Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 2740 https://internationalpubls.com Bounds for Product Eccentricity Energy of Graphs Priya Karen S1,a), Arokia Lancy A2,b) 1,2 PG and Research Department of Mathematics, Nirmala College for Women, Coimbatore, Tamilnadu, India a) Corresponding author: priyakaren2018@gmail.com b)aarokia.lancy@gmail.com Article History: Received: 12-01-2025 Revised: 15-02-2025 Accepted: 01-03-2025 Abstract: In this article some lower bounds for the product eccentricity energy [𝐸𝑃𝐸] of 𝐺 as well as a bound for the eigenvalues of the product eccentricity matrix [𝑃𝐸(𝐺)] are obtained. Mathematical Subject Classification :05C07, 050C50. Conclusion: This article gives an idea on few lower bounds for the product eccentricity energy based on its eigen values and various inequalities are also proved. Keywords: Energy, bounds, Product eccentricity energy. 1. Introduction Graph theory is a branch of discrete arithmetic that involves considering structures together with their attributes, goals, and relationships. Originally useful for resolving a wide range of mathematical problems, it periodically branched out into new areas of mathematical analysis when applied in complicated science, computer science, chemistry, and other disciplines. Simple, loop-less, and connected graphs are the types of graphs examined in this article. An essential concept in this theory is a vertex's eccentricity, which assesses the greatest distance between two vertices. The distance between two vertices π‘Ž and 𝑏 in 𝑉(𝐺) is the shortest a-b path length in 𝐺. The maximum distance between a particular vertex and any other vertex in the graph is determined by the vertex's eccentricity. Formally, it can be expressed as: πœ‰(𝑏) = max{𝑑(𝑏, π‘Ž)|βˆ€ π‘Ž ∈ 𝑉(𝐺)} A graph G's eccentricity matrix πœ‰(𝐺) is derived from its distance matrix by keeping the largest distances in each row and column and leaving zeros in the others. Summing the absolute values of the eigenvalues of πœ‰(𝐺) yields the eccentricity energy of 𝐺. Let 𝐺 be a graph with 𝑛 vertices and π‘š edges. Denote the absolute eigen values of 𝐺 as πœ†π‘– , 𝑖 = 1,2, β‹― 𝑛 arranged in order that is not increasing as |πœ†1| β‰₯ |πœ†2| β‰₯ β‹― β‰₯ |πœ†π‘›|. In 1978 Ivan Gutman [5] computed the energy of a graph 𝐺 as 𝐸(𝐺) = βˆ‘ |πœ†π‘–|𝑛 𝑖=1 . Li.X, Y. Shi and I. Gutman [6] introduced the energy of graph in 2012 in which the adjacency matrix of a graph 𝐺is defined as π‘Žπ‘–π‘— = { 1 𝑖𝑓 𝑣𝑖𝑣𝑗 ∈ 𝐸 0 π‘œπ‘‘β„Žπ‘’π‘Ÿπ‘€π‘–π‘ π‘’ Spectrum of the graph is denoted by 𝑆𝑝(𝐺) = [ πœ†1 πœ†2 β‹― πœ†π‘› π‘š1 π‘š2 β‹― π‘šπ‘› ] mailto:priyakaren2018@gmail.com mailto:aarokia.lancy@gmail.com Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 2741 https://internationalpubls.com Where π‘šπ‘– ′𝑠 denote the multiplicities of the corresponding eigen value. The total of the absolute values of the adjacency matrix's eigenvalues equals the graph's energy. Later, in 2009, C. Adiga et al. [1] defined the graph's maximum degree energy, which is dependent on the related graph's maximum degree matrix. The maximum degree matrix is defined as 𝑑𝑖𝑗 = { π‘šπ‘Žπ‘₯ {𝑑(𝑣𝑖), 𝑑(𝑣𝑗 )} , 𝑖𝑓 𝑣𝑖𝑣𝑗 ∈ 𝐸 0, π‘œπ‘‘β„Žπ‘’π‘Ÿπ‘€π‘–π‘ π‘’ In 2016, Ahmed M. Naji et.al [2] defined the concept of maximum eccentricity matrix. Later, Mohammad Issa Sowaity and B.Sharada [7] in 2017 introduced the concept of sum-eccentricity energy of a graph in 2017. Motivated by this we have introduced the product eccentricity energy of a graph 𝐺. In 2025 Priya Karen S and Arokia Lancy A [10] defined the idea of product eccentricity energy as 𝑃𝑖𝑗 = {𝑒(𝑣𝑖). 𝑒(𝑣𝑗) 𝑖𝑓 𝑣𝑖~ 𝑣𝑗 0 π‘œπ‘‘β„Žπ‘’π‘Ÿπ‘€π‘–π‘ π‘’ 𝑃𝑒(𝐺) denotes the product eccentricity energy of the graph. The characteristic polynomial of the product eccentricity matrix is defined by |πœ‚ 𝐼 βˆ’ 𝑃𝑒(𝐺)| and the corresponding characteristic equation is πœ‚πΌ βˆ’ 𝑃𝑒(𝐺) = 0. Here, 𝐼 denotes the identity matrix of order 𝑛. 𝑃𝑒(𝐺) is a real symmetric matrix with its trace zero. Since 𝐺 is a simple loopless graph all π‘Žπ‘–π‘– = 0 and its eigen values with real sum equals zero (π‘‘π‘Ÿ(𝑃𝑒(𝐺) = 0). Eigen values of the product eccentricity matrix are the roots of the corresponding characteristic polynomial. 𝐸𝑃𝐸(𝐺) is defined as the sum of the absolute eigen values, 𝐸𝑃𝐸(𝐺) = βˆ‘ |πœ‚π‘–| 𝑛 𝑖=1 πœ‚1, πœ‚2, β‹― πœ‚π‘› are the eigen values of the given product eccentricity matrix. 2. Preliminaries A few important theorems that are utilized throughout the work are listed below in order to show the complete results. Theorem 2.1:[9] Suppose π‘Žπ‘– and 𝑏𝑖, 1 ≀ 𝑖 ≀ 𝑛 are non-negative real numbers, then βˆ‘ π‘Žπ‘– 2 𝑛 𝑖=1 βˆ‘ 𝑏𝑖 2 𝑛 𝑖=1 ≀ 1 4 (√ 𝑀1𝑀2 π‘š1π‘š2 + √ π‘š1π‘š2 𝑀1𝑀2 ) 2 (βˆ‘ π‘Žπ‘–π‘π‘– 𝑛 𝑖=1 ) 2 Where 𝑀1 = max 1≀i≀n (π‘Žπ‘–) ; 𝑀2 = max 1≀i≀n (𝑏𝑖) ; π‘š1 = max 1≀i≀n (π‘Žπ‘–) ; π‘š2 = max 1≀i≀n (𝑏𝑖) Theorem 2.2:[8] Let π‘Žπ‘– and 𝑏𝑖, 1 ≀ 𝑖 ≀ 𝑛 are non-negative real numbers, then Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 2742 https://internationalpubls.com βˆ‘ π‘Žπ‘– 2 𝑛 𝑖=1 βˆ‘ 𝑏𝑖 2 𝑛 𝑖=1 βˆ’ (βˆ‘ π‘Žπ‘–π‘π‘– 𝑛 𝑖=1 ) 2 ≀ 𝑛2 4 (𝑀1𝑀2 βˆ’ π‘š1π‘š2)2 Where 𝑀1𝑀2 and π‘š1π‘š2 are defined similarly to theorem 2.1 Theorem 2.3:[3] Suppose π‘Žπ‘– and 𝑏𝑖, 1 ≀ 𝑖 ≀ 𝑛 are positive real numbers, then |𝑛 βˆ‘ π‘Žπ‘– 𝑏𝑖 𝑛 𝑖=1 βˆ’ βˆ‘ π‘Žπ‘– 𝑛 𝑖=1 βˆ‘ 𝑏𝑖 𝑛 𝑖=1 | ≀ πœ‡(𝑛)(𝐴 βˆ’ π‘Ž)(𝐡 βˆ’ 𝑏) Here π‘Ž, 𝑏, 𝐴 and 𝐡 are the real constants, 1 ≀ 𝑖 ≀ 𝑛, π‘Ž ≀ π‘Žπ‘– ≀ 𝐴 and 𝑏 ≀ 𝑏𝑖 ≀ 𝐡. Further we have , πœ‡(𝑛) = 𝑛 ⌊ 𝑛 2 βŒ‹ (1 βˆ’ 1 𝑛 ⌊ 𝑛 2 βŒ‹) Theorem 2.4:[4] Let π‘Žπ‘– and 𝑏𝑖, 1 ≀ 𝑖 ≀ 𝑛 are non-negative real numbers, then βˆ‘ 𝑏𝑖 2 𝑛 𝑖=1 + π‘Ÿπ‘… βˆ‘ π‘Žπ‘– 2 𝑛 𝑖=1 ≀ (π‘Ÿ + 𝑅) (βˆ‘ π‘Žπ‘–π‘π‘– 𝑛 𝑖=1 ) Here π‘Ÿ and 𝑅 are real constants, 1 ≀ 𝑖 ≀ 𝑛 holds π‘Ÿπ‘Žπ‘– ≀ 𝑏𝑖 ≀ π‘…π‘Žπ‘– 3.Bounds for the eigen values of Product Eccentricity Matrix of a graph The following lemma is required to support the subsequent findings. Lemma 3.1. If the trace of 𝑃𝐸(𝐺) = 0, then the eigen values obtained from 𝑃𝐸(𝐺) matrix satisfies the following 3. βˆ‘ πœ‚π‘– = 0𝑛 𝑖=1 4. βˆ‘ πœ‚π‘– 2𝑛 𝑖=1 = π‘‘π‘Ÿπ‘Žπ‘π‘’ (𝑃𝐸(𝐺)) 2 βˆ‘ πœ‚π‘– 2 𝑛 𝑖=1 = βˆ‘(πœ‚π‘–)2 𝑛 𝑖=1 = (π‘‘π‘Ÿπ‘Žπ‘π‘’(𝑃𝑒(𝐺))) 2 = βˆ‘ βˆ‘ π‘π‘–π‘˜π‘π‘˜π‘– 𝑛 π‘˜=1 𝑛 𝑖=1 = 2 βˆ‘ βˆ‘(π‘π‘–π‘˜)2 𝑛 𝑖<π‘˜ 𝑛 𝑖=1 = 2 βˆ‘ (𝑒(𝑣𝑖). 𝑒(𝑣𝑗)) 2 𝑛 𝑖=1,𝑖<π‘˜ βˆ‘(πœ‚π‘–)2 = 2 𝐻 𝑛 𝑖=1 Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 2743 https://internationalpubls.com Where 𝐻 = βˆ‘ (𝑒(𝑣𝑖). 𝑒(𝑣𝑗)) 2 𝑛 𝑖=1,𝑖<π‘˜ Theorem 3.2 Let 𝐺 be a graph with 𝑛 βˆ’ vertices, then πœ‚π‘– ≀ √ 2𝐻(𝑛 βˆ’ 1) 𝑛 Proof. Consider a graph 𝐺 with 𝑛 βˆ’vertices. Let 𝑃𝐸(𝐺) be the product eccentricity matrix of graph 𝐺 and πœ‚1, πœ‚2, β‹― πœ‚π‘› are the eigen values obtained from the 𝑃𝐸(𝐺) matrix, where πœ‚1 is the largest eigen value among all the eigen values computed and using the Cauchy-Schwarz inequality is used to obtain the bound for πœ‚1. (βˆ‘ π‘Žπ‘–π‘π‘– 𝑛 𝑖=1 ) 2 ≀ (βˆ‘ π‘Žπ‘– 2 𝑛 𝑖=1 ) (βˆ‘ 𝑏𝑖 2 𝑛 𝑖=1 ) Let π‘Žπ‘– = 1 and 𝑏𝑖 = πœ‚π‘– βˆ€ 𝑖 = 1,2,3, β‹― 𝑛 then the inequality becomes, (βˆ‘ 1. πœ‚π‘– 𝑛 𝑖=1 ) 2 ≀ (βˆ‘ 12 𝑛 𝑖=1 ) (βˆ‘ πœ‚π‘– 2 𝑛 𝑖=1 ) Using the idea of lemma 3.1 (i) βˆ‘ πœ‚π‘– 𝑛 𝑖=1 = 0 πœ‚1 + βˆ‘ πœ‚π‘– 𝑛 𝑖=2 = 0 βˆ‘ πœ‚π‘– 𝑛 𝑖=2 = βˆ’πœ‚1 On squaring we obtain (βˆ‘ πœ‚π‘– 𝑛 𝑖=2 ) 2 = (βˆ’πœ‚1)2 = πœ‚1 2 By (ii) of Lemma 3.1 (βˆ‘ πœ‚π‘– 𝑛 𝑖=2 ) 2 = 2𝐻 (πœ‚1)2 + (βˆ‘ πœ‚π‘– 𝑛 𝑖=2 ) 2 = 2𝐻 Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 2744 https://internationalpubls.com (βˆ‘ πœ‚π‘– 𝑛 𝑖=2 ) 2 = 2𝐻 βˆ’ (πœ‚1)2 Equation one becomes (βˆ’πœ‚1)2 ≀ (𝑛 βˆ’ 1)(2𝐻 βˆ’ πœ‚1 2) πœ‚1 2 ≀ 2𝐻 (𝑛 βˆ’ 1) βˆ’ πœ‚1 2(𝑛 βˆ’ 1) πœ‚1 2 + πœ‚1 2(𝑛 βˆ’ 1) ≀ 2𝐻(𝑛 βˆ’ 1) πœ‚1 2(𝑛) ≀ 2𝐻(𝑛 βˆ’ 1) πœ‚1 ≀ √ 2𝐻(𝑛 βˆ’ 1) 𝑛 Theorem 3.3 If 𝐺be a graph with 𝑛 βˆ’vertices then √2𝐻 ≀ 𝐸𝑃𝐸(𝐺) ≀ √2𝑛𝐻 Proof. Consider a graph 𝐺 with 𝑛 βˆ’vertices. Let 𝑃𝐸(𝐺) be the product eccentricity matrix of a graph 𝐺 and πœ‚1, πœ‚2, β‹― πœ‚π‘› are the eigen values obtained from the 𝑃𝐸(𝐺) matrix. By the idea of Cauchy- Schwartz inequality the theorem is proved (βˆ‘ π‘Žπ‘–π‘π‘– 𝑛 𝑖=1 ) 2 ≀ (βˆ‘ π‘Žπ‘– 2 𝑛 𝑖=1 ) (βˆ‘ 𝑏𝑖 2 𝑛 𝑖=1 ) Let us assume that π‘Žπ‘– = 1 and 𝑏𝑖 = πœ‚π‘– βˆ€ 𝑖 = 1,2,3, β‹― 𝑛. (βˆ‘ 1. πœ‚π‘– 𝑛 𝑖=1 ) 2 ≀ (βˆ‘ 12 𝑛 𝑖=1 ) (βˆ‘ πœ‚π‘– 2 𝑛 𝑖=1 ) (βˆ‘ πœ‚π‘– 𝑛 𝑖=1 ) 2 ≀ 𝑛 (βˆ‘ πœ‚π‘– 2 𝑛 𝑖=1 ) (𝐸𝑃𝐸(𝐺)) 2 ≀ 2𝑛𝐻 𝐸𝑃𝐸(𝐺) ≀ √2𝑛𝐻 This is an upper bound, We have, (𝐸𝑃𝐸(𝐺)) 2 = (βˆ‘ |πœ‚π‘–|𝑛 𝑖=1 )2 β‰₯ βˆ‘ |πœ‚π‘–|2 = 2 𝐻𝑛 𝑖=1 . Thus, we obtain 𝐸𝑃𝐸(𝐺) β‰₯ √2𝐻 which is the lower bound. Hence the inequality holds. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 2745 https://internationalpubls.com Thus we have, √2𝐻 ≀ 𝐸𝑃𝐸(𝐺) ≀ √2𝑛𝐻 Theorem 4.4: Let 𝐺 be a graph with 𝑛 βˆ’vertices and π‘š βˆ’ edges. If |πœ‚1| β‰₯ |πœ‚2| β‰₯ β‹― β‰₯ |πœ‚π‘›| are the eigen values of 𝑃𝐸(𝐺), then the following inequality holds. 𝐸𝑃𝐸(𝐺) β‰₯ 2 √2𝑛𝐻|πœ‚1||πœ‚π‘›| |πœ‚1| + πœ‚π‘›| Proof. Consider a graph 𝐺 with 𝑛 βˆ’vertices and |πœ‚1| β‰₯ |πœ‚2| β‰₯ β‹― β‰₯ |πœ‚π‘›| are the eigen values of 𝑃𝐸(𝐺), where |πœ‚1| and |πœ‚π‘›| are the maximum and minimum eigen values of |πœ‚π‘–| respectively. From theorem 2.1 βˆ‘ π‘Žπ‘– 2 𝑛 𝑖=1 βˆ‘ 𝑏𝑖 2 𝑛 𝑖=1 ≀ 1 4 (√ 𝑀1𝑀2 π‘š1π‘š2 + √ π‘š1π‘š2 𝑀1𝑀2 ) 2 (βˆ‘ π‘Žπ‘–π‘π‘– 𝑛 𝑖=1 ) 2 Assume π‘Žπ‘– = 1 and 𝑏𝑖 = |πœ‚π‘–|, 𝑀1𝑀2 = |πœ‚1| and π‘š1π‘š2 = |𝛼𝑛| then, βˆ‘ 12 𝑛 𝑖=1 βˆ‘|πœ‚π‘–|2 𝑛 𝑖=1 ≀ 1 4 (√ |πœ‚1| |πœ‚π‘›| + √ |πœ‚π‘›| |πœ‚1| ) 2 (βˆ‘ 1 |πœ‚π‘–| 𝑛 𝑖=1 ) 2 From lemma 3.1 and using the idea of Arithmetic-Geometric inequality we obtain, 2𝑛𝐻 ≀ 1 4 [ (|πœ‚1| + |πœ‚π‘›|)2 |πœ‚1||πœ‚π‘›| ] (𝐸𝑃𝐸(𝐺)) 2 (𝐸𝑃𝐸(𝐺)) 2 β‰₯ 8𝑛𝐻 |πœ‚1||πœ‚π‘›| (|πœ‚1| + |πœ‚π‘›|)2 (𝐸𝑃𝐸(𝐺)) 2 β‰₯ 2√2𝑛𝐻|πœ‚1||πœ‚π‘›| |πœ‚1| + |πœ‚π‘›| Theorem 3.5 Let 𝐺 be a graph with 𝑛 βˆ’vertices, then the following inequalities holds 𝐸𝑃𝐸(𝐺) β‰₯ 2𝐻_𝑛|πœ‚1||πœ‚π‘›| |πœ‚1| + |πœ‚π‘›| Proof. Consider a graph 𝐺 with order 𝑛 and size π‘š. Let |πœ‚1| β‰₯ |πœ‚2| β‰₯ β‹― β‰₯ |πœ‚π‘›| be the eigen balues of the product eccentricity matrix, arranged in non- increasing order, where |πœ‚1| and |πœ‚π‘›| are the maximum and minimum eigen values respectively. Using the inequality from theorem 2.4 βˆ‘ 𝑏𝑖 2 𝑛 𝑖=1 + π‘Ÿπ‘… βˆ‘ π‘Žπ‘– 2 𝑛 𝑖=1 ≀ (π‘Ÿ + 𝑅) (βˆ‘ π‘Žπ‘–π‘π‘– 𝑛 𝑖=1 ) Assume 𝑏𝑖 = |πœ‚π‘–|, π‘Žπ‘– = 1, π‘Ÿ = |πœ‚π‘›| and 𝑅 = |πœ‚1| , then the inequality implies to Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 2746 https://internationalpubls.com βˆ‘|πœ‚π‘–|2 𝑛 𝑖=1 + |πœ‚π‘›||πœ‚1| βˆ‘ 12 𝑛 𝑖=1 ≀ (|πœ‚π‘›| + |πœ‚1) (βˆ‘ 1|πœ‚π‘–| 𝑛 𝑖=1 ) Using lemma 3.1 2𝐻 + (|πœ‚π‘›||πœ‚1|)𝑛 ≀ (|πœ‚π‘›| + |πœ‚1|)𝐸𝑃𝐸(𝐺) 𝐸𝑃𝐸(𝐺) β‰₯ 2𝐻 + |πœ‚π‘›||πœ‚1| |πœ‚π‘›| + |πœ‚1| Theorem 3.6: Let 𝐺 be a graph with 𝑛 βˆ’ vertices, then the following inequality holds 𝐸𝑃𝐸(𝐺) β‰₯ √2𝑛𝐻 βˆ’ 𝑛2 4 (|πœ‚1| βˆ’ |πœ‚π‘›|)2 Proof. Consider a graph 𝐺 with order 𝑛 and size π‘š. Let |πœ‚1| β‰₯ |πœ‚2| β‰₯ β‹― |πœ‚π‘›| be the eigen values of 𝑃𝐸(𝐺) matrix, where |πœ‚1| and |πœ‚π‘›| are the maximum and minimum eigen values respectively. From theorem 2.2 we have the inequality βˆ‘ π‘Žπ‘– 2 𝑛 𝑖=1 βˆ‘ 𝑏𝑖 2 𝑛 𝑖=1 βˆ’ (βˆ‘ π‘Žπ‘–π‘π‘– 𝑛 𝑖=1 ) 2 ≀ 𝑛2 4 (𝑀1𝑀2 βˆ’ π‘š1π‘š2)2 Assume π‘Žπ‘– = 1, 𝑏𝑖 = |πœ‚π‘–|, 𝑀1𝑀2 = |πœ‚1| and π‘š1π‘š2 = |𝛼𝑛| then βˆ‘ 12 𝑛 𝑖=1 βˆ‘|πœ‚π‘–|2 𝑛 𝑖=1 βˆ’ (βˆ‘ 1 |πœ‚π‘–| 𝑛 𝑖=1 ) 2 ≀ 𝑛2 4 (|πœ‚1| + |πœ‚π‘›|)2 From lemma 3.1 2𝑛𝐻 βˆ’ (𝐸𝑃𝐸(𝐺)) 2 ≀ 𝑛2 4 (|πœ‚1| βˆ’ |πœ‚π‘›|)2 (𝐸𝑃𝐸(𝐺)) 2 β‰₯ √2𝑛𝐻 βˆ’ 𝑛2 4 (|πœ‚1| βˆ’ |πœ‚π‘›|)2 Hence the inequality holds true. Theorem 3.7: Let 𝐺 be a graph with 𝑛 βˆ’ vertices, then the following inequality holds 𝐸𝑃𝐸(𝐺) β‰₯ √2𝑛𝐻 βˆ’ πœ‡(𝑛)(|πœ‚1|βˆ’|πœ‚π‘›|)2 Proof. Consider a graph 𝐺 with order 𝑛 and size π‘š. Let |πœ‚1| β‰₯ |πœ‚2| β‰₯ β‹― |πœ‚π‘›| be the eigen values of 𝑃𝐸(𝐺) matrix, where |πœ‚1| and |πœ‚π‘›| are the maximum and minimum eigen values respectively. Consider the inequality from the theorem 2.3 Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 2747 https://internationalpubls.com |𝑛 βˆ‘ π‘Žπ‘–π‘π‘– βˆ’ βˆ‘ π‘Žπ‘– 𝑛 𝑖=1 βˆ‘ 𝑏𝑖 𝑛 𝑖=1 𝑛 𝑖=1 | ≀ πœ‡(𝑛)(𝐴 βˆ’ π‘Ž)(𝐡 βˆ’ 𝑏) Now assume that π‘Žπ‘– = 𝑏𝑖 = |πœ‚π‘–| , 𝐴 = 𝐡 = |πœ‚1| and π‘Ž = 𝑏 = |πœ‚π‘›|, then the inequality reduces to |𝑛 βˆ‘|πœ‚π‘–|2 βˆ’ (βˆ‘|πœ‚π‘–| 𝑛 𝑖=1 ) 2𝑛 𝑖=1 | ≀ πœ‡(𝑛)(|πœ‚1| βˆ’ |πœ‚π‘›|)(|πœ‚1| βˆ’ |πœ‚π‘›|) From lemma 3.1 |2𝑛𝐻 βˆ’ (𝐸𝑃𝐸(𝐺)) 2 | ≀ πœ‡(𝑛)(|πœ‚1| βˆ’ |πœ‚π‘›|)2 𝐸𝑃𝐸(𝐺) β‰₯ √2𝑛𝐻 βˆ’ πœ‡(𝑛)(|πœ‚1| βˆ’ |πœ‚π‘›|)2 Hence the inequality holds true. Refrences [1] Adiga.C and Smitha,M, On maximum degree energy of a graph, Int. J. Contempt. Math. Sci., 4(2009), 385-396. [2] Ahmed Naji.M and Soner N.D , The maximum eccentricity energy of a graph, Int. J. Sci. Engin. Research, 7(2016), 5-13 [3] M. Biernacki, H. Pidek and C. 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