<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE ArticleSet PUBLIC "-//NLM//DTD PubMed 2.7//EN" "https://dtd.nlm.nih.gov/ncbi/pubmed/in/PubMed.dtd">
<ArticleSet>
<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>24</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2024</Year>
					<Month>11</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Artificial Intelligence: conscious utilization</ArticleTitle>
<VernacularTitle>Artificial Intelligence: conscious utilization</VernacularTitle>
			<FirstPage></FirstPage>
			<LastPage></LastPage>
			<ELocationID EIdType="pii">3560</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Reza</FirstName>
					<LastName>Asgari</LastName>
<Affiliation>Editor-in-Chief</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2025</Year>
					<Month>01</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract></Abstract>
			<OtherAbstract Language="FA"></OtherAbstract>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_3560_0ae1dd3954ee840075de1395771b6c9c.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>24</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2024</Year>
					<Month>11</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Quantum properties of nondegenerate three-level laser coupled vacuum reservoir</ArticleTitle>
<VernacularTitle>Quantum properties of nondegenerate three-level laser coupled vacuum reservoir</VernacularTitle>
			<FirstPage>29</FirstPage>
			<LastPage>38</LastPage>
			<ELocationID EIdType="pii">3561</ELocationID>
			
<ELocationID EIdType="doi">10.47176/ijpr.24.3.21416</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Menisha</FirstName>
					<LastName>Alemu</LastName>
<Affiliation>Department of Physics, Wolkite University P. O. Box 07, Wolkite, Ethiopia</Affiliation>
<Identifier Source="ORCID">0000-0003-2419-0294</Identifier>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2022</Year>
					<Month>02</Month>
					<Day>14</Day>
				</PubDate>
			</History>
		<Abstract>In this paper, we have studied the squeezing and statistical properties of the light produced by a three-level laser whose cavity contains a parametric amplifier, and with the cavity mode driven by coherent light and coupled to a vacuum reservoir. We obtain stochastic differential equations associated with the normal ordering using the pertinent master equation. By making use of the solutions to the resulting differential equations, we calculate the quadrature variances. We also determine the mean and variance of the photon number for the cavity mode by employing the Q function. It is found that the parametric amplifier increases the degree of squeezing, while the driving coherent light does not have any effect on the squeezing. Moreover, the mean photon number increases considerably due to the driving coherent light and the parametric amplifier.</Abstract>
			<OtherAbstract Language="FA">In this paper, we have studied the squeezing and statistical properties of the light produced by a three-level laser whose cavity contains a parametric amplifier, and with the cavity mode driven by coherent light and coupled to a vacuum reservoir. We obtain stochastic differential equations associated with the normal ordering using the pertinent master equation. By making use of the solutions to the resulting differential equations, we calculate the quadrature variances. We also determine the mean and variance of the photon number for the cavity mode by employing the Q function. It is found that the parametric amplifier increases the degree of squeezing, while the driving coherent light does not have any effect on the squeezing. Moreover, the mean photon number increases considerably due to the driving coherent light and the parametric amplifier.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">stochastic differential equations</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">C-number Langevin equations</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">vacuum reservoir</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">mean photon number</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_3561_414a7497190eaef6b5d75d5a6a11afcf.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>24</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2024</Year>
					<Month>11</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Review of the measurements and results of the Coma cluster dark mass</ArticleTitle>
<VernacularTitle>Review of the measurements and results of the Coma cluster dark mass</VernacularTitle>
			<FirstPage>39</FirstPage>
			<LastPage>44</LastPage>
			<ELocationID EIdType="pii">3533</ELocationID>
			
<ELocationID EIdType="doi">10.47176/ijpr.24.3.91755</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Malalay</FirstName>
					<LastName>Ramazanoghly</LastName>
<Affiliation>Department of Physics, Faculty of Physics and Chemistry, Alzahra University, Tehran, Iran</Affiliation>
<Identifier Source="ORCID">0009-0006-4977-3874</Identifier>

</Author>
<Author>
					<FirstName>Ahmad</FirstName>
					<LastName>Shariati</LastName>
<Affiliation>Department of Physics, Faculty of Physics and Chemistry, Alzahra University, Tehran, Iran</Affiliation>
<Identifier Source="ORCID">0000-0002-8090-9905</Identifier>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2023</Year>
					<Month>09</Month>
					<Day>19</Day>
				</PubDate>
			</History>
		<Abstract>We have examined data from 852 Coma cluster galaxies from three different catalogs and grouped them according to their velocity and magnitude in two fields to survey the core (Coma1) and the periphery (i.e. southwest of the core and centered on NGC4839; Coma3). We have identified a group of these galaxies that appear to be a dense cluster (main cluster) of 545 galaxies (430 in Coma1 and 115 in Coma3) at a distance of 104 Mpc. Furthermore, we have calculated their kinetic energy (10&lt;sup&gt;54&lt;/sup&gt;±6J) and potential energy (10&lt;sup&gt;54&lt;/sup&gt;±0.7J) using observational data. Then we calculated the total mass (10&lt;sup&gt;45&lt;/sup&gt;±0.3kg) using luminosity and from the virial theorem, we obtained the virial mass (10&lt;sup&gt;47&lt;/sup&gt;±0.4  kg), that the virial mass was greater than the total mass of the galaxies in the cluster. These galaxies cover the range of 12.7 &lt; R &lt; 22.7, which corresponds to, −22.5 &lt; M&lt;sub&gt;R&lt;/sub&gt; &lt; −12.5 (H = 67.4 ± 0.5 km s&lt;sup&gt;-1&lt;/sup&gt; Mpc&lt;sup&gt;-1&lt;/sup&gt;) and the velocity of this set is in this range (1000 km s&lt;sup&gt;-1&lt;/sup&gt; &lt; v &lt; 10000 km s&lt;sup&gt;-1&lt;/sup&gt;). Our sample is 95% complete in redshift up to a magnitude b&lt;sub&gt;26.5&lt;/sub&gt; = 18.0 mag.</Abstract>
			<OtherAbstract Language="FA">We have examined data from 852 Coma cluster galaxies from three different catalogs and grouped them according to their velocity and magnitude in two fields to survey the core (Coma1) and the periphery (i.e. southwest of the core and centered on NGC4839; Coma3). We have identified a group of these galaxies that appear to be a dense cluster (main cluster) of 545 galaxies (430 in Coma1 and 115 in Coma3) at a distance of 104 Mpc. Furthermore, we have calculated their kinetic energy (10&lt;sup&gt;54&lt;/sup&gt;±6J) and potential energy (10&lt;sup&gt;54&lt;/sup&gt;±0.7J) using observational data. Then we calculated the total mass (10&lt;sup&gt;45&lt;/sup&gt;±0.3kg) using luminosity and from the virial theorem, we obtained the virial mass (10&lt;sup&gt;47&lt;/sup&gt;±0.4  kg), that the virial mass was greater than the total mass of the galaxies in the cluster. These galaxies cover the range of 12.7 &lt; R &lt; 22.7, which corresponds to, −22.5 &lt; M&lt;sub&gt;R&lt;/sub&gt; &lt; −12.5 (H = 67.4 ± 0.5 km s&lt;sup&gt;-1&lt;/sup&gt; Mpc&lt;sup&gt;-1&lt;/sup&gt;) and the velocity of this set is in this range (1000 km s&lt;sup&gt;-1&lt;/sup&gt; &lt; v &lt; 10000 km s&lt;sup&gt;-1&lt;/sup&gt;). Our sample is 95% complete in redshift up to a magnitude b&lt;sub&gt;26.5&lt;/sub&gt; = 18.0 mag.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Coma cluster</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Dark matter</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">galaxies</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Coma galaxy cluster</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_3533_5a9d8bf5b7a4b35f3110dde8673bdda2.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>24</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2024</Year>
					<Month>11</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Influence of dysprosium cation on structural and magnetic properties‌ of thin films nickel-cobalt ferrite: using spray pyrolysis method</ArticleTitle>
<VernacularTitle>Influence of dysprosium cation on structural and magnetic properties‌ of thin films nickel-cobalt ferrite: using spray pyrolysis method</VernacularTitle>
			<FirstPage>45</FirstPage>
			<LastPage>51</LastPage>
			<ELocationID EIdType="pii">3534</ELocationID>
			
<ELocationID EIdType="doi">10.47176/ijpr.24.3.11791</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Jalil</FirstName>
					<LastName>Khobzade</LastName>
<Affiliation>Physics Departement, College of Sciences, Yasouj University, Yasouj, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Abolghasem</FirstName>
					<LastName>Avazpour</LastName>
<Affiliation>Physics Departement, College of Sciences, Yasouj University, Yasouj, Iran</Affiliation>
<Identifier Source="ORCID">0000-0001-7650-7105</Identifier>

</Author>
<Author>
					<FirstName>Ali</FirstName>
					<LastName>Modaberasl</LastName>
<Affiliation>Physics Departement, College of Sciences, Yasouj University, Yasouj, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Alireza</FirstName>
					<LastName>Nikzad</LastName>
<Affiliation>Physics Departement, College of Sciences, Yasouj University, Yasouj, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2023</Year>
					<Month>11</Month>
					<Day>20</Day>
				</PubDate>
			</History>
		<Abstract>In this study, nickel-cobalt ferrite nanoparticles were prepared using spray pyrolysis. X-Ray Diffraction (XRD), Fourier Transform Infrared Spectroscopy (FTIR), and Vibration Sample Magnetometer (VSM) were used to examine the structural and magnetic properties of the obtained samples. In addition, the size, dispersion, and morphology of the particles on the surface of the glass substrate were observed and analyzed by atomic force microscope (AFM). The amount of dysprosium cation contamination was x=0.0, 0.025, 0.05, 0.075, and 1.0. All the peaks identified in the diffraction patterns of the samples were in good agreement with the reference card, and the Miller indices were indexed. FTIR spectra were obtained in the wavenumber range of 400-2000 cm&lt;sup&gt;-1&lt;/sup&gt;. The hysteresis loops are symmetric, and an increasing or decreasing trend of the parameters can be observed. This shows the high purity of the prepared samples without any distorted phases. In this study, the amount of magnetization (Ms) decreased, whereas an increasing trend was observed for the coercivity (Hc). The prepared magnetic nanoparticles have many applications in ferrofluids, color imaging, magnetic cooling, drug delivery, detoxification of biological fluids, and magnetic cell separation. In addition, they can be used in miniaturized inductive electric sensors, inductors, high-frequency equipment, and biotechnological applications.</Abstract>
			<OtherAbstract Language="FA">In this study, nickel-cobalt ferrite nanoparticles were prepared using spray pyrolysis. X-Ray Diffraction (XRD), Fourier Transform Infrared Spectroscopy (FTIR), and Vibration Sample Magnetometer (VSM) were used to examine the structural and magnetic properties of the obtained samples. In addition, the size, dispersion, and morphology of the particles on the surface of the glass substrate were observed and analyzed by atomic force microscope (AFM). The amount of dysprosium cation contamination was x=0.0, 0.025, 0.05, 0.075, and 1.0. All the peaks identified in the diffraction patterns of the samples were in good agreement with the reference card, and the Miller indices were indexed. FTIR spectra were obtained in the wavenumber range of 400-2000 cm&lt;sup&gt;-1&lt;/sup&gt;. The hysteresis loops are symmetric, and an increasing or decreasing trend of the parameters can be observed. This shows the high purity of the prepared samples without any distorted phases. In this study, the amount of magnetization (Ms) decreased, whereas an increasing trend was observed for the coercivity (Hc). The prepared magnetic nanoparticles have many applications in ferrofluids, color imaging, magnetic cooling, drug delivery, detoxification of biological fluids, and magnetic cell separation. In addition, they can be used in miniaturized inductive electric sensors, inductors, high-frequency equipment, and biotechnological applications.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">nanoparticles</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">magnetic properties</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">nickel-cobalt ferrite</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Spray pyrolysis</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_3534_aa97d584861474f4097cf13ccb5325da.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>24</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2024</Year>
					<Month>11</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Simulating the interactions between the produced neutrons from piezoelectric rocks and the surrounding medium during earthquakes</ArticleTitle>
<VernacularTitle>Simulating the interactions between the produced neutrons from piezoelectric rocks and the surrounding medium during earthquakes</VernacularTitle>
			<FirstPage>53</FirstPage>
			<LastPage>60</LastPage>
			<ELocationID EIdType="pii">3535</ELocationID>
			
<ELocationID EIdType="doi">10.47176/ijpr.24.3.11823</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Abouzar</FirstName>
					<LastName>Bahari</LastName>
<Affiliation>Department of Physics, Payame Noor University, Tehran, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Saeed</FirstName>
					<LastName>Mohammadi</LastName>
<Affiliation>Department of Physics, Payame Noor University, Tehran, Iran</Affiliation>
<Identifier Source="ORCID">0000-0001-7706-9856</Identifier>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2024</Year>
					<Month>01</Month>
					<Day>15</Day>
				</PubDate>
			</History>
		<Abstract>Many studies have shown that during earthquakes (EQs), the fracturing of piezoelectric rocks like granite causes atomic/ nuclear particles&#039; radiation into the Earth’s crust. With the help of an MCNPX simulation code, we have already studied the amount and energies of created atomic/ nuclear particles and the possible interactions for under-stressed piezoelectric blocks. In this research, applying the PACE4 code, we simulated the interactions between the created neutrons from under-stressed piezoelectric rocks and the elements of granite plus the elements of fractures’ filling fluids like water, air, methane, and CO&lt;sub&gt;2&lt;/sub&gt;, to study the mechanism of such reactions and find which new elements might be produced. The results indicate that compound nuclear reactions like fusion/ fission/ inelastic scattering can happen, resulting in the release of energy from the depths of the Earth in the aseismic regions. Furthermore, compound nuclear interactions from the piezoelectric effect can generate carbon (C), oxygen (O), hydrogen (H), and Nitrogen (N) in the granitic rocks’ medium or inside the fracture-filling fluids and trigger the life chain and/or the hydrocarbon chain (oil and gas), inside the Earth’s crust of the aseismic regions. It can also result in the production of CO&lt;sub&gt;2&lt;/sub&gt; gas. Moreover, in this process, some new elements like Al, Mg, etc., might also be produced in the texture of granitic rocks. In addition, we have found that the increasing amount of nuclear particles and radioactive elements on the surface could be a sign of an incoming earthquake.  Besides, neutron capturing might happen between neutrons and the hydrogen nuclei of the underground water, causing the production of deuterium. As a result, an increase in the amount of stable deuterium in the water around the aseismic regions can be a precursor of earthquakes.</Abstract>
			<OtherAbstract Language="FA">Many studies have shown that during earthquakes (EQs), the fracturing of piezoelectric rocks like granite causes atomic/ nuclear particles&#039; radiation into the Earth’s crust. With the help of an MCNPX simulation code, we have already studied the amount and energies of created atomic/ nuclear particles and the possible interactions for under-stressed piezoelectric blocks. In this research, applying the PACE4 code, we simulated the interactions between the created neutrons from under-stressed piezoelectric rocks and the elements of granite plus the elements of fractures’ filling fluids like water, air, methane, and CO&lt;sub&gt;2&lt;/sub&gt;, to study the mechanism of such reactions and find which new elements might be produced. The results indicate that compound nuclear reactions like fusion/ fission/ inelastic scattering can happen, resulting in the release of energy from the depths of the Earth in the aseismic regions. Furthermore, compound nuclear interactions from the piezoelectric effect can generate carbon (C), oxygen (O), hydrogen (H), and Nitrogen (N) in the granitic rocks’ medium or inside the fracture-filling fluids and trigger the life chain and/or the hydrocarbon chain (oil and gas), inside the Earth’s crust of the aseismic regions. It can also result in the production of CO&lt;sub&gt;2&lt;/sub&gt; gas. Moreover, in this process, some new elements like Al, Mg, etc., might also be produced in the texture of granitic rocks. In addition, we have found that the increasing amount of nuclear particles and radioactive elements on the surface could be a sign of an incoming earthquake.  Besides, neutron capturing might happen between neutrons and the hydrogen nuclei of the underground water, causing the production of deuterium. As a result, an increase in the amount of stable deuterium in the water around the aseismic regions can be a precursor of earthquakes.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">PACE4</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Particles’ radiation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">neutron</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Granite Rocks</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">piezoelectricity</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Earthquake</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_3535_b99d193b66a6542917d2b7bee52c2574.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>24</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2024</Year>
					<Month>11</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Measurement of nonlinear optical coefficients of zinc cobalt ferrite using the z-scan technique with variable intensity</ArticleTitle>
<VernacularTitle>Measurement of nonlinear optical coefficients of zinc cobalt ferrite using the z-scan technique with variable intensity</VernacularTitle>
			<FirstPage>61</FirstPage>
			<LastPage>67</LastPage>
			<ELocationID EIdType="pii">3537</ELocationID>
			
<ELocationID EIdType="doi">10.47176/ijpr.24.3.21853</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Forouzan</FirstName>
					<LastName>Habibi</LastName>
<Affiliation>Department of Physics, University of Shahrekord, Shahrekord, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Mohammad</FirstName>
					<LastName>Moradi</LastName>
<Affiliation>-Department of Physics, University of Shahrekord, Shahrekord, Iran
- Photonic Research Group, University of Shahrekord, Shahrekord, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Negar</FirstName>
					<LastName>Davoodian</LastName>
<Affiliation>Department of Physics, University of Shahrekord, Shahrekord, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2024</Year>
					<Month>02</Month>
					<Day>27</Day>
				</PubDate>
			</History>
		<Abstract>In this study, cobalt zinc ferrite nanoparticles were synthesized with the formula Co&lt;sub&gt;x-1&lt;/sub&gt;Zn&lt;sub&gt;x&lt;/sub&gt;Fe&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;4&lt;/sub&gt; using a Co-precipitation method, varying x values. A green laser was utilized as the excitation source to measure the nonlinear refractive index and absorption coefficient at three different intensities. The z-scan method was employed for both closed and open apertures at room temperature. The findings indicate that as the initial laser intensity increases, the nonlinear refractive index and nonlinear absorption coefficient decrease. Additionally, an increase in concentration at a specific intensity results in a limited appearance of nonlinear properties. Furthermore, an increase in the linear absorption coefficient corresponds to an increase in these nonlinear coefficients. This nanostructure proves valuable for night sensing applications due to its negative refractive index under strong nonlinearity. In this context, the spinel model of the nanostructure holds promising potential for 6G communication applications.</Abstract>
			<OtherAbstract Language="FA">In this study, cobalt zinc ferrite nanoparticles were synthesized with the formula Co&lt;sub&gt;x-1&lt;/sub&gt;Zn&lt;sub&gt;x&lt;/sub&gt;Fe&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;4&lt;/sub&gt; using a Co-precipitation method, varying x values. A green laser was utilized as the excitation source to measure the nonlinear refractive index and absorption coefficient at three different intensities. The z-scan method was employed for both closed and open apertures at room temperature. The findings indicate that as the initial laser intensity increases, the nonlinear refractive index and nonlinear absorption coefficient decrease. Additionally, an increase in concentration at a specific intensity results in a limited appearance of nonlinear properties. Furthermore, an increase in the linear absorption coefficient corresponds to an increase in these nonlinear coefficients. This nanostructure proves valuable for night sensing applications due to its negative refractive index under strong nonlinearity. In this context, the spinel model of the nanostructure holds promising potential for 6G communication applications.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">nanoparticles</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Zinc cobalt ferrite</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">z-scan method</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">nonlinear refractive index</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">nonlinear absorption index</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_3537_416849da96fb73bee793e2bf65ae43ac.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>24</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2024</Year>
					<Month>11</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Simulation the effects of temperature and magnetic field on the density of surface states in semiconductor heterostructures</ArticleTitle>
<VernacularTitle>Simulation the effects of temperature and magnetic field on the density of surface states in semiconductor heterostructures</VernacularTitle>
			<FirstPage>69</FirstPage>
			<LastPage>74</LastPage>
			<ELocationID EIdType="pii">3536</ELocationID>
			
<ELocationID EIdType="doi">10.47176/ijpr.24.3.21845</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Ulugbek</FirstName>
					<LastName>Erkaboev</LastName>
<Affiliation>Namangan Institute of Engineering and Technology, 160115, Namangan, Uzbekistan</Affiliation>
<Identifier Source="ORCID">0000-0002-6841-8214</Identifier>

</Author>
<Author>
					<FirstName>Nosir</FirstName>
					<LastName>Sharibaev</LastName>
<Affiliation>Namangan Institute of Engineering and Technology, 160115, Namangan, Uzbekistan</Affiliation>
<Identifier Source="ORCID">0000-0002-6417-9973</Identifier>

</Author>
<Author>
					<FirstName>Muzaffar</FirstName>
					<LastName>Dadamirzaev</LastName>
<Affiliation>1. Namangan Institute of Engineering and Technology, 160115, Namangan, Uzbekistan
2..Namangan Engineering-Construction Institute, 160103, Namangan, Uzbekistan</Affiliation>
<Identifier Source="ORCID">0009-0003-4190-4612</Identifier>

</Author>
<Author>
					<FirstName>Rustamjon</FirstName>
					<LastName>Rakhimov</LastName>
<Affiliation>Namangan Institute of Engineering and Technology, 160115, Namangan, Uzbekistan</Affiliation>
<Identifier Source="ORCID">0000-0003-0850-1398</Identifier>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2024</Year>
					<Month>02</Month>
					<Day>09</Day>
				</PubDate>
			</History>
		<Abstract>In this article, the physical properties of the surface of the CdS/Si(p) material under the influence of a magnetic field were studied . The dependence of the density of surface states of the p-type Si(p) semiconductor on the magnetic field and temperature has been studied. For the first time, a mathematical model has been developed to determine the temperature dependence of the density of surface states of a semiconductor under the influence of a strong magnetic field. Mathematical modeling of the processes was carried out using experimental values of the continuous energy spectrum of the density of surface states, obtained at various low temperatures and strong magnetic fields, whithin the band gap of silicon. The possibility of calculating discrete energy levels is demonstrated.</Abstract>
			<OtherAbstract Language="FA">In this article, the physical properties of the surface of the CdS/Si(p) material under the influence of a magnetic field were studied . The dependence of the density of surface states of the p-type Si(p) semiconductor on the magnetic field and temperature has been studied. For the first time, a mathematical model has been developed to determine the temperature dependence of the density of surface states of a semiconductor under the influence of a strong magnetic field. Mathematical modeling of the processes was carried out using experimental values of the continuous energy spectrum of the density of surface states, obtained at various low temperatures and strong magnetic fields, whithin the band gap of silicon. The possibility of calculating discrete energy levels is demonstrated.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Density of surface states</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">magnetic field</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">heterostructure</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">deep levels</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">capacitance-voltage characteristic</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Mathematical modeling</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Temperature</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_3536_291d43c696d8c3704cdbe0a72ade5f6c.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>24</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2024</Year>
					<Month>11</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Investigation of refractive index and group velocity of metal coated dielectric  spherical nanocomposites within both passive and active dielectric cores</ArticleTitle>
<VernacularTitle>Investigation of refractive index and group velocity of metal coated dielectric  spherical nanocomposites within both passive and active dielectric cores</VernacularTitle>
			<FirstPage>75</FirstPage>
			<LastPage>87</LastPage>
			<ELocationID EIdType="pii">3541</ELocationID>
			
<ELocationID EIdType="doi">10.47176/ijpr.24.3.51890</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Shewa</FirstName>
					<LastName>Getachew</LastName>
<Affiliation>Department of Physics, Wolkite University,  P. O. Box 07, Wolkite, Ethiopia</Affiliation>
<Identifier Source="ORCID">0009-0005-8265-0115</Identifier>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2024</Year>
					<Month>05</Month>
					<Day>02</Day>
				</PubDate>
			</History>
		<Abstract>This research paper focuses on studying how light behaves in metal-coated dielectric spherical nanocomposites. It investigates different types of light propagation, such as slow, backward, and fast lights. The paper examines the theoretical aspects of these phenomena in composite materials, specifically when spherical nanoinclusions are embedded in either active or passive dielectric cores, or when dielectric-coated metal spherical nanoinclusions are embedded in active or passive dielectric shells. Furthermore, the paper explores the optical properties of the composites at resonant frequencies and explores potential applications of systems that exhibit anomalous dispersion. The numerical observations in the paper discuss the occurrence of slow, backward, and superluminal light pulses in metal-coated dielectric and dielectric-coated metal nanocomposites with spherical nanoinclusions. Additionally, the paper suggests that incorporating gain layers with a negative dielectric function can improve the optical properties of the composite material.</Abstract>
			<OtherAbstract Language="FA">This research paper focuses on studying how light behaves in metal-coated dielectric spherical nanocomposites. It investigates different types of light propagation, such as slow, backward, and fast lights. The paper examines the theoretical aspects of these phenomena in composite materials, specifically when spherical nanoinclusions are embedded in either active or passive dielectric cores, or when dielectric-coated metal spherical nanoinclusions are embedded in active or passive dielectric shells. Furthermore, the paper explores the optical properties of the composites at resonant frequencies and explores potential applications of systems that exhibit anomalous dispersion. The numerical observations in the paper discuss the occurrence of slow, backward, and superluminal light pulses in metal-coated dielectric and dielectric-coated metal nanocomposites with spherical nanoinclusions. Additionally, the paper suggests that incorporating gain layers with a negative dielectric function can improve the optical properties of the composite material.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Anomalous dispersion</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">dielectric core</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">active dielectric core</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Nanocomposites</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">backward light</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_3541_c5f5c23be1b71adb51ea9dc8e9d444a8.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>24</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2024</Year>
					<Month>11</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Insight into the electronic and elastic properties of Li-rich- antiperovskite Li3OCl under hydrostatic pressures</ArticleTitle>
<VernacularTitle>Insight into the electronic and elastic properties of Li-rich- antiperovskite Li3OCl under hydrostatic pressures</VernacularTitle>
			<FirstPage>89</FirstPage>
			<LastPage>93</LastPage>
			<ELocationID EIdType="pii">3540</ELocationID>
			
<ELocationID EIdType="doi">10.47176/ijpr.24.3.41885</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Fethi</FirstName>
					<LastName>Redjem</LastName>
<Affiliation>Laboratoire d’étude et développement des Matériaux Semi-conducteur et Diélectriques (LEDMaScD), 
Université Amar Telidji , Bp37G 03000 Laghouat ,Algerie</Affiliation>

</Author>
<Author>
					<FirstName>Kouider</FirstName>
					<LastName>Souleh</LastName>
<Affiliation>Laboratoire d’étude et développement des Matériaux Semi-conducteur et Diélectriques (LEDMaScD), 
Université Amar Telidji , Bp37G 03000 Laghouat ,Algerie</Affiliation>

</Author>
<Author>
					<FirstName>Brahim</FirstName>
					<LastName>Lagoun</LastName>
<Affiliation>Laboratoire  physique des materiaux (LPM), Université Amar Telidji , Bp37G 03000 Laghouat ,Algerie.</Affiliation>

</Author>
<Author>
					<FirstName>H</FirstName>
					<LastName>Mebarki</LastName>
<Affiliation>Laboratoire de  matériaux  pour  Application et Valorisation des Enérgies Renouvelables (LMAVER), 
Université Amar Telidji , Bp37G 03000  Laghouat ,Algerie.</Affiliation>

</Author>
<Author>
					<FirstName>H</FirstName>
					<LastName>Lidjici</LastName>
<Affiliation>Laboratoire de  matériaux  pour  Application et Valorisation des Enérgies Renouvelables (LMAVER), 
Université Amar Telidji , Bp37G 03000  Laghouat ,Algerie.</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2024</Year>
					<Month>04</Month>
					<Day>20</Day>
				</PubDate>
			</History>
		<Abstract>Ab initio calculations were employed to examine the structural, elastic, and electrical properties of Li&lt;sub&gt;3&lt;/sub&gt;OCl, a cubic antiperovskite compound, under varying pressures. The calculations were performed using first principles density functional theory based on the full potential linearized augmented plane wave (FP-LAPW) method as implemented in a Wien2k package. The Perdew-Burke-Ernzerhof Generalized Gradient Approximation (PBE-GGA) was used as an exchange and correlation potential to investigate equilibrium structural parameters, energy band structure, density of states, and elastic characteristics for the Li&lt;sub&gt;3&lt;/sub&gt;OCl compound. We computed the Young modulus, Poisson ratio, and elastic anisotropy factor for this compound using elastic parameters. It is concluded that the material is mechanically stable according to the Born stability criteria and behaves in a brittle manner, referring to Pugh&#039;s index. Our results show that the predicted structural parameter values at 0 GPa are consistent with previous studies. Additionally, it has been found that the material exhibits a transition phase under a pressure of 1 GPa.</Abstract>
			<OtherAbstract Language="FA">Ab initio calculations were employed to examine the structural, elastic, and electrical properties of Li&lt;sub&gt;3&lt;/sub&gt;OCl, a cubic antiperovskite compound, under varying pressures. The calculations were performed using first principles density functional theory based on the full potential linearized augmented plane wave (FP-LAPW) method as implemented in a Wien2k package. The Perdew-Burke-Ernzerhof Generalized Gradient Approximation (PBE-GGA) was used as an exchange and correlation potential to investigate equilibrium structural parameters, energy band structure, density of states, and elastic characteristics for the Li&lt;sub&gt;3&lt;/sub&gt;OCl compound. We computed the Young modulus, Poisson ratio, and elastic anisotropy factor for this compound using elastic parameters. It is concluded that the material is mechanically stable according to the Born stability criteria and behaves in a brittle manner, referring to Pugh&#039;s index. Our results show that the predicted structural parameter values at 0 GPa are consistent with previous studies. Additionally, it has been found that the material exhibits a transition phase under a pressure of 1 GPa.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Antiperovskite</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">elastic properties</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">electronic structure</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Ab initio calculations</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Lithium battery</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_3540_8844c5f00372df2c3c4ee857c2451b45.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>24</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2024</Year>
					<Month>11</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>A matrix form solution of the multi-dimensional generalized Langevin equation in the quadratic potential</ArticleTitle>
<VernacularTitle>A matrix form solution of the multi-dimensional generalized Langevin equation in the quadratic potential</VernacularTitle>
			<FirstPage>95</FirstPage>
			<LastPage>97</LastPage>
			<ELocationID EIdType="pii">3544</ELocationID>
			
<ELocationID EIdType="doi">10.47176/ijpr.24.3.41887</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Rana Imran</FirstName>
					<LastName>Mushtaq</LastName>
<Affiliation>Institute of Theoretical Physics, School of Physics and Optoelectric Engineering, Ludong University, Yantai 264025,China</Affiliation>
<Identifier Source="ORCID">0009-0002-5050-5499</Identifier>

</Author>
<Author>
					<FirstName>Chunyang</FirstName>
					<LastName>Wang</LastName>
<Affiliation>-Institute of Theoretical Physics, School of Physics and Optoelectric Engineering, Ludong University, Yantai 264025,China
-Yantai Institute of Coastal Zone Research, Chinese Academy of Science, Yantai 264003, China</Affiliation>

</Author>
<Author>
					<FirstName>Shichao</FirstName>
					<LastName>Zhi</LastName>
<Affiliation>Institute of Theoretical Physics, School of Physics and Optoelectric Engineering, Ludong University, Yantai 264025,China</Affiliation>

</Author>
<Author>
					<FirstName>Zengxuan</FirstName>
					<LastName>Zhao</LastName>
<Affiliation>Institute of Theoretical Physics, School of Physics and Optoelectric Engineering, Ludong University, Yantai 264025,China</Affiliation>

</Author>
<Author>
					<FirstName>Jeolous Nyasulu</FirstName>
					<LastName>Malamula</LastName>
<Affiliation>Institute of Theoretical Physics, School of Physics and Optoelectric Engineering, Ludong University, Yantai 264025,China</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2024</Year>
					<Month>04</Month>
					<Day>22</Day>
				</PubDate>
			</History>
		<Abstract>In this research paper, we present an exact matrix form analytical solution of the multi-dimensional generalized Langevin equation with quadratic potentials. Our investigation provides detailed expressions for the two-dimensional probability distribution and extends the understanding of the dynamics governed by harmonic potentials. By utilizing the inverse Laplace transformation, we offer a precise method to solve these equations, corroborated by specific examples. This study contributes to the fundamental understanding of stochastic processes in multi-dimensional systems with harmonic potentials and clarifies the limitations of our approach. While the findings are specific to quadratic potentials, they provide a robust framework for exploring related phenomena within this context.</Abstract>
			<OtherAbstract Language="FA">In this research paper, we present an exact matrix form analytical solution of the multi-dimensional generalized Langevin equation with quadratic potentials. Our investigation provides detailed expressions for the two-dimensional probability distribution and extends the understanding of the dynamics governed by harmonic potentials. By utilizing the inverse Laplace transformation, we offer a precise method to solve these equations, corroborated by specific examples. This study contributes to the fundamental understanding of stochastic processes in multi-dimensional systems with harmonic potentials and clarifies the limitations of our approach. While the findings are specific to quadratic potentials, they provide a robust framework for exploring related phenomena within this context.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Generalized Langevin equation (GLE)</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">multi-dimensional dynamics</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Analytical Solution</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Laplace transformation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">stochastic processes</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_3544_147ebe637038ca50a1265abac8dea181.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>24</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2024</Year>
					<Month>11</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Proton-boron-11 fusion under effect of the temperature turbulence</ArticleTitle>
<VernacularTitle>Proton-boron-11 fusion under effect of the temperature turbulence</VernacularTitle>
			<FirstPage>99</FirstPage>
			<LastPage>109</LastPage>
			<ELocationID EIdType="pii">3542</ELocationID>
			
<ELocationID EIdType="doi">10.47176/ijpr.24.3.71937</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Fatemeh</FirstName>
					<LastName>Khodadadi Azadboni</LastName>
<Affiliation>Department of Physics Education, Farhangian University, P.O. Box 14665-889, Tehran, Iran</Affiliation>
<Identifier Source="ORCID">0000-0003-0896-7358</Identifier>

</Author>
<Author>
					<FirstName>Mohammad</FirstName>
					<LastName>Mahdavi</LastName>
<Affiliation>Physics Department, University of Mazandaran, P. O. Box 47415-416, Babolsar, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Elham</FirstName>
					<LastName>Khademlo</LastName>
<Affiliation>Physics Department, University of Mazandaran, P. O. Box 47415-416, Babolsar, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2024</Year>
					<Month>07</Month>
					<Day>12</Day>
				</PubDate>
			</History>
		<Abstract>The temperature turbulence generated by the ponderomotive force of the high-power laser can significantly modify P-11B fusion reactivity. The results of this study have shown that higher temperature turbulence leads to an increased requirement for the confinement parameter in P-11B fuel. As a result, achieving ignition necessitates greater driver energy and a longer development time. Additionally, a 50% reduction in the temperature turbulence parameter yields a substantial 71% decrease in the confinement parameter, accompanied by a 21% increase in the maximum fusion energy fraction. When the temperature turbulence exceeds a value of 10, the bremsstrahlung surpasses the fusion power, making ignition unattainable. The findings underscore the importance of maintaining temperature turbulence below 1 to approach the ignition conditions required for P-11B fuel.</Abstract>
			<OtherAbstract Language="FA">The temperature turbulence generated by the ponderomotive force of the high-power laser can significantly modify P-11B fusion reactivity. The results of this study have shown that higher temperature turbulence leads to an increased requirement for the confinement parameter in P-11B fuel. As a result, achieving ignition necessitates greater driver energy and a longer development time. Additionally, a 50% reduction in the temperature turbulence parameter yields a substantial 71% decrease in the confinement parameter, accompanied by a 21% increase in the maximum fusion energy fraction. When the temperature turbulence exceeds a value of 10, the bremsstrahlung surpasses the fusion power, making ignition unattainable. The findings underscore the importance of maintaining temperature turbulence below 1 to approach the ignition conditions required for P-11B fuel.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Confinement parameter</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Ignition condition</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">P-11B fuel</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Temperature turbulence</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_3542_8487e01fbaf43e758c17f86472cbf3e6.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>24</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2024</Year>
					<Month>11</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Modeling electric image in weakly electric fish using electrical impedance tomography</ArticleTitle>
<VernacularTitle>Modeling electric image in weakly electric fish using electrical impedance tomography</VernacularTitle>
			<FirstPage>111</FirstPage>
			<LastPage>116</LastPage>
			<ELocationID EIdType="pii">3543</ELocationID>
			
<ELocationID EIdType="doi">10.47176/ijpr.24.3.81944</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Alaleh</FirstName>
					<LastName>Ghasemi Kaliji</LastName>
<Affiliation>Department of Physics, Babol Noshirvani University of Technology, Babol, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Hossein</FirstName>
					<LastName>Mehri-Dehnavi</LastName>
<Affiliation>Department of Physics, Babol Noshirvani University of Technology, Babol, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Reza</FirstName>
					<LastName>Khanbabaie,</LastName>
<Affiliation>Department of Computer Science, Mathematics, Physics and Statistics, University of British Columbia, Canada</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2024</Year>
					<Month>08</Month>
					<Day>01</Day>
				</PubDate>
			</History>
		<Abstract>In this study, the electrical image of electric fish is modeled via electrical impedance tomography (EIT) using EIDORS, which is a toolkit in MATLAB. The modeling consists of three steps: (1) an 80 cm tank containing water similar to seawater, (2) a fish modeled with 10 electrodes arranged like a fish body, and (3) 1 mA current flow through an electrode and generating an electric dipole field for modeling the field around the fish. To explore the electric image, five important variables in object detection including object distance, position, conductivity, size, and object symmetry and orientation are examined. In general, the analysis of the model indicates that changing each of the variables has an effect on the electrical image. This modeling is able to distinguish between different objects and produce a specific electrical image for each specific object.</Abstract>
			<OtherAbstract Language="FA">In this study, the electrical image of electric fish is modeled via electrical impedance tomography (EIT) using EIDORS, which is a toolkit in MATLAB. The modeling consists of three steps: (1) an 80 cm tank containing water similar to seawater, (2) a fish modeled with 10 electrodes arranged like a fish body, and (3) 1 mA current flow through an electrode and generating an electric dipole field for modeling the field around the fish. To explore the electric image, five important variables in object detection including object distance, position, conductivity, size, and object symmetry and orientation are examined. In general, the analysis of the model indicates that changing each of the variables has an effect on the electrical image. This modeling is able to distinguish between different objects and produce a specific electrical image for each specific object.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Electric image</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Electrical Impedance Tomography</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">EIT</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Electric fish</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_3543_196f5641aa9dc87067da4ff90fd81e7b.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>24</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2024</Year>
					<Month>11</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Space weather disturbances and their geoeffectiveness during solar cycle 23 and 24</ArticleTitle>
<VernacularTitle>Space weather disturbances and their geoeffectiveness during solar cycle 23 and 24</VernacularTitle>
			<FirstPage>117</FirstPage>
			<LastPage>133</LastPage>
			<ELocationID EIdType="pii">3562</ELocationID>
			
<ELocationID EIdType="doi">10.47176/ijpr.24.3.31863</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Sham</FirstName>
					<LastName>Singh</LastName>
<Affiliation>Chandigarh Engineering College-CGC, Landran, Mohali-140307 India</Affiliation>
<Identifier Source="ORCID">0000-0003-4045-7841</Identifier>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2024</Year>
					<Month>03</Month>
					<Day>06</Day>
				</PubDate>
			</History>
		<Abstract>We present the findings of a study of the sequence of solar activity that eventually resulted in 80 large geomagnetic storms (distinguished by minimum Dst -100nT to -200nT), 11 super geomagnetic storms (Dst -200nT to -300nT), and 6 super great geomagnetic storms (Dst -300nT) that occurred between 1996 and 2012. Large storms were discovered to be mostly caused by solar flares (M- and X-class), while corotating interaction region (CIR) was also a significant contributor to several of these storms. During the peak and declining phases of solar cycle 23, all extremely powerful storms were observed (2000-2004). It has been noted that coronal mass ejections (CMEs) and flares were always related with super and super tremendous storms (100%). M-class and X-class flares frequently accompany superstorms associated to CMEs. It is observed that 66.6% (4/6) super great geomagnetic storms (Dst ≤ -300nT) were associated with CMEs and solar flares. The number of storms related to X-class flares or CMEs were 50% (3/6). X-class flare/CMEs are found to be responsible for super geomagnetic storms.</Abstract>
			<OtherAbstract Language="FA">We present the findings of a study of the sequence of solar activity that eventually resulted in 80 large geomagnetic storms (distinguished by minimum Dst -100nT to -200nT), 11 super geomagnetic storms (Dst -200nT to -300nT), and 6 super great geomagnetic storms (Dst -300nT) that occurred between 1996 and 2012. Large storms were discovered to be mostly caused by solar flares (M- and X-class), while corotating interaction region (CIR) was also a significant contributor to several of these storms. During the peak and declining phases of solar cycle 23, all extremely powerful storms were observed (2000-2004). It has been noted that coronal mass ejections (CMEs) and flares were always related with super and super tremendous storms (100%). M-class and X-class flares frequently accompany superstorms associated to CMEs. It is observed that 66.6% (4/6) super great geomagnetic storms (Dst ≤ -300nT) were associated with CMEs and solar flares. The number of storms related to X-class flares or CMEs were 50% (3/6). X-class flare/CMEs are found to be responsible for super geomagnetic storms.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">solar flares</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">interplanetary magnetic field</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">coronal mass ejections</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">geomagnetic storms</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_3562_ebf12cb74e96e67e63783d93c534ef27.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>24</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2024</Year>
					<Month>11</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Design and performance analysis of heterojunction dual wire gate all around nanosheet field effect transistor</ArticleTitle>
<VernacularTitle>Design and performance analysis of heterojunction dual wire gate all around nanosheet field effect transistor</VernacularTitle>
			<FirstPage>135</FirstPage>
			<LastPage>145</LastPage>
			<ELocationID EIdType="pii">3538</ELocationID>
			
<ELocationID EIdType="doi">10.47176/ijpr.24.3.31862</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Reza</FirstName>
					<LastName>Abbasnezhad</LastName>
<Affiliation>Department of Electrical Engineering, Shabestar Branch, Islamic Azad University, Shabestar, Iran</Affiliation>
<Identifier Source="ORCID">0000-0002-6767-1381</Identifier>

</Author>
<Author>
					<FirstName>Hassan</FirstName>
					<LastName>Rasooli Saghai</LastName>
<Affiliation>Department of Electrical Engineering, Tabriz Branch, Islamic Azad University, Tabriz, Iran.</Affiliation>

</Author>
<Author>
					<FirstName>Reza</FirstName>
					<LastName>Hosseini</LastName>
<Affiliation>Department of Electrical Engineering, Khoy Branch, Islamic Azad University, Khoy, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Aliasghar</FirstName>
					<LastName>Sedghi</LastName>
<Affiliation>Department of Physics, Shabestar Branch, Islamic Azad University, Shabestar, Iran.</Affiliation>

</Author>
<Author>
					<FirstName>Ali</FirstName>
					<LastName>Vahedi</LastName>
<Affiliation>Department of Physics, Tabriz Branch, Islamic Azad University, Tabriz, Iran</Affiliation>
<Identifier Source="ORCID">0000-0001-7210-1052</Identifier>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2024</Year>
					<Month>03</Month>
					<Day>05</Day>
				</PubDate>
			</History>
		<Abstract>In this paper, we introduce a new variation of the Gate All Around Nanosheet Field Effect Transistor (GAA NS FET) called the Dual Wire (DW), which integrates source heterojunctions and strained channels. We assess its electrical properties across different temperatures (300K, 400K, and 500K) and compare them to those of the Heterojunction DW Gate All Around Nanosheet Field Effect Transistor (Heterojunction DW GAA NS FET) and the Conventional DW Gate All Around Nanosheet Field Effect Transistor (Conventional DW GAA NS FET). Our investigation encompasses the electrostatic control effects on DC and analog parameters, including gate capacitance ( ), transconductance ( ), and cut-off frequency ( ) for all three device types. The channel regions in our structures feature Silicon Germanium (SiGe) (Si/Ge/Si), and the introduction of strain and a heterojunction structure notably enhances device performance. To analyze the semiconductor device accurately, we solve the Density Gradient (DG) equation self-consistently, utilizing the Shockley-Read-Hall (SRH) equation to estimate carrier generation, considering bandgap narrowing in transport behavior, and accounting for auger recombination. Additionally, at temperatures of 300K, 400K, and 500K, the Heterojunction DW GAA NS FET exhibits substantial improvement in  and  compared to the Conventional DW GAA NS FET. Overall, our results show a notable improvement in drain current, transconductance, and unity-gain frequency, with enhancements of around 34%, 9.5%, and 30%, respectively, observed across different temperatures. This improvement translates into superior RF performance for the Heterojunction DW GAA NS FET when compared to the conventional DW GAA NS FET.</Abstract>
			<OtherAbstract Language="FA">In this paper, we introduce a new variation of the Gate All Around Nanosheet Field Effect Transistor (GAA NS FET) called the Dual Wire (DW), which integrates source heterojunctions and strained channels. We assess its electrical properties across different temperatures (300K, 400K, and 500K) and compare them to those of the Heterojunction DW Gate All Around Nanosheet Field Effect Transistor (Heterojunction DW GAA NS FET) and the Conventional DW Gate All Around Nanosheet Field Effect Transistor (Conventional DW GAA NS FET). Our investigation encompasses the electrostatic control effects on DC and analog parameters, including gate capacitance ( ), transconductance ( ), and cut-off frequency ( ) for all three device types. The channel regions in our structures feature Silicon Germanium (SiGe) (Si/Ge/Si), and the introduction of strain and a heterojunction structure notably enhances device performance. To analyze the semiconductor device accurately, we solve the Density Gradient (DG) equation self-consistently, utilizing the Shockley-Read-Hall (SRH) equation to estimate carrier generation, considering bandgap narrowing in transport behavior, and accounting for auger recombination. Additionally, at temperatures of 300K, 400K, and 500K, the Heterojunction DW GAA NS FET exhibits substantial improvement in  and  compared to the Conventional DW GAA NS FET. Overall, our results show a notable improvement in drain current, transconductance, and unity-gain frequency, with enhancements of around 34%, 9.5%, and 30%, respectively, observed across different temperatures. This improvement translates into superior RF performance for the Heterojunction DW GAA NS FET when compared to the conventional DW GAA NS FET.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">half Heusler</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">phase transition</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">dielectic function</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">semiconductor</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">bulk modulus</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">band gap</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_3538_1458e7509aa5f47ecfb92536e7dd1dc7.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>24</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2024</Year>
					<Month>11</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Investigating the lateral distribution distortions of air showers‎ at different observation levels</ArticleTitle>
<VernacularTitle>Investigating the lateral distribution distortions of air showers‎ at different observation levels</VernacularTitle>
			<FirstPage>147</FirstPage>
			<LastPage>151</LastPage>
			<ELocationID EIdType="pii">3566</ELocationID>
			
<ELocationID EIdType="doi">10.47176/ijpr.24.3.81956</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Sozha</FirstName>
					<LastName>Sohaily</LastName>
<Affiliation>Department of Physics, Shahid Bahonar University of Kerman, Kerman, Iran</Affiliation>
<Identifier Source="ORCID">0000-0003-2434-4986</Identifier>

</Author>
<Author>
					<FirstName>Saeed</FirstName>
					<LastName>Doostmohammadi</LastName>
<Affiliation>Department of Physics, Shahid Bahonar University of Kerman, Kerman, Iran</Affiliation>
<Identifier Source="ORCID">0000-0001-9616-0428</Identifier>

</Author>
<Author>
					<FirstName>Negin</FirstName>
					<LastName>Sadeghi Nejad</LastName>
<Affiliation>Department of Physics, Shahid Bahonar University of Kerman, Kerman, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Mohammad</FirstName>
					<LastName>Vaziri</LastName>
<Affiliation>Department of Physics, Kerman Branch, Islamic Azad University, Kerman, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2024</Year>
					<Month>08</Month>
					<Day>16</Day>
				</PubDate>
			</History>
		<Abstract>The comprehension of the basic properties of ultrahigh energy Extensive Air Showers (EAS) is affected by the description of hadronic interactions beyond the LHC energy range. Diffractive interactions with a 20 – 30 percent occurrence probability of all inelastic hadronic collisions lead to high elasticity and large transverse momentum. These interactions are expected to modify the lateral shower development, as well as the measurable observable of the longitudinal profile. This study provides a new approach exploring the impact of diffractive hadronic interactions on lateral development patterns by investigating the fluctuations of simulated lateral distributions. In particular, this research interprets the influence of the observation level and primary energy on fluctuations of lateral electron density. Eventually, an optimized observation level with the maximum fluctuation is introduced as the most probable level to see unconventional EAS.</Abstract>
			<OtherAbstract Language="FA">The comprehension of the basic properties of ultrahigh energy Extensive Air Showers (EAS) is affected by the description of hadronic interactions beyond the LHC energy range. Diffractive interactions with a 20 – 30 percent occurrence probability of all inelastic hadronic collisions lead to high elasticity and large transverse momentum. These interactions are expected to modify the lateral shower development, as well as the measurable observable of the longitudinal profile. This study provides a new approach exploring the impact of diffractive hadronic interactions on lateral development patterns by investigating the fluctuations of simulated lateral distributions. In particular, this research interprets the influence of the observation level and primary energy on fluctuations of lateral electron density. Eventually, an optimized observation level with the maximum fluctuation is introduced as the most probable level to see unconventional EAS.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">extensive air showers</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">lateral distribution function</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">diffractive hadronic interaction</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">observation level</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_3566_6346dc723395e1ee8ef57f4883be4cb4.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>24</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2024</Year>
					<Month>11</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Ionoluminescence investigation of ambient humidity effects on CsI:Na scintillator crystal</ArticleTitle>
<VernacularTitle>Ionoluminescence investigation of ambient humidity effects on CsI:Na scintillator crystal</VernacularTitle>
			<FirstPage>153</FirstPage>
			<LastPage>158</LastPage>
			<ELocationID EIdType="pii">3567</ELocationID>
			
<ELocationID EIdType="doi">10.47176/ijpr.24.3.71931</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Tahereh</FirstName>
					<LastName>Nikbakht</LastName>
<Affiliation>Physics &amp; Accelerators Research School, Nuclear Science and Technology Research Institute (NSTRI), 14395-836, Tehran, Iran</Affiliation>

</Author>
<Author>
					<FirstName>Heidar</FirstName>
					<LastName>Faripour</LastName>
<Affiliation>Photonics and Quantum Technology Research School, Nuclear Science and Technology Research Institute (NSTRI), 14395-836, Tehran, Iran</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2024</Year>
					<Month>07</Month>
					<Day>07</Day>
				</PubDate>
			</History>
		<Abstract>Effects of ambient humidity on the ionoluminescence spectra of synthesized CsI:Na crystals were investigated for a time period of more than 500 days. Regarding the typical penetration depth of the applied ion beams in the ionoluminescence technique, it is suitable for investigating the humidity effects which are detectable at the outer surface of the scintillators. Three luminescence bands were observed for the samples, including CsI intrinsic luminescence and Na related bands, at ~ 310, 420 and 487 nm. It is shown that the relative intensity of the Na-related band, located at ~ 420 nm, significantly decreases over exposition time to humidity and exhibits considerable redshift. Since this band is the dominant one for detection purposes, its alteration leads to a decrease in the efficiency of CsI:Na scintillator. It was also observed that the relative intensity of this band for the sample which was grown in presence of trivial amount of humidity in the crucible, was initially much weaker and reacted less to the ambient humidity. The results of the present work demonstrate the capabilities of ionoluminescence as a suitable technique for scintillators’ characterization.</Abstract>
			<OtherAbstract Language="FA">Effects of ambient humidity on the ionoluminescence spectra of synthesized CsI:Na crystals were investigated for a time period of more than 500 days. Regarding the typical penetration depth of the applied ion beams in the ionoluminescence technique, it is suitable for investigating the humidity effects which are detectable at the outer surface of the scintillators. Three luminescence bands were observed for the samples, including CsI intrinsic luminescence and Na related bands, at ~ 310, 420 and 487 nm. It is shown that the relative intensity of the Na-related band, located at ~ 420 nm, significantly decreases over exposition time to humidity and exhibits considerable redshift. Since this band is the dominant one for detection purposes, its alteration leads to a decrease in the efficiency of CsI:Na scintillator. It was also observed that the relative intensity of this band for the sample which was grown in presence of trivial amount of humidity in the crucible, was initially much weaker and reacted less to the ambient humidity. The results of the present work demonstrate the capabilities of ionoluminescence as a suitable technique for scintillators’ characterization.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">CsI:Na scintillator</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">ionoluminescence</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">humidity effect</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_3567_dccab9bd9e0b69c49302025efdf19702.pdf</ArchiveCopySource>
</Article>
</ArticleSet>
