieren imaging method. This study revealed the
important role of decreasing the pulse repetition frequency in the mixed electric field in the SDBD-like plasma jet
structure. Increasing the cross-sectional area of the plasma colliding with the target surface is the most important
advantage of this structure for the generation of plasma jets. Also, the trend of decreasing plasma column
continuity with increasing pulse repetition frequency is another result of this study. Under these conditions, the
diameter of the cross section of the plasma jet increases to 9 mm without increasing the consumption of more
electrical power and with equal jet length. Finally, the surface hydrophilicity was measured after treatment by
plasma jet and the operation resulted in a super-hydrophilic surface.</Abstract>
		<ObjectList>
            		</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>OICC PRESS</PublisherName>
			<JournalTitle>Damping effects in ^{100}Sn ^{+ 16}O and ^{100}Sn ^{+ 16Ca} collisions</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 16 (2022)</Volume>
			<Issue>Issue 1, March 2022</Issue>
			<PubDate PubStatus="epublish">
                <Year>2022</Year>
                <Month>12</Month>
                <Day>21</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Damping effects in ^{100}Sn ^{+ 16}O and ^{100}Sn ^{+ 16Ca} collisions</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.30495/JTAP.162209</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            		</AuthorList>
		<PublicationType>Journal Article</PublicationType>
		<History>
			<PubDate PubStatus="received">
				<Year>2022</Year>
				<Month>12</Month>
				<Day>21</Day>
			</PubDate>
		</History>
		<Abstract>Skyrme Forces (SF) Based Mean Field Model (MFM) or related density function is widely used to describe nuclear states, collective vibrational excitation, and heavy-ion collisions. To investigate 100Sn+16O and 100Sn+48Ca collisions on a 3-dimensional(3D) mesh with Skyrme SV-bas forces in Ecm=100, 150, and 200 MeV, Time-Dependent Hartree-Fock Skyrme(TDHFS) computations were done. The effective interaction in the computation of reaction dynamics as an important role in understanding the dynamics of the reaction provides us with knowledge about the characteristics of heavy-ion reactions&#039; effective interaction. The effect of increasing the ratio of neutrons to protons and the symmetry and asymmetry of the nuclei, as well as the size of the box at different energies, on the structure of the composite core, was investigated. The 100Sn+16O collision time course findings reveal that the continuous dampening effect remains after the fusion process. The damping mechanism has been demonstrated to be connected to breaking the dependency on box size, which is like the twisted average boundary condition that may avoid box size impacts on the 3D coordinate space employed, whereas periodic boundary conditions are seen for 100Sn +48Ca.</Abstract>
		<ObjectList>
            		</ObjectList>
	</Article>
		<Article>
		<Journal>
			<PublisherName>OICC PRESS</PublisherName>
			<JournalTitle>Synthesis of titanium-silver bimetallic nanoparticles by thermal plasma method</JournalTitle>
			<Issn></Issn>
			<Volume>Volume 16 (2022)</Volume>
			<Issue>Issue 1, March 2022</Issue>
			<PubDate PubStatus="epublish">
                <Year>2022</Year>
                <Month>12</Month>
                <Day>11</Day>
			</PubDate>
		</Journal>
		<ArticleTitle>Synthesis of titanium-silver bimetallic nanoparticles by thermal plasma method</ArticleTitle>
		<VernacularTitle></VernacularTitle>
		<FirstPage></FirstPage>
		<LastPage></LastPage>
		<ELocationID EIdType="doi">10.30495/jtap.162210</ELocationID>
		<Language>EN</Language>
		<AuthorList>
            			<Author>
                				<FirstName>Sahar</FirstName>
				<LastName>Shehni</LastName>
				<Affiliation>Plasma physics research center, Science and research branch, Islamic Azad University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID"></Identifier>
			</Author>
            			<Author>
                				<FirstName>Shahrooz</FirstName>
				<LastName>Saviz</LastName>
				<Affiliation>Plasma physics research center, Science and research branch, Islamic Azad University, Tehran, Iran</Affiliation>
				<Identifier Source="ORCID">0000-0001-5874-3761</Identifier>
			</Author>
            			<Author>
                				<FirstName>Amir</FirstName>
				<LastName>Hosein Sari</LastName>
				<Affiliation>Plasma physics research center, 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>2022</Year>
				<Month>12</Month>
				<Day>11</Day>
			</PubDate>
		</History>
		<Abstract>In the present paper, the micron-size silver and titanium powder with desired weight ratios is used to produce
the silver-titanium nanocomposite using the self-developed thermal plasma equipment. The mixture is fed into
the plasma torch flame by the powder feed system and argon carrier gas. After evaporation, the particles are
cooled inside the cooling chamber and collected from the surface of the water-cooled double-walled chamber.
The production of Titanium-Silver bimetallic nanoparticles is achieved in two ways: the cooling chamber is
once filled with argon and once with atmospheric air. The nanoparticles are analyzed using scanning electron
microscope (SEM), Energy Dispersive X-ray Spectroscopy (EDS), and X-ray Diffraction (XRD) methods to
identify the nanoparticle size distribution, morphology and chemical composition properties. The morphology of
the produced nanocomposites is spherical and their average size is 30 nm. The results indicate that the average
size of nanoparticles produced in the presence of air is smaller than those in the presence of argon.</Abstract>
		<ObjectList>
            		</ObjectList>
	</Article>
	</ArticleSet>
