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<ArticleSet>
<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>7</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>The effect of crystalline and shape anisotropy on the magnetic properties of Co and Ni nanowires</ArticleTitle>
<VernacularTitle>The effect of crystalline and shape anisotropy on the magnetic properties of Co and Ni nanowires</VernacularTitle>
			<FirstPage>73</FirstPage>
			<LastPage>80</LastPage>
			<ELocationID EIdType="pii">568</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName></FirstName>
					<LastName>R. Golipour</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName></FirstName>
					<LastName>A. Khayyatian</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName></FirstName>
					<LastName>A. Ramazani</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName></FirstName>
					<LastName>M. Almasi Kashi</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>  Co and Ni magnetic nanowires with different diameter and deposition time were fabricated into the alumina template using ac electrodeposition. For Ni nanowires with 30 nm diameter the coercivity initially increased then dropped with deposition time, while it only increased with deposition time for all the other diameters. In general, the results showed that the coercivity reduced with diameter. The maximum coercivity was obtained for the Co nanowire made with 30 nm diameter and 30 s deposition time and further electrodeposition time causes a reduction of the coercivity. The effect of crystal and shape anisotropy on the magnetic properties were investigated and the results revealed that the crystal anisotropy has a dominant role on the coercive field of Co nanowires, while there is a competitive effect between both the anisotropies for the Ni nanowires changing the coercivity.</Abstract>
			<OtherAbstract Language="FA">  Co and Ni magnetic nanowires with different diameter and deposition time were fabricated into the alumina template using ac electrodeposition. For Ni nanowires with 30 nm diameter the coercivity initially increased then dropped with deposition time, while it only increased with deposition time for all the other diameters. In general, the results showed that the coercivity reduced with diameter. The maximum coercivity was obtained for the Co nanowire made with 30 nm diameter and 30 s deposition time and further electrodeposition time causes a reduction of the coercivity. The effect of crystal and shape anisotropy on the magnetic properties were investigated and the results revealed that the crystal anisotropy has a dominant role on the coercive field of Co nanowires, while there is a competitive effect between both the anisotropies for the Ni nanowires changing the coercivity.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Co nanowire</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Ni nanowire</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">crystal anisotropy</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">shape anisotropy</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">porous alumina</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_568_dd458505749b2941217ddd59394240e8.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>7</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>The structural and thermodynamical properties of binary ellipsoidal fluid mixture Gay-Berne interaction</ArticleTitle>
<VernacularTitle>The structural and thermodynamical properties of binary ellipsoidal fluid mixture Gay-Berne interaction</VernacularTitle>
			<FirstPage>81</FirstPage>
			<LastPage>90</LastPage>
			<ELocationID EIdType="pii">569</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName></FirstName>
					<LastName>M. Moradi</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName></FirstName>
					<LastName>R. Khordad</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, a uniform classical fluid mixture comprising ellipsoidal molecules is studied. This mixture is composed of two types of ellipsoidal molecules interacting through the Gay-Berne potential with different sizes at temperature T. For this system, the Ornstein-Zernike equation using the Percus-Yevick closure relation is solved. Then the direct correlation function, pair correlation function and the pressure of the fluid at temperature T are calculated. The obtained results are in agreement with the previous theories and the results of molecular dynamic computer simulation.</Abstract>
			<OtherAbstract Language="FA"> In this paper, a uniform classical fluid mixture comprising ellipsoidal molecules is studied. This mixture is composed of two types of ellipsoidal molecules interacting through the Gay-Berne potential with different sizes at temperature T. For this system, the Ornstein-Zernike equation using the Percus-Yevick closure relation is solved. Then the direct correlation function, pair correlation function and the pressure of the fluid at temperature T are calculated. The obtained results are in agreement with the previous theories and the results of molecular dynamic computer simulation.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">molecular fluids</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">binary mixture</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Gay-Berne interaction</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">correlation functions</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_569_8b16ebc056e613024c057be590b542eb.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>7</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>The mean field study of phase transitions in two dimensional Kagome lattice under local anisotropy</ArticleTitle>
<VernacularTitle>The mean field study of phase transitions in two dimensional Kagome lattice under local anisotropy</VernacularTitle>
			<FirstPage>91</FirstPage>
			<LastPage>100</LastPage>
			<ELocationID EIdType="pii">570</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName></FirstName>
					<LastName>S. Mortezapour</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName></FirstName>
					<LastName>F. 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 work we investigated the critical properties of the anti-ferromagnetic XY model on a two dimensional Kagome lattice under single-ion easy-axes anisotropy. Employing the mean field theory, we found that this model shows a second order phase transition from disordered to all-in all-out state for any value of anisotropy.</Abstract>
			<OtherAbstract Language="FA"> In this work we investigated the critical properties of the anti-ferromagnetic XY model on a two dimensional Kagome lattice under single-ion easy-axes anisotropy. Employing the mean field theory, we found that this model shows a second order phase transition from disordered to all-in all-out state for any value of anisotropy.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">XY model</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Kagome lattice</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">mean field theory</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">magnetic frustration</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_570_a86c450b76fb8c371afead6410d55534.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>7</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>The self-consistent method in calculating the ratio by using the structure functions and EMC ratios for 3He and 3H</ArticleTitle>
<VernacularTitle>The self-consistent method in calculating the ratio by using the structure functions and EMC ratios for 3He and 3H</VernacularTitle>
			<FirstPage>101</FirstPage>
			<LastPage>105</LastPage>
			<ELocationID EIdType="pii">571</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>M</FirstName>
					<LastName>Modarres</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>R</FirstName>
					<LastName>Mohammadi</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>By using the convolution formalism which consists of Fermi motion and binding effect, we investigate the deep inelastic electron scattering from A=3 mirror in the deep-valence region. The initial valence quark input is taken from the GRVs (Gluck, Reya and Vogt) fitting procedure and the next-to-leading order QCD evolution on FP &lt; /sup&gt;2 (x,Q2) which gives very good fit to the available data in the (x,Q2)-plane. It is shown that the free neutron to proton structure function ratios can be extracted from the corresponding EMC ratios for 3He and 3H mirror nuclei using the self - consistent iteration procedure and the results are in good agreement with other theoretical models as well as the current available experimental data and especially the projected data expected from the proposed 11GeV Jefferson Laboratory in near future.</Abstract>
			<OtherAbstract Language="FA">By using the convolution formalism which consists of Fermi motion and binding effect, we investigate the deep inelastic electron scattering from A=3 mirror in the deep-valence region. The initial valence quark input is taken from the GRVs (Gluck, Reya and Vogt) fitting procedure and the next-to-leading order QCD evolution on FP &lt; /sup&gt;2 (x,Q2) which gives very good fit to the available data in the (x,Q2)-plane. It is shown that the free neutron to proton structure function ratios can be extracted from the corresponding EMC ratios for 3He and 3H mirror nuclei using the self - consistent iteration procedure and the results are in good agreement with other theoretical models as well as the current available experimental data and especially the projected data expected from the proposed 11GeV Jefferson Laboratory in near future.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">structure function</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">EMC effect</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Fermi motion</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">self - consistent iteration equation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">convolution formalism</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_571_c9892a989183de32e976c6f04e700201.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>7</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Determining of electron temperature profile on the cross section of a Tokamak, using ECE technique</ArticleTitle>
<VernacularTitle>Determining of electron temperature profile on the cross section of a Tokamak, using ECE technique</VernacularTitle>
			<FirstPage>107</FirstPage>
			<LastPage>111</LastPage>
			<ELocationID EIdType="pii">572</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName></FirstName>
					<LastName>M. Hosseinpour</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName></FirstName>
					<LastName>A. Anvari</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName></FirstName>
					<LastName>M. Ghorannevis</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 we have used plasma electron cyclotron emissions at the second harmonic frequency of extraordinary mode to determine the temperature profile of the plasma produced in IR-T1 Tokamak. The emissions obtained at different frequencies by a 5-channel heterodyne receiver, have been analyzed to determine the spatial variation of the electron temperature on the plasma cross section. The results have been also used to show the three-dimensional time evolution of the temperature profile during the period of confinement.</Abstract>
			<OtherAbstract Language="FA"> In this paper we have used plasma electron cyclotron emissions at the second harmonic frequency of extraordinary mode to determine the temperature profile of the plasma produced in IR-T1 Tokamak. The emissions obtained at different frequencies by a 5-channel heterodyne receiver, have been analyzed to determine the spatial variation of the electron temperature on the plasma cross section. The results have been also used to show the three-dimensional time evolution of the temperature profile during the period of confinement.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">IR-T1 Tokamak</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">electron cyclotron emission</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">electron temperature</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_572_e6b4b2a746ed40e1af829d1fa82daa10.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>7</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Multiscale entropy (MSE) and multicomponent complexity (MCC)</ArticleTitle>
<VernacularTitle>Multiscale entropy (MSE) and multicomponent complexity (MCC)</VernacularTitle>
			<FirstPage>113</FirstPage>
			<LastPage>118</LastPage>
			<ELocationID EIdType="pii">573</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName></FirstName>
					<LastName>M. Boorboor</LastName>
<Affiliation></Affiliation>

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

</Author>
<Author>
					<FirstName></FirstName>
					<LastName>B. Mirza</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>Multiscale entropy (MSE) is a powerful method for determining the complexity of random time series. In this paper we, investigate the cardiac heart interbeat interval (RR) time series by introducing a new method based on MSE, called multicomponent complexity (MCC) and find clear difference between healthy samples and samples with Congestive heart failure (CHF) disease.</Abstract>
			<OtherAbstract Language="FA">Multiscale entropy (MSE) is a powerful method for determining the complexity of random time series. In this paper we, investigate the cardiac heart interbeat interval (RR) time series by introducing a new method based on MSE, called multicomponent complexity (MCC) and find clear difference between healthy samples and samples with Congestive heart failure (CHF) disease.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">sample entropy</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">multiscale entropy</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">multicomponent complexity</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">coarse graining</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_573_e5f6ad6ce374177eef023bf5d0c018b6.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>7</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Barrier and well-width dependence of optical emission of GaN/AlGaN quantum well nanostructures</ArticleTitle>
<VernacularTitle>Barrier and well-width dependence of optical emission of GaN/AlGaN quantum well nanostructures</VernacularTitle>
			<FirstPage>119</FirstPage>
			<LastPage>125</LastPage>
			<ELocationID EIdType="pii">574</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName></FirstName>
					<LastName>H. Haratizadeh</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName></FirstName>
					<LastName>M. Esmaeili</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName></FirstName>
					<LastName>P. O. Holtz</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>Internal polarizations field which take place in quantum structures of group-III nitrides have an important consequence on their optical properties. Optical properties of wurtzite AlGaN/GaN quantum well (QW) structures grown by MBE and MOCVD on c-plane sapphire substrates have been investigated by means of photoluminescence (PL) and time resolved photoluminescence (TRPL) at low-temperature. PL spectra exhibit a blue-shifted emission of AlGaN/GaN quantum well (QW) nanostructures by decreasing the barrier width contrary to the arsenide system. The trend of the barrier-width dependence of the internal polarization field is reproduced by using simple electrostatic arguments. In addition the effect of well width variation on the optical transition and decay time of GaN MQWs have been investigated and it has been shown that the screening of the piezoelectric field and the electron-hole separation are strongly dependent on the well thickness and have a profound effect on the optical properties of the GaN/AlGaN MQWs.</Abstract>
			<OtherAbstract Language="FA">Internal polarizations field which take place in quantum structures of group-III nitrides have an important consequence on their optical properties. Optical properties of wurtzite AlGaN/GaN quantum well (QW) structures grown by MBE and MOCVD on c-plane sapphire substrates have been investigated by means of photoluminescence (PL) and time resolved photoluminescence (TRPL) at low-temperature. PL spectra exhibit a blue-shifted emission of AlGaN/GaN quantum well (QW) nanostructures by decreasing the barrier width contrary to the arsenide system. The trend of the barrier-width dependence of the internal polarization field is reproduced by using simple electrostatic arguments. In addition the effect of well width variation on the optical transition and decay time of GaN MQWs have been investigated and it has been shown that the screening of the piezoelectric field and the electron-hole separation are strongly dependent on the well thickness and have a profound effect on the optical properties of the GaN/AlGaN MQWs.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">GaN/AlGaN multiple quantum well (MQW)</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">photoluminescence (PL)</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">time resolved photoluminescence (TRPL)</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">polarization field</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">semiconductor nano-structure</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">piezoelectric field</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_574_f0e52b27a7a5d6a1a87373dffa53dbe5.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>7</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Hypercentral constituent quark model and the hyperfine dependence potential</ArticleTitle>
<VernacularTitle>Hypercentral constituent quark model and the hyperfine dependence potential</VernacularTitle>
			<FirstPage>127</FirstPage>
			<LastPage>127</LastPage>
			<ELocationID EIdType="pii">575</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>M. R.</FirstName>
					<LastName>Shojaei</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>A. A.</FirstName>
					<LastName>Rajabi</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 article nucleons are discussed based on constituent quark model. This model aims at studying the forces among three particles and the corresponding standard two-body potential contribution. The quark potential contains a hypercentral interaction. The confining potential is composed of four components,color charge, the oscillatory potential, the interaction quark and neutral gluon, and the dipole – dipole electromagnetic interaction. Dirac equation can be solved carefully and analytically by means of these potentials. In addition to the above potentials, there is a hyperfine potential which is related to isospin – isospin and spin –isopin interactions. These potentials were considered as perturbation potentials and their energy shift was calculated.</Abstract>
			<OtherAbstract Language="FA">  In this article nucleons are discussed based on constituent quark model. This model aims at studying the forces among three particles and the corresponding standard two-body potential contribution. The quark potential contains a hypercentral interaction. The confining potential is composed of four components,color charge, the oscillatory potential, the interaction quark and neutral gluon, and the dipole – dipole electromagnetic interaction. Dirac equation can be solved carefully and analytically by means of these potentials. In addition to the above potentials, there is a hyperfine potential which is related to isospin – isospin and spin –isopin interactions. These potentials were considered as perturbation potentials and their energy shift was calculated.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Dirac equation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">hypercentral</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Jacobian coordinate</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">hyperfine-isospin</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_575_ffeabd223de0d4eacb9a3e6e53e5448d.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>7</Volume>
				<Issue>2</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Quantum averaging and resonances: two-level atom in a one-mode classical laser field</ArticleTitle>
<VernacularTitle>Quantum averaging and resonances: two-level atom in a one-mode classical laser field</VernacularTitle>
			<FirstPage>128</FirstPage>
			<LastPage>128</LastPage>
			<ELocationID EIdType="pii">576</ELocationID>
			
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName></FirstName>
					<LastName>M. Amniat-Talab</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName></FirstName>
					<LastName>H. Sedghi</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName></FirstName>
					<LastName>R. Khoda-Bakhsh</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 use a nonperturbative method based on quantum averaging and an adapted from of resonant transformations to treat the resonances of the Hamiltonian of a two-level atom interacting with a one-mode classical field in Floquet formalism. We illustrate this method by extraction of effective Hamiltonians of the system in two regimes of weak and strong coupling. The results obtained in the strong-coupling regime, are valid in the whole range of the coupling constant for the one-photon zero-field resonance.</Abstract>
			<OtherAbstract Language="FA">  We use a nonperturbative method based on quantum averaging and an adapted from of resonant transformations to treat the resonances of the Hamiltonian of a two-level atom interacting with a one-mode classical field in Floquet formalism. We illustrate this method by extraction of effective Hamiltonians of the system in two regimes of weak and strong coupling. The results obtained in the strong-coupling regime, are valid in the whole range of the coupling constant for the one-photon zero-field resonance.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">quantum averaging</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">two-level atom</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Floquet formalism</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">resonant transformation</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">nonlinear resonance</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_576_a7aeed74714116f3b292a982238f83d2.pdf</ArchiveCopySource>
</Article>
</ArticleSet>
