<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">APM</journal-id><journal-title-group><journal-title>Advances in Pure Mathematics</journal-title></journal-title-group><issn pub-type="epub">2160-0368</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/apm.2017.76021</article-id><article-id pub-id-type="publisher-id">APM-77056</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  The Energy and Operations of Graphs
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Haicheng</surname><given-names>Ma</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Xiaohua</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Mathematics, Qinghai Nationalities University, Xining, China</addr-line></aff><pub-date pub-type="epub"><day>09</day><month>06</month><year>2017</year></pub-date><volume>07</volume><issue>06</issue><fpage>345</fpage><lpage>351</lpage><history><date date-type="received"><day>25,</day>	<month>April</month>	<year>2017</year></date><date date-type="rev-recd"><day>18,</day>	<month>June</month>	<year>2017</year>	</date><date date-type="accepted"><day>21,</day>	<month>June</month>	<year>2017</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p><html>
 <head></head>
 
  Let 
  <em>G</em> be a finite and undirected simple graph on 
  <em>n </em>vertices, 
  <em>A(G)</em> is the adjacency matrix of 
  <em>G</em>, 
  λ<sub>1</sub>,λ<sub>2</sub>,...,λ<sub>n</sub> are eigenvalues of 
  <em style="white-space:normal;">A(G)</em>, then the energy of 
  <em>G</em> is 
  <img src="Edit_23a7ac86-a712-4abf-9c4d-7bfcc42d0dac.bmp" alt="" />. In this paper, we determine the energy of graphs obtained from a graph by other unary operations, or graphs obtained from two graphs by other binary operations. In terms of binary operation, we prove that the energy of product graphs 
  <img src="Edit_b73ec3b0-104a-4bd1-894e-d5f88c910ee4.bmp" alt="" /> is equal to the product of the energy of graphs 
  <em>G</em>
  <sub><em>1</em></sub> and 
  <em>G</em>
  <sub><em>2</em></sub>, and give the computational formulas of the energy of Corona graph 
  <img src="Edit_d3e12e54-d04d-492e-bcde-a1868f125e4c.bmp" alt="" />, join graph 
  <img src="Edit_9fa2df41-9ad0-42e7-8b66-545a06abcfca.bmp" alt="" />of two regular graphs 
  <em>G</em> and 
  <em>H</em>, respectively. In terms of unary operation, we give the computational formulas of the energy of the duplication graph 
  <em>D</em>
  <sub><em>m</em></sub>
  <em>G</em>, the line graph 
  <em>L(G)</em>, the subdivision graph 
  <em>S(G)</em>, and the total graph 
  <em>T(G)</em> of a regular graph 
  <em>G</em>, respectively. In particularly, we obtained a lot of graphs pair of equienergetic.
 
</html></p></abstract><kwd-group><kwd>Graph</kwd><kwd> Matrix</kwd><kwd> Energy</kwd><kwd> Operation</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Let G be a finite and undirected simple graph, with vertex set V ( G ) and edge set E ( G ) . The number of vertices of G is n, and its vertices are labeled by v 1 , v 2 , ⋯ , v n . The adjacency matrix A ( G ) of the graph G is a square matrix of order n, whose ( i , j ) -entry is equal to 1 if the vertices v i and v j are adjacent and is equal to zero otherwise. The characteristic polynomial of the adjacency matrix, i.e., d e t ( x I n − A ( G ) ) , where I n is the unit matrix of order n, is said to be the characteristic polynomial of the graph G and will be denoted by ϕ ( G , x ) . The eigenvalues of a graph G are defined as the eigenvalues of its adjacency matrix A ( G ) , and so they are just the roots of the equation ϕ ( G , x ) = 0 . since A ( G ) is a real symmetric matrix, so its eigenvalues are all real. Denoting them by λ 1 , λ 2 , ⋯ , λ n and as a whole, they are called the spectrum of G. Spectral pro- perties of graphs, including properties of the characteristic polynomial, have been extensively studied, for details, we refer to [<xref ref-type="bibr" rid="scirp.77056-ref1">1</xref>] . In the 1970s, I. Gutman in [<xref ref-type="bibr" rid="scirp.77056-ref2">2</xref>] introduced the concept of the energy of G by</p><p>ε ( G ) = ∑ i = 1 n | λ i | (1)</p><p>In the H&#252;ckel molecular orbital (HMO) theory, the energy approximates the the molecular orbital energy levels of π-electrons in conjugated hydrocarbons (see [<xref ref-type="bibr" rid="scirp.77056-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.77056-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.77056-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.77056-ref6">6</xref>] ). Up to now, the energy of G has been extensively studied, for details, we refer to [<xref ref-type="bibr" rid="scirp.77056-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.77056-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.77056-ref9">9</xref>] . In this paper, we determine the energy of graphs obtained from a graph by other unary operations, or graphs obtained from two graphs by other binary operations. In terms of binary operation, we prove that the energy of product graphs G 1 &#215; G 2 is equal to the product of the energy of graphs G 1 and G 2 , and give the computational formulas of the energy of Corona graph G ∘ H , join graph G ∇ H of two regular graphs G and H, respectively. In terms of unary operation, we give the computational formulas of the energy of the duplication graph D m G , the line graph L ( G ) , the sub- division graph S ( G ) , and the total graph T ( G ) of a regular graph G, re- spectively. In particularly, we obtained a lot of graphs pair of equienergetic.</p><p>Two nonisomorphic graphs are said to be equienergetic if they have the same energy. Let G and H be two vertex disjoint graphs, G ∪ H denotes the union graph of G and H. m G denoted the union graph of m copies of G. K n denotes the complete graph with n vertices. For more notation and terminology, we refer the readers to standard textbooks [<xref ref-type="bibr" rid="scirp.77056-ref10">10</xref>] .</p></sec><sec id="s2"><title>2. The Binary Operations of Graphs</title><p>Let G 1 and G 2 be two graphs with vertex set V ( G 1 ) and V ( G 2 ) respec- tively. the product G 1 &#215; G 2 is the graph with vertex set V ( G 1 ) &#215; V ( G 2 ) , in which two vertices, say ( x 1 , y 1 ) and ( x 2 , y 2 ) , are adjacent if and only if x 1 is adjacent to x 2 in G 1 and y 1 is adjacent to y 2 in G 2 . Let A = ( a i j ) m &#215; n , B = ( b i j ) p &#215; q be two matrices, the Kronecker product A ⊗ B of A and B is the m p &#215; n q matrix obtained from A by replacing each element a i j with the block a i j B .</p><p>Lemma 2.1. [<xref ref-type="bibr" rid="scirp.77056-ref1">1</xref>] Let A ( G 1 ) , A ( G 2 ) be adjacency matrices of graphs G 1 , G 2 , respectively. Then the product graph G 1 &#215; G 2 has as adjacency matrix A ( G 1 ) ⊗ A ( G 2 ) .</p><p>Lemma 2.2. [<xref ref-type="bibr" rid="scirp.77056-ref11">11</xref>] Let A, B, C, D be matrices and the products AC, BD exist. Then</p><p>( A ⊗ B ) ( C ⊗ D ) = ( A C ) ⊗ ( B D ) . (2)</p><p>Theorem 2.1. Let G, H be two graphs. Then</p><p>ε ( G &#215; H ) = ε ( G ) &#215; ε ( H ) . (3)</p><p>Proof. Let λ 1 , λ 2 , ⋯ , λ n and μ 1 , μ 2 , ⋯ , μ m be the eigenvalues of G and H, respectively, suppose x i ( i = 1 , 2 , ⋯ , n ) are linearly independent eigenvectors of A ( G ) corresponding to λ 1 , λ 2 , ⋯ , λ n respectively, and y i ( i = 1 , 2 , ⋯ , m ) are linearly independent eigenvectors of A ( H ) corresponding to μ 1 , μ 2 , ⋯ , μ m respectively, Consider the vector z i j = x i ⊗ y j ( i = 1 , 2 , ⋯ , n , j = 1 , 2 , ⋯ , m ) . Using Lemma 2.1, we see that</p><p>( A ( G ) ⊗ A ( H ) ) z i j = ( A ( G ) x i ) ⊗ ( A ( H ) y j ) = λ i μ j x i ⊗ y j = λ i μ j z i j .</p><p>In this way ,we find m n linearly independent eigenvectors, and hence λ i μ j ( i = 1 , 2 , ⋯ , n , j = 1 , 2 , ⋯ , m ) are the eigenvalues of G &#215; H .</p><p>And so</p><p>ε ( G &#215; H ) = ∑ i = 1 n ∑ j = 1 m | λ i μ j | = ∑ i = 1 n | λ i | ∑ j = 1 m | μ j | = ε ( G ) ε ( H ) .</p><p>,</p><p>Corollary 2.1. Let G 1 , G 2 , ⋯ , G k be k graphs. Then</p><p>ε ( G 1 &#215; G 2 &#215; ⋯ &#215; G k ) = ε ( G 1 ) ε ( G 2 ) ⋯ ε ( G k ) . (4)</p><p>Let G be a graph with n vertices, and let H be a graph with m vertices. The Corona G ∘ H is the graph with n + m n vertices obtained from G and n copies of H by joining the i-th vertex of G to each vertex in i-th copy of H ( i = 1 , 2 , ⋯ , n ) .</p><p>Lemma 2.3. [<xref ref-type="bibr" rid="scirp.77056-ref1">1</xref>] Let G be a graph with n vertices, and let H be an r-regular graph with m vertices. Then the characteristic polynomial of the corona G ∘ H is given by</p><p>ϕ ( G ∘ H , x ) = ϕ ( G , x − m x − r ) ( ϕ ( H , x ) ) n . (5)</p><p>Theorem 2.2. Let G be a graph with n vertices, and let H be an r-regular graph with m vertices. If λ 1 , λ 2 , ⋯ , λ n and r , μ 2 , ⋯ , μ m be the eigenvalues of G and H, respectively. then</p><p>ε ( G ∘ H ) = 1 2 ∑ i = 1 n ( | r + λ i + ( r − λ i ) 2 + 4 m | + | r + λ i − ( r − λ i ) 2 + 4 m | ) + n ( ε ( H ) − r ) . (6)</p><p>Proof. By Lemma 2.3, we have</p><p>ϕ ( G ∘ H , x ) = ( x − r ) n ( x − μ 2 ) n ⋯ ( x − μ m ) n ∏ i = 1 n ( x − m x − r − λ i ) = ( x − μ 2 ) n ⋯ ( x − μ m ) n ∏ i = 1 n ( x 2 − ( r + λ i ) x + r λ i − m ) .</p><p>And so</p><p>ε ( G ∘ H ) = 1 2 ∑ i = 1 n ( | r + λ i + ( r − λ i ) 2 + 4 m | + | r + λ i − ( r − λ i ) 2 + 4 m | ) + n ( ∑ j = 2 m | μ j | ) = 1 2 ∑ i = 1 n ( | r + λ i + ( r − λ i ) 2 + 4 m | + | r + λ i − ( r − λ i ) 2 + 4 m | ) + n ( ε ( H ) − r ) .</p><p>,</p><p>Corollary 2.2. Let H 1 and H 2 be two equienergetic r-regular graph with m vertices, and let G be a graph with n vertices. Then G ∘ H 1 and G ∘ H 2 are equienergetic.</p><p>Corollary 2.3. Let m ≥ 2, n ≥ 3 . Then ε ( K n ∘ K m ) = m n + m − 2 + ( n − 1 ) m 2 + 4 m .</p><p>Proof. K m has spectrum n − 1, − 1 ( n − 1 times). Since</p><p>( m − 1 ) − 1 − ( m − 1 + 1 ) 2 + 4 m ≤ 0 , and m ≥ 2, n ≥ 3 means</p><p>( m − 1 ) + ( n − 1 ) − ( m − n ) 2 + 4 m ≥ 0 . Hence</p><p>ε ( K n ∘ K m ) = 1 2 ∑ i = 1 n ( | ( m − 1 ) + λ i + ( m − 1 − λ i ) 2 + 4 m |     + | m − 1 + λ i − ( m − 1 − λ i ) 2 + 4 m | ) + n ( ε ( H ) − ( m − 1 ) ) = m + n − 2 + ( n − 1 ) m 2 + 4 m + n ( m − 1 ) = m n + m − 2 + ( n − 1 ) m 2 + 4 m .</p><p>Let G and H be two graphs, The join G ∇ H of (disjoint) grapgs G and H is the graph obtained from G ∪ H by joining each vertex of G to each vertex of H.</p><p>Lemma 2.4. [<xref ref-type="bibr" rid="scirp.77056-ref1">1</xref>] If G 1 is r 1 -regular with n 1 vertices, and G 2 is r 2 - regular with n 2 vertices, then the characteristic polynomial of the join G 1 ∇ G 2 is given by</p><p>ϕ ( G 1 ∇ G 2 , x ) = ϕ ( G 1 , x ) ϕ ( G 2 , x ) ( x − r 1 ) ( x − r 2 ) ( ( x − r 1 ) ( x − r 2 ) − n 1 n 2 ) . (7)</p><p>Corollary 2.4. Let G i be r i -regular graph with n i vertices, i = 1 , 2. Then</p><p>ε ( G 1 ∇ G 2 ) = ε ( G 1 ) + ε ( G 2 ) − ( r 1 + r 2 ) + ( r 1 + r 2 ) 2 + 4 ( n 1 n 2 − r 1 r 2 ) . (8)</p><p>Corollary 2.5. Let G 1 and H 1 be two equienergetic r 1 -regular graph with n 1 vertices, and let G 2 and H 2 be two equienergetic r 2 -regular graph with n 2 vertices, then G 1 ∇ G 2 and H 1 ∇ H 2 are equienergetic.</p><p>Lemma 2.5. [<xref ref-type="bibr" rid="scirp.77056-ref1">1</xref>] Let G 1 , G 2 , ⋯ , G k be regular graphs, let G i have degree r i and n i vertices ( i = 1 , 2 , ⋯ , k ) . where the relations</p><p>n 1 − r 1 = n 2 − r 2 = ⋯ = n k − r k = s hold. Then the graph G = G 1 ∇ G 2 ∇ ⋯ ∇ G k has n = n 1 + n 2 + ⋯ + n k vertices and is regular of degree r = n − s , the charac- teristic polynomial of the join G is given by</p><p>ϕ ( G , x ) = ( x − r ) ( x + n − r ) k − 1 ∏ i = 1 k ϕ ( G i , x ) x − r i . (9)</p><p>By Lemma 2.5, we have following Corollary.</p><p>Corollary 2.6. Let G 1 , G 2 , ⋯ , G k be regular graphs, let G i have degree r i and n i vertices ( i = 1 , 2 , ⋯ , k ) . where the relations n 1 − r 1 = n 2 − r 2 = ⋯ = n k − r k = s hold. Then</p><p>ε ( G 1 ∇ G 2 ∇ ⋯ ∇ G k ) = 2 ( k − 1 ) s + ∑ i = 1 k     ε ( G i ) . (10)</p></sec><sec id="s3"><title>3. The Unary Operations of Graphs</title><p>Let G be a graph with vertex set V ( G ) = { v 1 , v 2 , ⋯ , v n } , the duplication graph D m G is the graph with m n vertices obtained from m G by joining v i to each neighbors of v i in the j-th copy of G ( j = 1 , 2 , ⋯ , m , i = 1 , 2 , ⋯ , n ) .</p><p>Theorem 3.1. Let G be a graph. Then</p><p>ε ( D m G ) = m ε ( G ) . (11)</p><p>Proof. If A ( G ) is the adjacency matrix of graph G, then, it is obviously that the adjacency matrix of the duplication graph D m G is J m ⊗ A ( G ) , where J m is all 1 matrix of order m. the spectrum of J m is m ,0 ( m − 1 ) times, similar to the proof of Theorem 2.1, we have ε ( D m G ) = m ε ( G ) .</p><p>Corollary 3.1. Let G and H be two equienergetic graph, then D m G and D m H are equienergetic.</p><p>Let G be a graph, the line graph L ( G ) of graph G is the graph whose vertices are the edges of G, with two vertices in L ( G ) adjacent whenever the corre- sponding edge in G have exactly one vertex in common.</p><p>Lemma 3.1 [<xref ref-type="bibr" rid="scirp.77056-ref1">1</xref>] If G is a regular graph of degree r, with n vertices and</p><p>m ( = 1 2 n r ) edges, then</p><p>ϕ ( L ( G ) , x ) = ( x + 2 ) m − n ϕ ( G , x − r + 2 ) . (12)</p><p>Corollary 3.2. Let G be a regular graph of degree r, with n vertices and</p><p>m ( = 1 2 n r ) edges, If λ 1 ( = r ) , λ 2 , ⋯ , λ n is the eigenvalues of G, then</p><p>ε ( L ( G ) ) = 2 ( m − n ) + ∑ i = 1 n | r + λ i − 2 | . (13)</p><p>Corollary 3.3.</p><p>ε ( L ( K n ) ) = { 2 n 2 − 6 n 4 ≤ n ,   4 ( n − 2 ) 2 ≤ n ≤ 3. (14)</p><p>Let G be a graph, the subdivision graph S ( G ) of graph G is the graph obtained by inserting a new vertex into every edge of G. The graph R ( G ) of graph G is the graph obtained from G by adding, for each edge uv, a new vertex whose neighbours are u and v. The graph Q ( G ) of graph G is the graph obtained from G by inserting a new vertex into every edge of G, and joining by edges those pairs of new vertices which lie on adjacent edges of G. The total graph T ( G ) of graph G is the graph whose vertices are the vertices and edges of G, with two vertices of T ( G ) adjacent if and only if the corresponding element of G are adjacent or incident.</p><p>Lemma 3.2. [<xref ref-type="bibr" rid="scirp.77056-ref1">1</xref>] If G is a regular graph of degree r, with n vertices and</p><p>m ( = 1 2 n r ) edges, then</p><p>1) ϕ ( S ( G ) , x ) = x m − n ϕ ( G , x 2 − r ) ,</p><p>2) ϕ ( R ( G ) , x ) = x m − n ( x + 1 ) n ϕ ( G , x 2 − r x + 1 ) ,</p><p>3) ϕ ( Q ( G ) , x ) = ( x + 2 ) m − n ( x + 1 ) n ϕ ( G , x 2 − ( r − 2 ) x − r x + 1 ) .</p><p>4) The total graph T ( G ) has m − n eigenvalues equal to −2 and the following 2n eigenvalues:</p><p>1 2 ( 2 λ i + r − 2 &#177; 4 λ i + r 2 + 4 ) ,     ( i = 1 , 2 , ⋯ , n ) .</p><p>Theorem 3.2. Let G be a regular graph of degree r, with n vertices and</p><p>m ( = 1 2 n r ) edges, If λ 1 ( = r ) , λ 2 , ⋯ , λ n is the eigenvalues of G, then</p><p>1) ε ( S ( G ) ) = 2 ∑ i = 1 n r + λ i ,</p><p>2) ε ( R ( G ) ) = ∑ i = 1 n λ i 2 + 4 ( r + λ i ) ,</p><p>3) ε ( Q ( G ) ) = 2 ( m − n ) + ∑ i = 1 n ( r + λ i ) 2 + 4 ,</p><p>4) ε ( T ( G ) ) = 2 ( m − n ) + 1 2 ∑ i = 1 n ( | 2 λ i + r − 2 + 4 λ i + r 2 + 4 |     + | 2 λ i + r − 2 − 4 λ i + r 2 + 4 | ) .</p><p>Proof. (1) By Lemma 3.2 (1), we know that the spectrum of S ( G ) is { 0 ( m − n   times ) , &#177; r + λ i ( i = 1 , 2 , ⋯ , n ) } . So ε ( S ( G ) ) = 2 ∑ i = 1 n r + λ i .</p><p>(2) By Lemma 3.2 (2), we know that the spectrum of R ( G ) is</p><p>{ 0 ( m − n   times ) , λ i &#177; λ i 2 + 4 ( r + λ i ) 2 ( i = 1 , 2 , ⋯ , n ) } . So ε ( R ( G ) ) = ∑ i = 1 n λ i 2 + 4 ( r + λ i ) .</p><p>(3), (4) Proof is similar to (1).</p><p>Corollary 3.4. 1) If n ≥ 2, then ε ( S ( K n ) ) = 2 ( 2 n − 2 + ( n − 1 ) n − 2 ) .</p><p>2) If n ≥ 2, then ε ( R ( K n ) ) = n 2 + 6 n − 7 + ( n − 1 ) 4 n − 7 .</p><p>3) ε ( Q ( K n ) ) = n 2 − 3 n + 2 n 2 − 2 n + 2 + ( n − 1 ) n 2 − 4 n + 8 .</p><p>4) If n ≥ 2, then ε ( T ( K n ) ) = { 2 n 2 − 2 n − 4 n ≥ 3 , 4 n = 2.</p></sec><sec id="s4"><title>4. Conclusion</title><p>In this paper, we prove that ε ( G &#215; H ) = ε ( G ) &#215; ε ( H ) , ε ( D m G ) = m ε ( G ) . For regular graphs G and H, we give the computational formulas of ε ( G ∇ H ) , ε ( G ∘ H ) , ε ( L ( G ) ) , ε ( S ( G ) ) , ε ( R ( G ) ) , ε ( Q ( G ) ) , and ε ( T ( G ) ) re- spectively. In particularly, we obtained a lot of graphs pair of equienergetic.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This work is supported by National Natural Science Foundation of China (11561056, 11661066), National Natural Science Foundation of Qinghai Provence (2016-ZJ-914), and Scientific Research Fund of Qinghai University for Nationalities (2015G02).</p></sec><sec id="s6"><title>Cite this paper</title><p>Ma, H.C. and Liu, X.H. (2017) The Energy and Operations of Graphs. Advances in Pure Mathematics, 7, 345-351. https://doi.org/10.4236/apm.2017.76021</p></sec></body><back><ref-list><title>References</title><ref id="scirp.77056-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Cvetkovi&amp;cacute;, D., Rowlinson, P. and Simi&amp;cacute;, S. (2010) An Introduction to the Theory of Graph Spectra. 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