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<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>14</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Multichannel Kondo approach to the cuprate and recent laser ARPES data</ArticleTitle>
<VernacularTitle>Multichannel Kondo approach to the cuprate and recent laser ARPES data</VernacularTitle>
			<FirstPage>25</FirstPage>
			<LastPage>34</LastPage>
			<ELocationID EIdType="pii">1084</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>M A</FirstName>
					<LastName>Mojumder</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>The existing theoretical approaches have been unable to confront the large corpus of outstanding data on the cuprate superconductor in a persuasive and unified manner. There is a general opinion now growing that these theories miss some essential points. We propose one based on multichannel Kondo effect that is  physically justifiable and confronts the data adequately. In addition to earlier data, the definitive proof of involvement of this effect has been now provided by the numerical agreement of the characteristic Kondo temperatures with the fluctuation frequencies at which Eliashberg function peaks. It is, therefore, suggested that the theory of multichannel Kondo effect be accepted as the correct theory of underdoped cuprate.</Abstract>
			<OtherAbstract Language="FA">The existing theoretical approaches have been unable to confront the large corpus of outstanding data on the cuprate superconductor in a persuasive and unified manner. There is a general opinion now growing that these theories miss some essential points. We propose one based on multichannel Kondo effect that is  physically justifiable and confronts the data adequately. In addition to earlier data, the definitive proof of involvement of this effect has been now provided by the numerical agreement of the characteristic Kondo temperatures with the fluctuation frequencies at which Eliashberg function peaks. It is, therefore, suggested that the theory of multichannel Kondo effect be accepted as the correct theory of underdoped cuprate.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">cuprates physics</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">high-Tc superconductivity</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">multichannel Kondo effect</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">pseudogap</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">of two channel Kondo effect</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_1084_9f36407ead0629fc166f14dde7970f68.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>14</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Strange quark matter attached to string cloud in general scalar tensor theory of gravitation</ArticleTitle>
<VernacularTitle>Strange quark matter attached to string cloud in general scalar tensor theory of gravitation</VernacularTitle>
			<FirstPage>35</FirstPage>
			<LastPage>39</LastPage>
			<ELocationID EIdType="pii">1085</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>V U M</FirstName>
					<LastName>Rao</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>D</FirstName>
					<LastName>Neelima</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>Bianchi type-VI0 space time with strange quark matter attached to string cloud in Nordtvedt [1] general scalar tensor theory of gravitation with the help of a special case proposed by Schwinger [2] is obtained. The field equations have been solved by using the anisotropy feature of the universe in the Bianchi type-VI0 space time. Some important features of the model, thus obtained, have been discussed</Abstract>
			<OtherAbstract Language="FA">Bianchi type-VI0 space time with strange quark matter attached to string cloud in Nordtvedt [1] general scalar tensor theory of gravitation with the help of a special case proposed by Schwinger [2] is obtained. The field equations have been solved by using the anisotropy feature of the universe in the Bianchi type-VI0 space time. Some important features of the model, thus obtained, have been discussed</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Bianchi type-VI0</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">quark matter</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">cosmic strings</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">general scalar tensor theory of gravitation</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_1085_4f16c818875d9fcb6867c7bdc89be7eb.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>14</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Influence of shielding gas composition on weld profile in pulsed Nd:YAG laser welding of low carbon steel</ArticleTitle>
<VernacularTitle>Influence of shielding gas composition on weld profile in pulsed Nd:YAG laser welding of low carbon steel</VernacularTitle>
			<FirstPage>41</FirstPage>
			<LastPage>46</LastPage>
			<ELocationID EIdType="pii">1086</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>M</FirstName>
					<LastName>Jokar</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>F</FirstName>
					<LastName>MalekGhaini</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>M J</FirstName>
					<LastName>Torkamany</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>M</FirstName>
					<LastName>Sheikhi</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>Weld area and weld depth/width ratio can be considered to be of the most important geometrical factors in pulsed laser welding. The effects of carbon dioxide and oxygen additions to the argon shielding gas on the weld properties in pulsed laser welding of low carbon steel is investigated. Presence of carbon dioxide and oxygen up to 10 and 15 percent respectively decreases the weld geometrical factors. But, at higher levels of additions, the weld geometrical factors will increase. It is observed that the plasma plume temperature decreases from 6000K to 5500K with the addition of 15% carbon dioxide but increases to 7700K with 25% carbon dioxide addition. Increase in laser absorption coefficient, laser energy absorption, formation of oxide layer on the work-piece surface, exothermic reactions and their competitive effects can be considered as the competing phenomena involved in such a behavior in the weld profile</Abstract>
			<OtherAbstract Language="FA">Weld area and weld depth/width ratio can be considered to be of the most important geometrical factors in pulsed laser welding. The effects of carbon dioxide and oxygen additions to the argon shielding gas on the weld properties in pulsed laser welding of low carbon steel is investigated. Presence of carbon dioxide and oxygen up to 10 and 15 percent respectively decreases the weld geometrical factors. But, at higher levels of additions, the weld geometrical factors will increase. It is observed that the plasma plume temperature decreases from 6000K to 5500K with the addition of 15% carbon dioxide but increases to 7700K with 25% carbon dioxide addition. Increase in laser absorption coefficient, laser energy absorption, formation of oxide layer on the work-piece surface, exothermic reactions and their competitive effects can be considered as the competing phenomena involved in such a behavior in the weld profile</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">weld area</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">weld depth/width ratio</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">laser welding</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">shielding gas</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">weld profile</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">plasma plume</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_1086_d91d1b4d82419de8a614abce9cc0e6d4.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>14</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Formation of different microstructures on a polyethersulfone film following XeCl laser irradiation</ArticleTitle>
<VernacularTitle>Formation of different microstructures on a polyethersulfone film following XeCl laser irradiation</VernacularTitle>
			<FirstPage>47</FirstPage>
			<LastPage>52</LastPage>
			<ELocationID EIdType="pii">1087</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>H</FirstName>
					<LastName>Pazokian</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>M</FirstName>
					<LastName>Mollabashi</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>S</FirstName>
					<LastName>Jelvani</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>J</FirstName>
					<LastName>Barzin</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>SH</FirstName>
					<LastName>Abolhoseini</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>Laser irradiation parameters, especially the laser fluence and the number of pulses are very important factors affecting microstructures formation and improvement of the surface characteristics in different medical, electronic and the other industrial applications. Information about the fluence domain and the number of pulses for the formation of the structures is very important and determines the desirable or unwanted effects of the laser irradiation on the surfaces regarding the desired applications. In this paper Polyethersulfone films were irradiated with a XeCl laser at fluences above the ablation threshold. The effects of the laser fluence and the number of pulses on the formation of different microstructures on the surface were investigated</Abstract>
			<OtherAbstract Language="FA">Laser irradiation parameters, especially the laser fluence and the number of pulses are very important factors affecting microstructures formation and improvement of the surface characteristics in different medical, electronic and the other industrial applications. Information about the fluence domain and the number of pulses for the formation of the structures is very important and determines the desirable or unwanted effects of the laser irradiation on the surfaces regarding the desired applications. In this paper Polyethersulfone films were irradiated with a XeCl laser at fluences above the ablation threshold. The effects of the laser fluence and the number of pulses on the formation of different microstructures on the surface were investigated</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">polyethersulfone</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">XeCl laser</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">microstructure</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Cone- periodic ripples</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_1087_a26398dca6f47b49876cbaffbc9954f9.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>14</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Synthesis and characterization of MWCNT/CdS nanocomposite</ArticleTitle>
<VernacularTitle>Synthesis and characterization of MWCNT/CdS nanocomposite</VernacularTitle>
			<FirstPage>53</FirstPage>
			<LastPage>56</LastPage>
			<ELocationID EIdType="pii">1088</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>M R</FirstName>
					<LastName>Khanlary</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>M</FirstName>
					<LastName>Keshavarz</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>In this work we report the synthesis and characterization of hybrid nanostructures of multiwall carbon nanotubes (MWCNT) and cadmium sulphide (CdS) nanoparticles. In a solution of thioacetamide and cadmium sulphide, purified MWCNT are added to prepare the CNT/CdS hetrostructure. XRD diagrams, SEM images, and also photoluminescence spectra of the prepared samples are analyzed. SEM images show the CdS nanoparticles of 17nm size coated on the CNTs. Visible photoluminescence with peaks at 435 nm and 535 nm, obtained from the prepared CNT/CdS, is discussed. The synthesis technique can be simply extended to other luminescent dopants, and the possibility of making optoelectronic devises based on the CNTs is confirmed by this method</Abstract>
			<OtherAbstract Language="FA">In this work we report the synthesis and characterization of hybrid nanostructures of multiwall carbon nanotubes (MWCNT) and cadmium sulphide (CdS) nanoparticles. In a solution of thioacetamide and cadmium sulphide, purified MWCNT are added to prepare the CNT/CdS hetrostructure. XRD diagrams, SEM images, and also photoluminescence spectra of the prepared samples are analyzed. SEM images show the CdS nanoparticles of 17nm size coated on the CNTs. Visible photoluminescence with peaks at 435 nm and 535 nm, obtained from the prepared CNT/CdS, is discussed. The synthesis technique can be simply extended to other luminescent dopants, and the possibility of making optoelectronic devises based on the CNTs is confirmed by this method</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">CVD</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">nanocomposite</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">carbon nanotubes</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">cadmium Sulphide</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">photoluminescence</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_1088_b1563a78ec59337587f6ab6397699afc.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>14</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Investigation into the temperature dependence of isotropic- nematic phase transition of Gay- Berne liquid crystals</ArticleTitle>
<VernacularTitle>Investigation into the temperature dependence of isotropic- nematic phase transition of Gay- Berne liquid crystals</VernacularTitle>
			<FirstPage>57</FirstPage>
			<LastPage>65</LastPage>
			<ELocationID EIdType="pii">1089</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>A</FirstName>
					<LastName>Avazpour</LastName>
<Affiliation></Affiliation>
<Identifier Source="ORCID">0000-0001-7650-7105</Identifier>

</Author>
<Author>
					<FirstName>S M</FirstName>
					<LastName>Hekmatzadeh</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>Density functional approach was used to study the isotropic- nematic (I-N) transition and calculate the values of freezing parameters of the Gay- Berne liquid crystal model. New direct and pair correlation functions of a molecular fluid with Gay- Berne pair potential were used. These new functions were used in density functional theory as input to calculate the isotropic- nematic transition densities for elongation   at various reduced temperatures. It was observed that the isotropic- nematic transition densities increase as the temperature increases. It was found that the new direct correlation function is suitable to study the isotropic- nematic transition of Gay- Berne liquids. Comparison to other works showed qualitative agreement</Abstract>
			<OtherAbstract Language="FA">Density functional approach was used to study the isotropic- nematic (I-N) transition and calculate the values of freezing parameters of the Gay- Berne liquid crystal model. New direct and pair correlation functions of a molecular fluid with Gay- Berne pair potential were used. These new functions were used in density functional theory as input to calculate the isotropic- nematic transition densities for elongation   at various reduced temperatures. It was observed that the isotropic- nematic transition densities increase as the temperature increases. It was found that the new direct correlation function is suitable to study the isotropic- nematic transition of Gay- Berne liquids. Comparison to other works showed qualitative agreement</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Gay- Berne potential</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">direct correlation function</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">density functional theory</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">isotropic- nematic transition</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_1089_03f544613917945245041ea1581df0c2.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>14</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Electronic transport through dsDNA based junction: a Fibonacci model</ArticleTitle>
<VernacularTitle>Electronic transport through dsDNA based junction: a Fibonacci model</VernacularTitle>
			<FirstPage>67</FirstPage>
			<LastPage>72</LastPage>
			<ELocationID EIdType="pii">1090</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>S A</FirstName>
					<LastName>Ketabi</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>H</FirstName>
					<LastName>Khouzestani</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>A numerical study is presented to investigate the electronic transport properties through a synthetic DNA molecule based on a quasiperiodic arrangement of its constituent nucleotides. Using a generalized Green&#039;s function technique, the electronic conduction through the poly(GACT)-poly(CTGA) DNA molecule in a metal/DNA/metal model structure has been studied. Making use of a renormalization scheme we transform the Hamiltonian of double-stranded DNA (dsDNA) molecule to an effective Hamiltonian corresponding to a one-dimensional chain in which the effective on-site energies are arranged as a quasiperiodic lattice according to Fibonacci sequence. The room temperature current-voltage characteristic of dsDNA has been investigated in this Fibonacci model and compared with those corresponding to poly(GACT)-poly(CTGA) DNA molecule. Our results indicate the main effect of the quasiperiodic arrangement of the nucleotides as the Fibonacci sequence on the electronic spectrum structure of the dsDNA is that the energy band gaps of the molecule have a tendency for suppression. The room temperature I-V characteristic of the DNA Fibonacci model shows a linear and ohmic-like behavior</Abstract>
			<OtherAbstract Language="FA">A numerical study is presented to investigate the electronic transport properties through a synthetic DNA molecule based on a quasiperiodic arrangement of its constituent nucleotides. Using a generalized Green&#039;s function technique, the electronic conduction through the poly(GACT)-poly(CTGA) DNA molecule in a metal/DNA/metal model structure has been studied. Making use of a renormalization scheme we transform the Hamiltonian of double-stranded DNA (dsDNA) molecule to an effective Hamiltonian corresponding to a one-dimensional chain in which the effective on-site energies are arranged as a quasiperiodic lattice according to Fibonacci sequence. The room temperature current-voltage characteristic of dsDNA has been investigated in this Fibonacci model and compared with those corresponding to poly(GACT)-poly(CTGA) DNA molecule. Our results indicate the main effect of the quasiperiodic arrangement of the nucleotides as the Fibonacci sequence on the electronic spectrum structure of the dsDNA is that the energy band gaps of the molecule have a tendency for suppression. The room temperature I-V characteristic of the DNA Fibonacci model shows a linear and ohmic-like behavior</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">DNA</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Green's function</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">current-voltage characteristic</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Fibonacci model</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Green\'s function</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_1090_8b4066554730ddfaa0266346bdc1b202.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>14</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Damping of visco-resistive Alfven waves in solar spicules</ArticleTitle>
<VernacularTitle>Damping of visco-resistive Alfven waves in solar spicules</VernacularTitle>
			<FirstPage>73</FirstPage>
			<LastPage>78</LastPage>
			<ELocationID EIdType="pii">1091</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Z</FirstName>
					<LastName>Fazel</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>H</FirstName>
					<LastName>Ebadi</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>Interaction of Alfven waves with plasma inhomogeneity generates phase mixing which can cause the dissipation of Alfven waves. We investigated the dissipation of standing Alfven waves due to phase mixing at the presence of steady flow and sheared magnetic field in solar spicules. Moreover, the transition region between chromosphere and corona was considered. Our numerical simulation showed that the phase mixing and dissipation rate of Alfven waves are enhanced relative to viscosity and resistivity gradients. Comparison of the results of our models with and without these gradients illustrated a significant difference between them. In other words, with these assumptions, Alfven waves may transfer the photospheric energy to the corona during timescales corresponding to the observed lifetimes of spicules. It should be noted that the results of our numerical simulation were in good agreement with observational scaling law obtained by Kuridze et al. [1]</Abstract>
			<OtherAbstract Language="FA">Interaction of Alfven waves with plasma inhomogeneity generates phase mixing which can cause the dissipation of Alfven waves. We investigated the dissipation of standing Alfven waves due to phase mixing at the presence of steady flow and sheared magnetic field in solar spicules. Moreover, the transition region between chromosphere and corona was considered. Our numerical simulation showed that the phase mixing and dissipation rate of Alfven waves are enhanced relative to viscosity and resistivity gradients. Comparison of the results of our models with and without these gradients illustrated a significant difference between them. In other words, with these assumptions, Alfven waves may transfer the photospheric energy to the corona during timescales corresponding to the observed lifetimes of spicules. It should be noted that the results of our numerical simulation were in good agreement with observational scaling law obtained by Kuridze et al. [1]</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">solar spicules</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Alfven waves</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">damping</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">transition region</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_1091_754dda4b1ba34c6fa89716b85d68532b.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>14</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>High order perturbation study of the frustrated quantum Ising chain</ArticleTitle>
<VernacularTitle>High order perturbation study of the frustrated quantum Ising chain</VernacularTitle>
			<FirstPage>79</FirstPage>
			<LastPage>83</LastPage>
			<ELocationID EIdType="pii">1092</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>A</FirstName>
					<LastName>Hajibabaei</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>F</FirstName>
					<LastName>Shahbazi</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>In this paper, using high order perturbative series expansion method, the critical exponents of the order parameter and susceptibility in transition from ferromagnetic to disordered phases for 1D quantum Ising model in transverse field, with ferromagnetic nearest neighbor and anti-ferromagnetic next to nearest neighbor interactions, are calculated. It is found that for small value of the frustrating second neighbor coupling ( k</Abstract>
			<OtherAbstract Language="FA">In this paper, using high order perturbative series expansion method, the critical exponents of the order parameter and susceptibility in transition from ferromagnetic to disordered phases for 1D quantum Ising model in transverse field, with ferromagnetic nearest neighbor and anti-ferromagnetic next to nearest neighbor interactions, are calculated. It is found that for small value of the frustrating second neighbor coupling ( k</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">quantum phase transition</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">quantum Ising model</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">cluster expansion</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">series expansion</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">frustrated systems</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">ANNNI model</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_1092_6a2feef8ed6a9fe76d6b3f30f02150b4.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>14</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>QED second order corrections on the speed of light at low temperature</ArticleTitle>
<VernacularTitle>QED second order corrections on the speed of light at low temperature</VernacularTitle>
			<FirstPage>85</FirstPage>
			<LastPage>88</LastPage>
			<ELocationID EIdType="pii">1093</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>M</FirstName>
					<LastName>‎Razmi</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>H</FirstName>
					<LastName>Zamani</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>We want to study thermal corrections on the speed of light at low temperature considering temperature dependence of  photon vacuum polarization tensor at two-loop level in the standard QED‎. It is found that the heat bath  behaves as a dispersive medium for the propagation of light and reduces its speed proportional to the second order of temperature‎. ‎Similarities and differences‎, ‎in light of already known calculations which are based on Euler-Heisenberg Lagrangian and/or those using temperature dependent electromagnetic properties of the medium are discussed‎.</Abstract>
			<OtherAbstract Language="FA">We want to study thermal corrections on the speed of light at low temperature considering temperature dependence of  photon vacuum polarization tensor at two-loop level in the standard QED‎. It is found that the heat bath  behaves as a dispersive medium for the propagation of light and reduces its speed proportional to the second order of temperature‎. ‎Similarities and differences‎, ‎in light of already known calculations which are based on Euler-Heisenberg Lagrangian and/or those using temperature dependent electromagnetic properties of the medium are discussed‎.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">QED radiative corrections</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">finite temperature quantum field theory</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">the speed of light</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_1093_68b1fbe7f16e4ae3024973f12f3cb313.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>14</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>A study of energy gap, refractive index and electronic polarizability of ternary chalcopyrite semiconductors</ArticleTitle>
<VernacularTitle>A study of energy gap, refractive index and electronic polarizability of ternary chalcopyrite semiconductors</VernacularTitle>
			<FirstPage>89</FirstPage>
			<LastPage>93</LastPage>
			<ELocationID EIdType="pii">1094</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>A</FirstName>
					<LastName>Ahmad</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>M</FirstName>
					<LastName>Mohib-ul Haq</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>A simple relation between the optical electronegativity, energy gap, refractive index and electronic polarizability is given for ternary chalcopyrite semiconductors. Energy gap has been evaluated from the optical electronegativity whereas refractive index and electronic polarizability values have been evaluated from the energy gap by proposing a linear relation between them. The calculated values are in fair agreement with the experimental values and earlier researchers. This work highlights the significance of interrelation between these parameters.</Abstract>
			<OtherAbstract Language="FA">A simple relation between the optical electronegativity, energy gap, refractive index and electronic polarizability is given for ternary chalcopyrite semiconductors. Energy gap has been evaluated from the optical electronegativity whereas refractive index and electronic polarizability values have been evaluated from the energy gap by proposing a linear relation between them. The calculated values are in fair agreement with the experimental values and earlier researchers. This work highlights the significance of interrelation between these parameters.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">semiconductors</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">electronegativity</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">energy gap</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">refractive index and electronic polarizability</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_1094_41bfd20a38bb1b0bec75acf0845530a7.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>14</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Studies of Three-Body B^+âD Ì^* ã(2007)ã^0 K^+ K Ì^0 and B^0âD^* ã(2010)ã^- K^+ K Ì^0 Decays</ArticleTitle>
<VernacularTitle>Studies of Three-Body B^+âD Ì^* ã(2007)ã^0 K^+ K Ì^0 and B^0âD^* ã(2010)ã^- K^+ K Ì^0 Decays</VernacularTitle>
			<FirstPage>95</FirstPage>
			<LastPage>100</LastPage>
			<ELocationID EIdType="pii">1095</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>B</FirstName>
					<LastName>Mohammadi</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>H</FirstName>
					<LastName>Mehraban</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>We analyze three-body decays of and . Under the factorization approach, there are tree level diagrams for these decay modes and the transition matrix element of decay is factorized into a  form factor multiplied by  decay constant and form factor multiplied into weak vertices form factor. The transition matrix element of  decay is also factorized into a  form factor multiplied into  weak vertices form factor. We investigate these decays by using the Dalitz plot technique. First, we use the general form of this technique and calculate the branching ratios of the  and  decays and obtain the values  of and , while the experimental results are less than  and respectively. Then we assume that, in the  decays, because the mass of the  is too heavy against the K-mesons.So the momentum of the  can have a small amount. Namely, the  carries small momentum. In the probability summation of the amplitudes, the momentum of the , instead of starting from its maximum value, starts from a state in which two light mesons make an angle of  degrees. Using our assumption, we calculate the branching ratios of and  decays and obtain  and  respectively. In addition, we estimate the branching ratios for different angles between the two light mesons and get that when the angle between them is , in fact they decay back to back, and these values become  and , which are the best answers close to the experimental values. The branching ratios obtained by applying our assumption are compatible with the experimental results.</Abstract>
			<OtherAbstract Language="FA">We analyze three-body decays of and . Under the factorization approach, there are tree level diagrams for these decay modes and the transition matrix element of decay is factorized into a  form factor multiplied by  decay constant and form factor multiplied into weak vertices form factor. The transition matrix element of  decay is also factorized into a  form factor multiplied into  weak vertices form factor. We investigate these decays by using the Dalitz plot technique. First, we use the general form of this technique and calculate the branching ratios of the  and  decays and obtain the values  of and , while the experimental results are less than  and respectively. Then we assume that, in the  decays, because the mass of the  is too heavy against the K-mesons.So the momentum of the  can have a small amount. Namely, the  carries small momentum. In the probability summation of the amplitudes, the momentum of the , instead of starting from its maximum value, starts from a state in which two light mesons make an angle of  degrees. Using our assumption, we calculate the branching ratios of and  decays and obtain  and  respectively. In addition, we estimate the branching ratios for different angles between the two light mesons and get that when the angle between them is , in fact they decay back to back, and these values become  and , which are the best answers close to the experimental values. The branching ratios obtained by applying our assumption are compatible with the experimental results.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">B meson decays</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">factorization</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">dalitz plot analysis</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_1095_d6723e7cd6735df68d1ce4c704c29a04.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>14</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Low loss coupler to interface silicon waveguide and hybrid plasmonic waveguide</ArticleTitle>
<VernacularTitle>Low loss coupler to interface silicon waveguide and hybrid plasmonic waveguide</VernacularTitle>
			<FirstPage>101</FirstPage>
			<LastPage>103</LastPage>
			<ELocationID EIdType="pii">1096</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>H R</FirstName>
					<LastName>Zangeneh</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>M</FirstName>
					<LastName>Asadnia Fard Jahromi</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>A metallic coupler is proposed to interface a silicon on insulator (SOI) waveguide with a narrow hybrid plasmonic waveguide (200× 200 nm). The device operation is investigated and optimized to attain the best tradeoff between the mode confinement and the propagation loss. Calculations reveal that a high confinement and low loss of the energy is achieved from a silicon slab waveguide into the dielectric slot of area 200×200 nm2 and a coupling efficiency of 70% (0.8 dB) at the 1.55 μm telecommunication wavelength can be achieved</Abstract>
			<OtherAbstract Language="FA">A metallic coupler is proposed to interface a silicon on insulator (SOI) waveguide with a narrow hybrid plasmonic waveguide (200× 200 nm). The device operation is investigated and optimized to attain the best tradeoff between the mode confinement and the propagation loss. Calculations reveal that a high confinement and low loss of the energy is achieved from a silicon slab waveguide into the dielectric slot of area 200×200 nm2 and a coupling efficiency of 70% (0.8 dB) at the 1.55 μm telecommunication wavelength can be achieved</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">surface plasmon</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">waveguide</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">coupler</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_1096_4e2545f819e67f0615003dd7e04a6087.pdf</ArchiveCopySource>
</Article>
</ArticleSet>
