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<Journal>
				<PublisherName>Shahid Rajaee Teacher Training University</PublisherName>
				<JournalTitle>Journal of Discrete Mathematics and Its Applications</JournalTitle>
				<Issn>2981-0809</Issn>
				<Volume>6</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2016</Year>
					<Month>06</Month>
					<Day>01</Day>
				</PubDate>
			</Journal>
<ArticleTitle>On the energy of fullerene graphs</ArticleTitle>
<VernacularTitle></VernacularTitle>
			<FirstPage>1</FirstPage>
			<LastPage>10</LastPage>
			<ELocationID EIdType="pii">499</ELocationID>
			
<ELocationID EIdType="doi">10.22061/jmns.2016.499</ELocationID>
			
			<Language>EN</Language>
<AuthorList>
<Author>
					<FirstName>Mahin</FirstName>
					<LastName>Songhori</LastName>
<Affiliation>Srtt University</Affiliation>

</Author>
<Author>
					<FirstName>Modjtaba</FirstName>
					<LastName>Ghorbani</LastName>
<Affiliation>Srtt University</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2016</Year>
					<Month>02</Month>
					<Day>11</Day>
				</PubDate>
			</History>
		<Abstract>The concept of energy of graph is defined as the sum of the absolute values of the eigenvalues of a graph. Let λ&lt;sub&gt;1&lt;/sub&gt;, λ&lt;sub&gt;2&lt;/sub&gt;, . . . , λ&lt;sub&gt;n &lt;/sub&gt;be eigenvalues of graph G, then the energy of G is defined as E (G) =∑&lt;sup&gt;n&lt;/sup&gt;&lt;sub&gt;n=1&lt;/sub&gt;|λ&lt;sub&gt;ه&lt;/sub&gt;|. The aim of this paper is to compute the eigenvalues of two fullerene graphs C&lt;sub&gt;60&lt;/sub&gt; and C&lt;sub&gt;80&lt;/sub&gt;.</Abstract>
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			<Param Name="value">fullerene</Param>
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			<Param Name="value">graph energy</Param>
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<Article>
<Journal>
				<PublisherName>Shahid Rajaee Teacher Training University</PublisherName>
				<JournalTitle>Journal of Discrete Mathematics and Its Applications</JournalTitle>
				<Issn>2981-0809</Issn>
				<Volume>6</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2016</Year>
					<Month>06</Month>
					<Day>01</Day>
				</PubDate>
			</Journal>
<ArticleTitle>A study on Landau levels in thin films</ArticleTitle>
<VernacularTitle></VernacularTitle>
			<FirstPage>11</FirstPage>
			<LastPage>16</LastPage>
			<ELocationID EIdType="pii">515</ELocationID>
			
<ELocationID EIdType="doi">10.22061/jmns.2016.515</ELocationID>
			
			<Language>EN</Language>
<AuthorList>
<Author>
					<FirstName>Fatemeh</FirstName>
					<LastName>Ahmadi</LastName>
<Affiliation>Department of Physics, Shahid Rajaee Teacher Training University</Affiliation>

</Author>
<Author>
					<FirstName>Mehdi</FirstName>
					<LastName>Saadat</LastName>
<Affiliation>Department of Physics, Shahid Rajaee Teacher Training University</Affiliation>

</Author>
<Author>
					<FirstName>Zainab</FirstName>
					<LastName>Bahrampori</LastName>
<Affiliation>Department of Physics, Shahid Rajaee Teacher Training University</Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2015</Year>
					<Month>09</Month>
					<Day>02</Day>
				</PubDate>
			</History>
		<Abstract>In this paper, we study the energy levels of an electron moving in a thin film. This film is considered as a two-dimensional electron gas which is under the influence of a uniform external magnetic field B and a uniform external electric field E. Here, the magnetic field is perpendicular to the film. Also, in this paper, we have selected the Landau gauge, because this gauge is useful for working in rectangular geometries.</Abstract>
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			<Param Name="value">energy levels</Param>
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			<Param Name="value">wavefunctions</Param>
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