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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>21</Volume>
				<Issue>3</Issue>
				<PubDate PubStatus="epublish">
					<Year>2021</Year>
					<Month>11</Month>
					<Day>22</Day>
				</PubDate>
			</Journal>
<ArticleTitle>‎   ‎Properties of  132Xe Neutral Atoms Scattering for 165K and 275K ‎Temperatures</ArticleTitle>
<VernacularTitle>‎   ‎Properties of  132Xe Neutral Atoms Scattering for 165K and 275K ‎Temperatures</VernacularTitle>
			<FirstPage>49</FirstPage>
			<LastPage>54</LastPage>
			<ELocationID EIdType="pii">1711</ELocationID>
			
<ELocationID EIdType="doi">10.47176/ijpr.21.3.38481&nbsp;</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>A</FirstName>
					<LastName>Akour</LastName>
<Affiliation>Department of Basic Science, Al-Huson College, Al-Balqa Applied University, Salt, Jordan</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2019</Year>
					<Month>07</Month>
					<Day>22</Day>
				</PubDate>
			</History>
		<Abstract>This work aims to use an important method Galitskii-Migdal-Feynman (GMF) for ‎diatomic molecules 132Xe2, to calculate the effective phase shifts which are then used to ‎compute the effective total and viscosity cross sections at low density and temperature . ‎this study has shown that it’s crucial to include partial waves up to ‎ ‎; for ‎ ‎, the ‎effect of the potential becomes negligible .‎&lt;br /&gt;‎ Comparing with partial waves cross sections we deduce that the cross section is ‎dominated by S-wave scattering for low energy (wave number k &lt; 0.1 Å-1), otherwise D ‎and G partial waves dominate . The highest peak rises from the partial effective D and G-‎wave resonance, where the system sustains a quasi-bound state trapped by the centrifugal barrier. The average cross section is also determined. ‎</Abstract>
			<OtherAbstract Language="FA">This work aims to use an important method Galitskii-Migdal-Feynman (GMF) for ‎diatomic molecules 132Xe2, to calculate the effective phase shifts which are then used to ‎compute the effective total and viscosity cross sections at low density and temperature . ‎this study has shown that it’s crucial to include partial waves up to ‎ ‎; for ‎ ‎, the ‎effect of the potential becomes negligible .‎&lt;br /&gt;‎ Comparing with partial waves cross sections we deduce that the cross section is ‎dominated by S-wave scattering for low energy (wave number k &lt; 0.1 Å-1), otherwise D ‎and G partial waves dominate . The highest peak rises from the partial effective D and G-‎wave resonance, where the system sustains a quasi-bound state trapped by the centrifugal barrier. The average cross section is also determined. ‎</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Effective Total Cross Section</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Effective Phase Shifts</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Effective Viscosity Cross Section</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Galitskii-Migdal-Feynman Formalism</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">132Xe Gas</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_1711_a941493eeea57ede8214fd77d41806bc.pdf</ArchiveCopySource>
</Article>
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