Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 7s (2025) 530 https://internationalpubls.com Quasi- Laplacian energy of some novel classes of graphs Manash Protim Borah a,*, Karam Ratan Singh b a,* Department of Mathematics, L.T.K. College, Azad, North Lakhimpur, 787031, Assam, India, b Department of Basic and Applied Science, National Institute of Technology Arunachal Pradesh, Papum pare, 791113, Arunachal Pradesh, India. *Corresponding author Email address: mpborah36@gmail.com (Manash Protim Borah) Article History: Received: 26-10-2024 Revised:10-11-2024 Accepted:18-12-2024 Abstract: We formulate the relationship of quasi-Laplacian energy of some novel classes of graphs with their corresponding original graphs. The novel graphs in our discussion are the ๐’ฎ-graph, โ„›-graph, ๐’ฌ-graph, total graph, and their join and corona operations graphs. The whole formulation is based on the relationship between quasi-Laplacian energy and the vertex degrees of the novel graph. It is also noted that quasi- Laplacian energy is closely related with the first Zagreb index, number of vertices and edges of the graph. The exact formulas of quasi-Laplacian energy of novel graphs are obtained in terms of the corresponding quasi-Laplacian energies, the first Zagreb indices, and the number of vertices and edges of the original graphs. Keywords: Quasi-Laplacian energy, degree of vertex, Zagreb index, join, corona. Mathematics Subject Classification: 05C07, 05C09, 05C50, 05C76 1. Introduction All graphs discussed in this paper are simple and undirected. Let ๐บ be a graph with vertices denoted by ๐‘‰(๐บ) and edges denoted by ๐ธ(๐บ). Let |๐‘‰(๐บ)| = ๐‘ and |๐ธ(๐บ)| = ๐‘ž. Let ๐‘‘๐บ(๐‘ฃ) represent the degree of vertices in ๐บ, where ๐‘ข โˆˆ ๐‘‰(๐บ). Let ๐ท(๐บ) denote the diagonal matrix and ๐ด(๐บ) the adjacency matrix. The quasi Laplacian matrix, represented by ๐‘„(๐บ), is defined as ๐‘„(๐บ) = ๐ท(๐บ) + ๐ด(๐บ). Let ๐œ‡1(๐บ) โ‰ฅ ๐œ‡2(๐บ) โ‰ฅ โ‹ฏ โ‰ฅ ๐œ‡๐‘›(๐บ) denote the real, symmetric, and positive semi definite eigenvalues of ๐‘„(๐บ). It is known that various graph operations can create novel classes of graphs from the original graphs. Therefore, understanding the relationships between some invariants of such novel graphs and the equivalent invariants of the original graphs is relevant. Graph energy is one such invariant based on the graph spectrum introduced by Gutman [9]. We discuss here the quasi-Laplacian energy [6] of graph ๐บ, represented as ๐ธ๐‘„(๐บ) and determined by the equation ๐ธ๐‘„(๐บ) =โˆ‘ โ€Š ๐‘ ๐‘–=1 ๐œ‡๐‘– 2 Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 7s (2025) 531 https://internationalpubls.com Yue, Cao and Qi, in the paper [6], defined quasi-Laplacian energy of ๐บ is expressed as follows ๐ธ๐‘„(๐บ) =โˆ‘ โ€Š ๐‘ ๐‘–=1 โ€Š๐‘‘๐บ 2(๐‘ข๐‘–) +โˆ‘ โ€Š ๐‘ ๐‘–=1 โ€Š๐‘‘๐บ(๐‘ข๐‘–), ๐‘ข โˆˆ ๐‘‰(๐บ)โ€ฆโ€ฆโ€ฆ(1.1) Also, equation (1.1) can be represented as follows ๐ธ๐‘„(๐บ) =โˆ‘ โ€Š ๐‘ ๐‘–=1 โ€Š๐‘‘๐บ 2(๐‘ฃ๐‘–) +โˆ‘ โ€Š ๐‘ ๐‘–=1 โ€Š๐‘‘๐บ(๐‘ฃ๐‘–) = ๐‘€1(๐บ) + 2๐‘ž โ€ฆโ€ฆโ€ฆ(1.2) where, ๐‘€1 is called first Zagreb index [10] and second part of equation (1.2) is the handshaking lemma โˆ‘๐‘–=1 ๐‘ โ€Š๐‘‘๐บ(๐‘ฃ๐‘–) = 2๐‘ž. It is noticed that the quasi-Laplacian energy of any graph depends upon the degrees of vertices of that graph. Based on the above result discussed in the paper [6]. We formulate the relations of the quasi- Laplacian energy of some classes of novel graphs in terms of corresponding original graphs. The subdivision graph ๐’ฎ(๐บ), โ„›-graph โ„›(๐บ), ๐’ฌ graph ๐’ฌ(๐บ), total graph ๐’ฏ(๐บ) [3] and their join and corona operations graphs are the novel graphs for our discussion. Indulal [8] first defined ๐’ฎ-vertex and ๐’ฎ edge join and Liu and Zhang [16] determined their spectra. Lu and Miao [13] defined ๐’ฎ-vertex corona and edge corona. Liu and Lu [14] defined ๐’ฎ-vertex and edge neighbourhood corona. Sun, Shang, and Bu [16] defined ๐’ฌ-vertex and edge join graphs. The ๐’ฌ- vertex and edge corona are defined by Najiya and Chithra [2]. The definition of the corona of the total graph of one regular and another arbitrary graph, and spectra of the corona of the total graph is determined by Zhu, Tian, and Cui [19]. Also, ๐’ฎ vertex- โ„› vertex join, ๐’ฎ edge- โ„› edge join, ๐’ฎ vertex- โ„› edge join and ๐’ฎ edge- โ„› vertex join are defined by Das and Panigrahi [5, 7]. The ๐’ฎ-vertex-vertex-edge join of three ๐’ฎ graphs is defined by Wen, Zhang, and Li [17]. Berberler [1] derived the quasi-Laplacian energy of graphs based on โ„› graphs [13]. We derive formulas of the quasi-Laplacian energy of ๐’ฎ,๐’ฌ and ๐’ฏ graphs and further, obtain quasi-Laplacian energy of ๐’ฎ-vertex and edge join, ๐’ฎ-vertex and edge corona, ๐’ฎ-vertex and edge neighbourhood corona in terms of their corresponding original graphs. Similarly, we derive quasi-Laplacian energy of ๐’ฌ-vertex and edge join, ๐’ฌ-vertex and edge corona and ๐’ฏ- graph corona. The quasi-Laplacian energy of ๐’ฎ vertex- โ„› vertex join, ๐’ฎedge- โ„› edge join, ๐’ฎ vertex- โ„› edge join, ๐’ฎ edge- โ„› vertex join and ๐’ฎ-vertex-vertex-edge of three graphs join are also derived in terms of their corresponding original graphs. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 7s (2025) 532 https://internationalpubls.com Let ๐บ be the (๐‘, ๐‘ž) graph where sets of old vertices |๐‘‰(๐บ)| = ๐‘ and sets of inserted new vertices ๐ผ(๐บ) โˆฃ= ๐‘ž. Let ๐ป1 be the (๐‘1, ๐‘ž1) graph and ๐ป2 be the (๐‘2, ๐‘ž2) graph. Consequently, |๐‘‰(๐ป1)| = ๐‘1, |๐ผ(๐ป1)| = ๐‘ž1, |๐‘‰(๐ป2)| = ๐‘2 and |๐ผ(๐ป2)| = ๐‘ž2. 2. ๐ธ๐‘„ based on ๐’ฎ graphs The quasi-Laplacian energy of the ๐’ฎ graph, ๐’ฎ join and ๐’ฎ corona graphs are formulated in this section based on the degree of vertices of the ๐’ฎ-graph, ๐’ฎ-join, and ๐’ฎ-corona graphs respectively. Let ๐‘ข be any vertex in ๐’ฎ(๐บ), then the degree of ๐’ฎ(๐บ) is represented by ๐‘‘๐’ฎ(๐บ)(๐‘ข๐‘–) = { ๐‘‘๐บ(๐‘ข๐‘–), if ๐‘ข โˆˆ ๐‘‰(๐บ); 2, if ๐‘ข โˆˆ ๐ผ(๐บ). Theorem 2.1. ๐ธ๐‘„(๐’ฎ(๐บ)) = ๐ธ๐‘„(๐บ) + 6๐‘ž Proof. Using definition (1.1) on the ๐’ฎ(๐บ)-graph, we have ๐ธ๐‘„(๐’ฎ(๐บ))= โˆ‘ โ€Š |๐‘‰(๐’ฎ(๐บ))| ๐‘–=1 โ€Š๐‘‘๐’ฎ(๐บ) 2 (๐‘ข๐‘–) + โˆ‘ โ€Š |๐‘‰(๐’ฎ(๐บ))| ๐‘–=1 โ€Š๐‘‘๐’ฎ(๐บ)(๐‘ข๐‘–) =โˆ‘ โ€Š ๐‘ ๐‘–=1 โ€Š๐‘‘(๐บ) 2 (๐‘ข๐‘–) +โˆ‘ โ€Š ๐‘ž ๐‘–=1 โ€Š22 +โˆ‘โ€Š ๐‘ ๐‘–=1 โ€Š๐‘‘(๐บ)(๐‘ข๐‘–) +โˆ‘ โ€Š ๐‘ž ๐‘–=1 โ€Š2 = ๐ธ๐‘„(๐บ) + 6๐‘ž Now, let ๐‘ข be any vertex in ๐’ฎ-vertex join (๐ป1 โˆจฬ‡ ๐ป2) of two graphs ๐ป1 and ๐ป2. Then, the degree of the vertex ๐‘ข in (๐ป1 โˆจฬ‡ ๐ป2) is given by ๐‘‘๐ป1Vฬ‡๐ป2(๐‘ข๐‘–) = { ๐‘‘๐ป1(๐‘ข๐‘–) + ๐‘2, if ๐‘ข โˆˆ ๐‘‰(๐ป1), for i = 1,2,โ€ฆ p1; 2, if ๐‘ฃ โˆˆ ๐ผ(๐บ1); ๐‘‘๐ป2(๐‘ข๐‘—) + ๐‘1, if ๐‘ฃ โˆˆ ๐‘‰(๐ป2), for j = 1,2,โ€ฆ p2. and ๐ป1 โˆจฬ‡ ๐ป2 has ๐‘1 + ๐‘ž1 + ๐‘2 vertices. We derive quasi-Laplacian energy of ๐’ฎ-vertex join in terms of corresponding original graphs ๐ป1 and ๐ป2. Theorem 2.2. ๐ธ๐‘„(๐ป1 โˆจฬ‡ ๐ป2) = ๐ธ๐‘„(๐ป1) + ๐ธ๐‘„(๐ป2) + 4๐‘ž1๐‘2 + ๐‘1๐‘2 2 + 6๐‘ž1 + 4๐‘1๐‘ž2 + ๐‘1 2๐‘2 + 2๐‘1๐‘2 Proof. Using definition (1.1), quasi-Laplacian energy of ๐’ฎ-vertex join is obtained by Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 7s (2025) 533 https://internationalpubls.com ๐ธ๐‘„(๐ป1 โˆจฬ‡ ๐ป2) = โˆ‘ โ€Š ๐‘1+๐‘ž1+๐‘2 ๐‘–=1 โ€Š๐‘‘๐ป1โˆจฬ‡๐บ2 2 (๐‘ข๐‘–) + โˆ‘ โ€Š ๐‘1+๐‘ž1+๐‘2 ๐‘–=1 โ€Š๐‘‘๐ป1โˆจฬ‡๐ป2(๐‘ข๐‘–) =โˆ‘ โ€Š ๐‘1 ๐‘–=1 โ€Š๐‘‘(๐ป1) 2 (๐‘ข๐‘–) + 2๐‘2โˆ‘โ€Š ๐‘1 ๐‘–=1 โ€Š๐‘‘(๐ป1)(๐‘ข๐‘–) + ๐‘2 2โˆ‘โ€Š ๐‘1 ๐‘–=1 โ€Š+ 4๐‘ž1 +โˆ‘โ€Š ๐‘2 ๐‘—=1 โ€Š๐‘‘(๐ป2) 2 (๐‘ข๐‘—) + 2๐‘1โˆ‘โ€Š ๐‘2 ๐‘—=1 โ€Š๐‘‘(๐ป2)(๐‘ข๐‘—) + ๐‘1 2โˆ‘โ€Š ๐‘2 ๐‘—=1 โ€Š +โˆ‘ โ€Š ๐‘1 ๐‘–=1 โ€Š๐‘‘(๐ป1)(๐‘ข๐‘–) + ๐‘2โˆ‘โ€Š ๐‘1 ๐‘–=1 โ€Š+ 2๐‘ž1 +โˆ‘ โ€Š ๐‘2 ๐‘—=1 โ€Š๐‘‘(๐ป2)(๐‘ข๐‘—) + ๐‘1โˆ‘โ€Š ๐‘2 ๐‘—=1 โ€Š = ๐ธ๐‘„(๐ป1) + ๐ธ๐‘„(๐ป2) + 4๐‘ž1๐‘2 + ๐‘1๐‘2 2 + 6๐‘ž1 + 4๐‘1๐‘ž2 + ๐‘1 2๐‘2 + 2๐‘1๐‘2. Next, we formulate a relation of quasi-Laplacian energy of ๐ป1 โˆจ ๐ป2 join. Let ๐‘ข be any vertex in ๐’ฎ-edge join. The degree of vertex ๐‘ข in ๐ป1 โˆจ ๐ป2 join is given by ๐‘‘๐ป1โˆช๐ป2(๐‘ข๐‘–) = { ๐‘‘๐ป1(๐‘ข๐‘–), if ๐‘ข โˆˆ ๐‘‰(๐ป1); 2 + ๐‘2, if ๐‘ข โˆˆ ๐ผ(๐ป1) ๐‘‘๐ป2(๐‘ฃ๐‘–) + ๐‘ž1, if ๐‘ข โˆˆ ๐‘‰(๐ป2). ; and ๐ป1 โˆจ ๐ป2 has ๐‘1 + ๐‘ž1 + ๐‘2 vertices. Theorem 2.3. ๐ธ๐‘„(๐ป1 โˆจ ๐ป2) = ๐ธ๐‘„(๐ป1) + ๐ธ๐‘„(๐ป2) + 6๐‘ž1๐‘2 + ๐‘ž1๐‘2 2 + 6๐‘ž1 + 4๐‘ž1๐‘ž2 + ๐‘ž1 2๐‘2 Proof. Using equation (1.1), we get ๐ธ๐‘„(๐ป1 โˆจ ๐ป2) = โˆ‘ โ€Š ๐‘1+๐‘ž1+๐‘2 ๐‘–=1 โ€Š๐‘‘๐ป1โŠต๐ป2 2 (๐‘ข๐‘–) + โˆ‘ โ€Š ๐‘1+๐‘ž1+๐‘2 ๐‘–=1 โ€Š๐‘‘๐ป1โˆจ๐ป2(๐‘ข๐‘–) =โˆ‘ โ€Š ๐‘1 ๐‘–=1 โ€Š๐‘‘๐ป1 2 (๐‘ข๐‘–) +โˆ‘ โ€Š ๐‘ž1 ๐‘–=1 โ€Š (2 + ๐‘2) 2 +โˆ‘โ€Š ๐‘2 ๐‘–=1 โ€Š (๐‘‘(๐ป2)(๐‘ข๐‘–) + ๐‘ž1) 2 +โˆ‘โ€Š ๐‘1 ๐‘–=1 โ€Š๐‘‘(๐ป1)(๐‘ข๐‘–) +โˆ‘ โ€Š ๐‘ž1 ๐‘–=1 โ€Š2 +โˆ‘ โ€Š ๐‘2 ๐‘–=1 โ€Š๐‘‘(๐ป2)(๐‘ข๐‘–) + ๐‘ž1 The result can be derived easily. 2.1. ๐ธ๐‘„ of ๐’ฎ-vertex and edge corona Let ๐‘ข be any vertex in ๐’ฎ-vertex corona. The degree of vertex of ๐‘ข in ๐’ฎ-vertex corona is given by ๐‘‘๐ป1โŠ™๐ป2(๐‘ข๐‘–) = { ๐‘‘๐ป1(๐‘ข๐‘–) + ๐‘2, if ๐‘ข โˆˆ ๐‘‰(๐ป1); 2, if ๐‘ข โˆˆ ๐ผ(๐ป1); ๐‘‘๐ป2(๐‘ฃ๐‘— ๐‘–) + 1, if ๐‘ข = ๐‘ฃ๐‘— ๐‘– , for ๐‘– = 1,2,โ€ฆ ๐‘1, for ๐‘— = 1,2,โ€ฆ ๐‘2. and ๐ป1โŠ™๐ป2 has ๐‘1 + ๐‘ž1 + ๐‘1๐‘2 vertices. The formula of quasi-Laplacian energy of ๐’ฎ-vertex corona is given below Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 7s (2025) 534 https://internationalpubls.com Theorem2.4. ๐ธ๐‘„(๐ป1โŠ™๐ป2) = ๐ธ๐‘„(๐ป1) + ๐‘1๐ธ๐‘„(๐ป2) + ๐‘1๐‘2 2 + 4๐‘ž1๐‘2 + 3๐‘ž1 + 3๐‘1๐‘2 + 4๐‘1๐‘ž2 Proof. By using definition (1.1), we get ๐ธ๐‘„(๐ป1โŠ™๐ป2) = โˆ‘ โ€Š ๐‘1+๐‘ž1+๐‘1๐‘2 ๐‘–=1 โ€Š๐‘‘๐ป1โŠ™๐ป2 2 (๐‘ฃ๐‘–) + โˆ‘ โ€Š ๐‘1+๐‘ž1+๐‘1๐‘2 ๐‘–=1 โ€Š๐‘‘๐ป1โŠ™๐ป2(๐‘ข๐‘–) =โˆ‘ โ€Š ๐‘1 ๐‘–=1 โ€Š๐‘‘๐ป1(๐‘ข๐‘–) + ๐‘2) 2 +โˆ‘โ€Š ๐‘ž1 ๐‘–=1 โ€Š22 +โˆ‘ โ€Š ๐‘1 ๐‘–=1 โ€Šโˆ‘ โ€Š ๐‘2 ๐‘—=1 โ€Š (๐‘‘๐ป2(๐‘ฃ๐‘— ๐‘–) + 1) 2 +โˆ‘ โ€Š ๐‘1 ๐‘–=1 โ€Š๐‘‘(๐ป1)(๐‘ข๐‘–) + ๐‘2 +โˆ‘โ€Š ๐‘ž1 ๐‘–=1 โ€Š2 +โˆ‘ โ€Š ๐‘1 ๐‘–=1 โ€Šโˆ‘ โ€Š ๐‘2 ๐‘—=1 โ€Š๐‘‘๐ป2(๐‘ฃ๐‘— ๐‘–) + 1 = ๐‘2 2โˆ‘โ€Š ๐‘1 ๐‘–=1 โ€Š+ 2๐‘2โˆ‘โ€Š ๐‘1 ๐‘–=1 โ€Š๐‘‘๐ป1(๐‘ข๐‘–) +โˆ‘ โ€Š ๐‘1 ๐‘–=1 โ€Š๐‘‘๐ป1 2 (๐‘ข๐‘–) + 4๐‘ž1 +โˆ‘ โ€Š ๐‘1 ๐‘–=1 โ€Šโˆ‘ โ€Š ๐‘2 ๐‘—=1 โ€Š +2โˆ‘ โ€Š ๐‘1 ๐‘–=1 โ€Šโˆ‘ โ€Š ๐‘2 ๐‘—=1 โ€Š๐‘‘๐ป2(๐‘ฃ๐‘—) +โˆ‘ โ€Š ๐‘1 ๐‘–=1 โ€Šโˆ‘ โ€Š ๐‘2 ๐‘—=1 โ€Š๐‘‘๐ป2 2 (๐‘ฃ๐‘—) + ๐‘1๐‘2 +โˆ‘ โ€Š ๐‘1 ๐‘–=1 โ€Š๐‘‘๐ป1(๐‘ข๐‘–) +2๐‘ž1 +โˆ‘โ€Š ๐‘1 ๐‘–=1 โ€Šโˆ‘ โ€Š ๐‘2 ๐‘—=1 โ€Š +โˆ‘ โ€Š ๐‘1 ๐‘–=1 โ€Šโˆ‘ โ€Š ๐‘2 ๐‘—=1 โ€Š๐‘‘๐ป2(๐‘ฃ๐‘—) Hence, the result follows. Let ๐‘ข be any vertex in ๐’ฎ-edge corona, then the degree of the vertex ๐‘ข is given by ๐‘‘๐ป1โŠ–๐ป2(๐‘ข๐‘–) = { ๐‘‘๐ป1(๐‘ข๐‘–), if ๐‘ข โˆˆ ๐‘‰(๐ป1); 2 + ๐‘2, if ๐‘ข โˆˆ ๐ผ(๐ป1) ๐‘‘๐ป2(๐‘ฃ๐‘— ๐‘–) + 1, if ๐‘ข = ๐‘ฃ๐‘— ๐‘– , for ๐‘– = 1,2,โ€ฆ ๐‘ž1, for ๐‘— = 1,2,โ€ฆ ๐‘2. ; and ๐ป1ฮ˜๐ป2 has ๐‘1 + ๐‘ž1 + ๐‘ž1๐‘2 vertices. The formula of quasi-Laplacian energy of ๐’ฎ-edge corona is given by Theorem 2.5. ๐ธ๐‘„(๐ป1โŠ–๐ป2) = ๐ธ๐‘„(๐ป1) + ๐‘ž1๐ธ๐‘„(๐ป2) + 6๐‘ž1 + 7๐‘ž1๐‘2 + 4๐‘ž1๐‘ž2 Proof. Using definition (1.1), Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 7s (2025) 535 https://internationalpubls.com ๐ธ๐‘„(๐ป1โŠ™๐ป2) = โˆ‘ โ€Š |๐‘‰(๐ป1โŠ–๐ป2)| ๐‘–=1 โ€Š๐‘‘๐ป1โŠ–๐ป2 2 (๐‘ข๐‘–) + โˆ‘ โ€Š |๐‘‰(๐ป1โŠ–๐ป2)| ๐‘–=1 โ€Š๐‘‘๐ป1โŠ–๐ป2(๐‘ข๐‘–) = โˆ‘ โ€Š ๐‘1+๐‘ž1+๐‘ž1๐‘2 ๐‘–=1 โ€Š๐‘‘๐ป1โŠ–๐ป2 2 (๐‘ข๐‘–) + โˆ‘ โ€Š ๐‘1+๐‘ž1+๐‘ž1๐‘2 ๐‘–=1 โ€Š๐‘‘๐ป1โŠ–๐ป2 (๐‘ข๐‘–) =โˆ‘ โ€Š ๐‘1 ๐‘–=1 โ€Š๐‘‘๐ป1 2 (๐‘ข๐‘–) +โˆ‘ โ€Š ๐‘ž1 ๐‘–=1 โ€Š (2 + ๐‘2) 2 +โˆ‘ โ€Š ๐‘ž1 ๐‘–=1 โ€Šโˆ‘ โ€Š ๐‘2 ๐‘—=1 โ€Š (๐‘‘๐ป2(๐‘ฃ๐‘— ๐‘–) + 1) 2 +โˆ‘ โ€Š ๐‘1 ๐‘–=1 โ€Š๐‘‘(๐ป1)(๐‘ข๐‘–) +โˆ‘ โ€Š ๐‘ž1 ๐‘–=1 โ€Š2 +โˆ‘ โ€Š ๐‘ž1 ๐‘–=1 โ€Šโˆ‘ โ€Š ๐‘2 ๐‘—=1 โ€Š๐‘‘๐ป2(๐‘ฃ๐‘— ๐‘–) + 1 Hence, the result follows. 2.2. ๐ธ๐‘„ of ๐’ฎ-vertex and edge neighbourhood corona Let ๐‘ข be any vertex in ๐’ฎ-vertex neighbourhood corona. Then degree of vertices is given by ๐‘‘๐ป1โŠŸ๐ป2(๐‘ฃ๐‘–) = { ๐‘‘๐ป1(๐‘ข๐‘–), if ๐‘ข โˆˆ ๐‘‰(๐ป1); 2 + 2๐‘2, if ๐‘ข โˆˆ ๐ผ(๐ป1); ๐‘‘๐ป1(๐‘ข๐‘–) + ๐‘‘๐ป2(๐‘ฃ๐‘—), if ๐‘ข = ๐‘ฃ๐‘— ๐‘– , for ๐‘– = 1,2,โ€ฆ ๐‘1, for ๐‘— = 1,2,โ€ฆ ๐‘2. and ๐ป1โŠŸ๐ป2 has ๐‘1 + ๐‘ž1 + ๐‘1๐‘2 vertices. The quasi-Laplacian energy of ๐’ฎ-vertex neighbourhood corona is given by Theorem 2.6. ๐ธ๐‘„(๐ป1โŠŸ๐ป2) = (1 + ๐‘2)๐ธ๐‘„(๐ป1) + ๐‘1๐ธ๐‘„(๐ป2) + 6๐‘ž1 + 10๐‘ž1๐‘2 + 4๐‘ž1๐‘2 2 + 8๐‘ž1๐‘ž2 Proof: Using definition (1.1), the above Theorem can be easily proved. Also, the degree of any vertex of ๐‘ข in ๐’ฎ-edge neighbourhood corona is given by ๐‘‘๐ป1โŠŸ๐ป2(๐‘ข๐‘–) = { (1 + ๐‘2)๐‘‘๐ป1(๐‘ข๐‘–), if ๐‘ข โˆˆ ๐‘‰(๐ป1); 2, if ๐‘ข โˆˆ ๐ผ(๐ป1) 2 + ๐‘‘๐ป2(๐‘ข๐‘—), if ๐‘ข = ๐‘ฃ๐‘— ๐‘– , for ๐‘– = 1,2,โ€ฆ ๐‘ž1, for ๐‘— = 1,2, โ€ฆ ๐‘2. ; and ๐ป1โŠŸ๐ป2 has ๐‘1 + ๐‘ž1 + ๐‘ž1๐‘2 vertices. The quasi-Laplacian energy of ๐’ฎ-edge neighbourhood corona is given by Theorem 2.7. ๐ธ๐‘„(๐ป1โŠŸ๐ป2) = (1 + 2๐‘2)๐ธ๐‘„(๐ป1) + 2๐‘ž1๐ธ๐‘„(๐ป2) + ๐‘2 2๐‘€1(๐ป1) + 4๐‘ž1 + 2๐‘ž1๐‘2 + 12๐‘ž1๐‘ž2, where ๐‘€1 is the first Zagreb index. Using definition (1.1), the above Theorem can be easily proved. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 7s (2025) 536 https://internationalpubls.com 3. ๐ธ๐‘„ based on ๐’ฌ graph The energy of the ๐’ฌ graph, ๐’ฌ join and ๐’ฌ corona graphs are formulated in this section based on the degree of vertices of the ๐’ฌ-graph, ๐’ฌ-join, and ๐’ฌ-corona graphs respectively. Let ๐‘ข be any vertex in ๐’ฌ(๐บ). Then, the degree of vertex is given by ๐‘‘๐’ฎ(๐บ)(๐‘ข๐‘–) = { ๐‘‘๐บ(๐‘ข๐‘–), if ๐‘ข โˆˆ ๐‘‰(๐บ); 4, if ๐‘ข โˆˆ ๐ผ(๐บ). We derive a formula of energy of ๐’ฌ(๐บ). Theorem 3.1. ๐ธ๐‘„(๐’ฌ(๐บ)) = ๐ธ๐‘„(๐บ) + 20๐‘ž Proof. We follow from definition (1.1), ๐ธ๐‘„(๐’ฌ(๐บ)) == โˆ‘ โ€Š ๐‘+๐‘ž ๐‘–=1 โ€Š๐‘‘๐’ฌ(๐บ) 2 (๐‘ฃ๐‘–) +โˆ‘ โ€Š ๐‘+๐‘ž ๐‘–=1 โ€Š๐‘‘๐’ฌ(๐บ)(๐‘ข๐‘–) = โˆ‘ โ€Š ๐‘ ๐‘–=1 โ€Š๐‘‘(๐บ) 2 (๐‘ข๐‘–) +โˆ‘ โ€Š ๐‘ž ๐‘–=1 โ€Š42 +โˆ‘ โ€Š ๐‘ ๐‘–=1 โ€Š๐‘‘(๐บ)(๐‘ข๐‘–) +โˆ‘ โ€Š ๐‘ž ๐‘–=1 โ€Š4 = ๐ธ๐‘„(๐บ) + 20๐‘ž 3.1. ๐ธ๐‘„ of ๐’ฌ-vertex and edge join Let ๐‘ข be any vertex in ๐ป1โŸจ๐‘ฃโŸฉ๐ป2. Then, the degree of vertex of ๐ป1โŸจ๐‘ฃโŸฉ๐ป2 is given by ๐‘‘๐ป1โŸจ๐‘ฃโŸฉ๐ป2(๐‘ข๐‘–) = { ๐‘‘๐ป1(๐‘ข๐‘–) + ๐‘2, if ๐‘ข โˆˆ ๐‘‰(๐ป1); 4, if ๐‘ข โˆˆ ๐ผ(๐ป1); ๐‘‘๐ป2(๐‘ข๐‘–) + ๐‘1, if ๐‘ข โˆˆ ๐‘‰(๐ป2). ๐ป1โŸจ๐‘ฃโŸฉ๐ป2 has ๐‘1 + ๐‘ž1 + ๐‘2 vertices. The relation of quasi-Laplacian energy in between ๐’ฌ-vertex join with corresponding two original graphs is obtained easily by using definition (1.1) as follows Theorem 3.2. ๐ธ๐‘„(๐ป1โŸจ๐‘ฃโŸฉ๐ป2) = ๐ธ๐‘„(๐ป1) + ๐ธ๐‘„(๐ป2) + 4๐‘ž1๐‘2 + ๐‘1๐‘2 2 + 20๐‘ž1 + 4๐‘1๐‘ž2 + ๐‘1 2๐‘2 + 2๐‘1๐‘ž2 Also, let ๐‘ข be any vertex in ๐’ฌ-edge join. The degree of vertex ๐‘ข of ๐’ฌ-edge join is given by ๐‘‘๐ป1โŸจ๐‘’โŸฉ๐ป2(๐‘ข๐‘–) = { ๐‘‘๐ป1(๐‘ข๐‘–), if ๐‘ข โˆˆ ๐‘‰(๐ป1); 2 + ๐‘2, if ๐‘ข โˆˆ ๐ผ(๐ป1) ๐‘‘๐ป2(๐‘ข๐‘–) + ๐‘ž1, if ๐‘ข โˆˆ ๐‘‰(๐ป2). ; Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 7s (2025) 537 https://internationalpubls.com ๐ป1โŸจ๐‘’โŸฉ๐ป2 has ๐‘1 + ๐‘ž1 + ๐‘2 vertices. The relation of quasi-Laplacian energy in between ๐’ฌ-edge join with corresponding two original graphs is obtained easily by using definition (1.1) as follows Theorem 3.3. ๐ธ๐‘„(๐ป1โŸจ๐‘’โŸฉ๐ป2) = ๐ธ๐‘„(๐ป1) + ๐ธ๐‘„(๐ป2) + 12๐‘ž1๐‘2 + ๐‘ž1๐‘2 + 20๐‘ž1 + ๐‘ž1 2๐‘2 + ๐‘ž1๐‘2 2 3.2. ๐ธ๐‘„ of ๐’ฌ-vertex and edge corona Let ๐‘ข be any vertex in ๐’ฌ-vertex corona. Then, the degree of any vertex ๐‘ข in ๐’ฌ-vertex corona is given by ๐‘‘๐ป1O๐ป2(๐‘ฃ๐‘–) = { ๐‘‘๐ป1(๐‘ข๐‘–)+2, if ๐‘ข โˆˆ ๐‘‰(๐ป1); 4, if ๐‘ข โˆˆ ๐ผ(๐ป1) ๐‘‘๐ป2(๐‘ฃ๐‘— ๐‘–) + 1, if ๐‘ข = ๐‘ฃ๐‘— ๐‘– , for ๐‘– = 1,2,3, โ€ฆ๐‘1, for ๐‘— = 1,2,3, . . ๐‘2. ; ๐ป1o๐ป2 has ๐‘1 + ๐‘ž1 + ๐‘1๐‘2 vertices. Then, by using equation (1.1) we get Theorem 3.4. ๐ธ๐‘„(๐ป1๐‘œ๐ป2) = ๐ธ๐‘„(๐ป1) + ๐‘1๐ธ๐‘„(๐ป2) + ๐‘1๐‘2 2 + 20๐‘ž1 + 4๐‘1๐‘ž2 + 3๐‘1๐‘2 + 4๐‘ž1๐‘2 Next, the degree of any vertex of ๐‘ข in ๐’ฌ-edge corona is given by ๐‘‘๐ป1โŠ›๐ป2(๐‘ข๐‘–) = { ๐‘‘๐ป1(๐‘ข๐‘–), if ๐‘ข โˆˆ ๐‘‰(๐ป1); ๐‘2 + 4, if ๐‘ข โˆˆ ๐ผ(๐ป1); ๐‘‘๐ป2(๐‘ฃ๐‘— ๐‘–) + 1, if ๐‘ข = ๐‘ฃ๐‘— ๐‘– , for ๐‘– = 1,2, โ€ฆ ๐‘1, for ๐‘— = 1,2,โ€ฆ ๐‘2. ๐บ1โŠ›๐บ2 has ๐‘1 + ๐‘ž1 + ๐‘ž1๐‘2 vertices. Then, the quasi-Laplacian energy of ๐’ฌ-edge corona is easily obtained as follows Theorem 3.5. ๐ธ๐‘„(๐ป1โŠ›๐ป2) = ๐ธ๐‘„(๐ป1) + ๐‘1๐ธ๐‘„(๐ป2) + ๐‘ž1๐‘2 2 + 9๐‘ž1๐‘2 + 20๐‘ž1 + 4๐‘ž2๐‘1 + 2๐‘1๐‘ž2 4. ๐ธ๐‘„ based on ๐’ฏ-graph We derive energy of ๐’ฏ graph and ๐’ฏ graph corona based on the degree of vertices of the ๐’ฏ- graph and ๐’ฏ-corona graphs are determined here. Let ๐‘ข be any vertex in ๐’ฏ(๐บ), then the degree of vertex ๐‘ข in ๐’ฏ(๐บ) is given by ๐‘‘๐’ฏ(๐บ)(๐‘ข๐‘–) = { 2๐‘‘๐บ(๐‘ฃ๐‘–), if ๐‘ข โˆˆ ๐‘‰(๐บ); 4, if ๐‘ข โˆˆ ๐ผ(๐บ). The vertices of ๐’ฏ(๐บ) is ๐‘ + ๐‘ž. The ๐‘„ energy of ๐’ฏ(๐บ) is given by Theorem 4.1. ๐ธ๐‘„(๐’ฏ(๐บ)) = 2๐ธ๐‘„(๐บ) + 20๐‘ž + 2๐‘€1(๐บ) Where, ๐‘€1 is the first Zagreb index. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 7s (2025) 538 https://internationalpubls.com 4.1. ๐ธ๐‘„ of ๐’ฏ-graph corona Let ๐ป1 be ๐‘Ÿ1 regular and ๐ป2 be any graph. Also, let ๐‘ข be any vertex in ๐’ฏ(๐บ). Then, the degree of vertex of ๐’ฏ - corona is given by ๐‘‘๐ป1โ‹†๐ป2(๐‘ข๐‘–) = { 2๐‘‘๐ป1(๐‘ข๐‘–) + ๐‘2, if ๐‘ข โˆˆ ๐‘‰(๐ป1); 2๐‘Ÿ1, if ๐‘ข โˆˆ ๐ผ(๐ป1) ๐‘‘๐ป2(๐‘ฃ๐‘— ๐‘–) + 1, if ๐‘ข = ๐‘ฃ๐‘— ๐‘– , for ๐‘– = 1,2,โ€ฆ ๐‘1, for ๐‘— = 1,2,โ€ฆ ๐‘2. ; ๐ป1 โ‹† ๐ป2 has ๐‘1 + ๐‘ž1 + ๐‘1๐‘2 vertices. The ๐ธ๐‘„ of ๐’ฏ-graph corona is easily obtained by using equation (1.1) as follows Theorem 4.2. ๐ธ๐‘„(๐ป1 โ‹† ๐ป2) = 2๐ธ๐‘„(๐ป1) + ๐‘1๐ธ๐‘„(๐ป2) + 2๐‘€1(๐ป1) + 5๐‘1๐‘2 + ๐‘2 2๐‘1 + 4๐‘Ÿ1 2๐‘ž1 + 2๐‘Ÿ1๐‘ž1 + 4๐‘1๐‘ž2 + 2๐‘1๐‘2 where, ๐‘€1 is the first Zagreb index. 5. ๐ธ๐‘„ based on ๐’ฎ-graph and โ„›-graph join The ๐ธ๐‘„ energy of four ๐’ฎ-graph and โ„›-graph joins with their corresponding original graphs ๐ป1 and ๐ป2 are formulated in this part. 5.1. ๐ธ๐‘„ of ๐’ฎ-vertex and โ„›-vertex join First, we formulate the quasi-Laplacian energy of ๐’ฎ-vertex and โ„›-vertex join. Let ๐‘ข be any vertex in ๐’ฎ-vertex and โ„›-vertex join. Then, the degrre of any vertex in ๐’ฎ(๐ป1) โˆจฬˆ โ„›(๐ป2) is given by ๐‘‘๐’ฎ(๐ป1)โˆจฬˆโ„›(๐ป2)(๐‘ข๐‘–) = { ๐‘‘๐ป1(๐‘ข๐‘–) + ๐‘2, if ๐‘ข โˆˆ ๐‘‰(๐ป1); 2, if ๐‘ข โˆˆ ๐ผ(๐ป1) โˆช ๐ผ(๐ป2); 2๐‘‘๐ป2(๐‘ข๐‘–) + ๐‘1, if ๐‘ข โˆˆ ๐‘‰(๐ป2). ๐’ฎ(๐ป1) โˆจฬˆ โ„›(๐ป2) has ๐‘1 + ๐‘ž1 + ๐‘2 + ๐‘ž2 vertices. Theorem 5.1. The quasi-Laplacian energy of ๐ธ๐‘„(๐’ฎ(๐ป1) โˆจฬˆ โ„›(๐ป2)) = ๐ธ๐‘„(๐ป1) + 4๐ธ๐‘„(๐ป2) + ๐‘2 2๐‘1 + ๐‘1 2๐‘2 + 4๐‘ž1๐‘2 + 8๐‘ž2๐‘1 + 2๐‘ž2 + 6๐‘ž1 + 2๐‘1๐‘2 Proof. By using equation (1.1), we get Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 7s (2025) 539 https://internationalpubls.com ๐ธ๐‘„(๐’ฎ(๐ป1) โˆจฬˆ โ„›(๐ป2)) = โˆ‘ โ€Š ๐‘1+๐‘ž1+๐‘2+๐‘ž2 ๐‘–=1 โ€Š๐‘‘๐’ฎ(๐ป1) 2 โˆจฬˆ โ„›(๐ป2)(๐‘ข๐‘–) + โˆ‘ โ€Š ๐‘1+๐‘ž1+๐‘2+๐‘ž2 ๐‘–=1 โ€Š๐‘‘๐’ฎ(๐บ1)โˆจฬˆโ„›(๐บ2)(๐‘ข๐‘–) =โˆ‘ โ€Š ๐‘1 ๐‘–=1 โ€Š๐‘‘๐’ฎ(๐ป1)โˆจฬˆโ„›(๐ป2) 2 (๐‘ข๐‘–) +โˆ‘ โ€Š ๐‘ž1 ๐‘–=1 โ€Š๐‘‘๐’ฎ(๐ป1)โˆจฬˆโ„›(๐ป2) 2 (๐‘ข๐‘–) +โˆ‘ โ€Š ๐‘2 ๐‘—=1 โ€Š๐‘‘๐’ฎ(๐ป1)โˆจฬˆโ„›(๐ป2) 2 (๐‘ข๐‘–) +โˆ‘ โ€Š ๐‘ž2 ๐‘–=1 โ€Š๐‘‘๐’ฎ(๐ป1)โˆจฬˆโ„›(๐ป2) 2 (๐‘ข๐‘–) +โˆ‘ โ€Š ๐‘1 ๐‘–=1 โ€Š๐‘‘๐’ฎ(๐ป1)โˆจฬˆโ„›(๐ป2)(๐‘ข๐‘–) +โˆ‘ โ€Š ๐‘ž1 ๐‘–=1 โ€Š๐‘‘๐’ฎ(๐ป1)โˆจฬˆโ„›(๐ป2)(๐‘ข๐‘–) +โˆ‘ โ€Š ๐‘2 ๐‘–=1 โ€Š๐‘‘๐’ฎ(๐ป1)โˆจฬˆโ„›(๐ป2)(๐‘ข๐‘–) +โˆ‘ โ€Š ๐‘ž2 ๐‘–=1 โ€Š๐‘‘๐’ฎ(๐ป1)โˆจฬˆโ„›(๐ป2)(๐‘ข๐‘–) Hence, the result follows. 5.2. ๐ธ๐‘„ of ๐’ฎ-edge and โ„›-edge join Let ๐‘ข be any vertex in ๐’ฎ-edge and โ„›-edge join. Then, the degree of any vertex of ๐‘ข in ๐’ฎ-edge and โ„›-edge join ๐’ฎ(๐ป1)๐‘‰โ€พโ„›(๐ป2) is given by ๐‘‘๐’ฎ(๐ป1)๐‘‰โ€พโ„›(๐ป2)(๐‘ข๐‘–) = { ๐‘‘๐ป1(๐‘ข๐‘–), if ๐‘ข โˆˆ ๐‘‰(๐ป1); 2 + ๐‘ž2, if ๐‘ฃ โˆˆ ๐ผ(๐ป1); 2๐‘‘๐ป2(๐‘ข๐‘–), if ๐‘ข โˆˆ ๐‘‰(๐ป2); 2 + ๐‘ž1, if ๐‘ข โˆˆ ๐ผ(๐ป2). ๐’ฎ(๐ป1)๐‘‰โ€พโ„›(๐ป2) has ๐‘1 + ๐‘ž1 + ๐‘2 + ๐‘ž2 vertices. The ๐‘„-energy is obtained easily by using equation (1.1). Theorem 5.2. ๐ธ๐‘„ (๐’ฎ(๐ป1)๐‘‰โ€พโ„›(๐ป2)) = ๐ธ๐‘„(๐ป1) + 4๐ธ๐‘„(๐ป2) + 6๐‘ž1 + 10๐‘ž1๐‘ž2 + ๐‘ž1๐‘ž2(๐‘ž1 +๐‘ž2) + 6๐‘ž2 5.3. ๐ธ๐‘„ of ๐’ฎ-vertex and โ„›-edge join Let ๐‘ข be any vertex in ๐’ฎ-vertex and โ„›-edge join. Then, the degree of any vertex of ๐‘ข in ๐’ฎ-vertex and โ„›-edge join ๐’ฎ(๐ป1)๐‘‰โ€พฬ‡โ„›(๐ป2) is given by ๐‘‘๐’ฎ(๐ป1)๏ฟฝฬ‡๏ฟฝโ„›(๐ป2)(๐‘ข๐‘–) = { ๐‘‘๐ป1(๐‘ข๐‘–) + ๐‘ž2, if ๐‘ข โˆˆ ๐‘‰(๐ป1); 2, if ๐‘ข โˆˆ ๐ผ(๐ป1); 2๐‘‘๐ป2(๐‘ข๐‘–), if ๐‘ข โˆˆ ๐‘‰(๐ป2); 2 + ๐‘1, if ๐‘ข โˆˆ ๐ผ(๐ป2). ๐’ฎ(๐บ1)๐‘‰โ€พฬ‡โ„›(๐บ2) has ๐‘1 + ๐‘ž1 + ๐‘2 + ๐‘ž2 vertices. We get the following result by using equation (1.1). Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 7s (2025) 540 https://internationalpubls.com Theorem 5.3. ๐ธ๐‘„ (๐’ฎ(๐ป1)๐‘‰โ€พฬ‡โ„›(๐ป2)) = ๐ธ๐‘„(๐ป1) + 4๐ธ๐‘„(๐ป2) + ๐‘ž2 2๐‘1 + 4๐‘ž1๐‘ž2 + 6๐‘ž1 + 6๐‘ž2๐‘1 + ๐‘2 2๐‘ž2 + 4๐‘ž2 5.4. ๐ธ๐‘„ of ๐’ฎ-edge and โ„›-vertex join Let ๐‘ข be any vertex in ๐’ฎ-edge and โ„›-vertex join. Then, the degree of any vertex of ๐‘ข in ๐’ฎ-edge and โ„›-vertex join ๐’ฎ(๐ป1)๐‘‰โ€พฬ‡โ„›(๐ป2) is given by ๐‘‘๐’ฎ(๐ป1)๐‘‰โ€พโ„›(๐ป2)(๐‘ข๐‘–) = { ๐‘‘๐ป1(๐‘ข๐‘–), if ๐‘ข โˆˆ ๐‘‰(๐ป1); 2 + ๐‘2, if ๐‘ข โˆˆ ๐ผ(๐ป1); 2๐‘‘๐ป2(๐‘ข๐‘–) + ๐‘ž1, if ๐‘ข โˆˆ ๐‘‰(๐ป2); 2, if ๐‘ข โˆˆ ๐ผ(๐ป2). ๐’ฎ(๐ป1)๏ฟฝฬ‡๏ฟฝโ„›(๐ป2) has ๐‘1 + ๐‘ž1 + ๐‘2 + ๐‘ž2 vertices. We easily get the following Theorem by using equation (1.1) Theorem 5.4. ๐ธ๐‘„ (๐’ฎ(๐ป1)๏ฟฝฬ‡๏ฟฝโ„›(๐ป2)) = ๐ธ๐‘„(๐ป1) + 4๐ธ๐‘„(๐ป2) + 6๐‘ž1 + 6๐‘ž1๐‘2 + ๐‘ž1 2๐‘2 + ๐‘ž1๐‘2 2 + 10๐‘ž2 6. ๐ธ๐‘„ of ๐’ฎ-vertex-vertex-edge join of triple graphs Let ๐ป3 be (๐‘3, ๐‘ž3) graph. Then ๐’ฎ-vertex-vertex-edge join of three ๐’ฎ graphs is denoted by ๐ป1 ๐‘† โ–น (๐ป2 ๐‘‰ โˆช ๐ป3 ๐ธ). The degree of vertex ๐‘ข โˆˆ ๐ป1 ๐‘† โ–น (๐ป2 ๐‘‰ โˆช ๐ป3 ๐ธ) is given by ๐‘‘๐ป1๐‘†โ–น(๐ป2๐‘‰โˆช๐ป3๐ธ) (๐‘ข๐‘–) = { ๐‘‘๐ป1(๐‘ข๐‘–) + ๐‘2, if ๐‘ข โˆˆ ๐‘‰(๐ป1); 2 + ๐‘1, if ๐‘ข โˆˆ ๐ผ(๐ป1); ๐‘‘๐ป2(๐‘ข๐‘—) + ๐‘1, if ๐‘ข โˆˆ ๐‘‰(๐ป2), ๐‘— = 1,2,โ€ฆ ๐‘2; ๐‘‘๐ป3(๐‘ค๐‘˜), if ๐‘ข = ๐‘ค๐‘˜ โˆˆ ๐‘‰(๐ป3), ๐‘˜ = 1,2โ€ฆ๐‘3. ๐ป1 ๐‘† โ–น (๐ป2 ๐‘‰ โˆช ๐ป3 ๐ธ) has ๐‘1 + ๐‘ž1 + ๐‘2 + ๐‘3 vertices. The following Theorem is easily obtained by using equation (1.1). Theorem 6.1. ๐ธ๐‘„(๐ป1 ๐‘† โ–น (๐ป2 ๐‘‰ โˆช ๐ป3 ๐ธ) = ๐ธ๐‘„(๐ป1) + ๐ธ๐‘„(๐ป2) + ๐ธ๐‘„(๐ป3) + 4๐‘ž1๐‘2 +๐‘ž1๐‘2 2 + 6๐‘ž1 + 5๐‘ž1๐‘1 + ๐‘1 2๐‘ž1 + 4๐‘ž2๐‘1 + ๐‘1 2๐‘2 + 4๐‘ž1๐‘ž3 + ๐‘ž1 2๐‘3 + 2๐‘1๐‘2 + ๐‘ž1๐‘3. Coclusion: We establish a relation between the quasi-Laplacian energy of few novel graphs and their respective original graphs. 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