Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 31 No. 2 (2024) 416 https://internationalpubls.com Computing Topological Indices of Certain Networks Vidya S Umadi1, A M Sangogi2 1Assistant Professor Department of Mathematics, Vidya Samvardhak Mandal’s Somashekhar R Kothiwale Institute of Technology, Nipani, Karnataka State, India vidyaumadi@gmail.com 2Professor Department of Mathematics, SGBIT, Belagavi, Karnataka State, India. amsangogi@gmail.com Article History: Received: 01-03-2024 Revised: 29-04-2024 Accepted: 15-05-2024 Abstract: In mathematical chemistry, topological indices are molecular descriptors that are calculated on the molecular graph of a chemical compound. The molecular graph is a graph which is obtained from some chemical structures. The degree of every molecular graph cannot exceeds 4. Topological indices are numerical quantities of a graph that describe its topology. An atom represents a vertex and a bond between two atoms represents an edge in a molecular graph. Mainly there are three types of topological indices viz., degree-based, distance based and eigenvalue-based topological indices. The first degree-based topological indices are the first and second Zagreb indices. The first Zagreb index M_1 is defined as the sum of squares of degrees of each vertex in a graph G and the second Zagreb index M_2 is the product of degree of every adjacent vertices. In this case the summation goes on the set of edges of a graph G. The most studied topological indices are degree-based topological indices. Motivated by these topological indices in this paper, we introduce five new degree-based topological indices based on the neighborhood degree of a vertex. Further, we compute the values of various nanostructures like hexagonal parallelogram P(m,n) nanotube, triangular benzenoid G_n,zigzag-edge coronoid fused with starphene nanotubes ZCS(k,l,m), dominating derived networks D_1,D_2,D_3, Porphyrin Dendrimer, Zinc-Porphyrin Dendrimer, Propyl Ether Imine Dendrimer, Poly(Ethylene amido amine Dendrimer, PAMAM dendrimers(𝑃𝐷1,𝑃𝐷2,𝐷𝑆1), linear polyomino chain L_n,Z_n,B_n^1 (nβ‰₯3),B_n^2 (nβ‰₯3) and triangular, hourglass, and jagged-rectangle benzenoid systems of these indices. The standard computational techniques are used for the computation of topological indices of nanostructures. For the edge partition of the nanostructures the algebraic techniques are used. Using these techniques computation of topological indices became easy and also helped to get the more accurate results. Keywords: Molecular Graph, Nanostructures, Dendrimers, Topological indices. 1. Introduction In the realm of modern chemistry, the quest to understand the intricate structures of molecules and their impact on chemical properties has led researchers to explore various analytical tools and methodologies. Among these, the field of mathematical chemistry stands out for its emphasis on applying mathematical concepts and techniques to unravel the Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 31 No. 2 (2024) 417 https://internationalpubls.com mysteries of molecular structures. Central to this endeavor is the study of molecular graphs and their characterization through topological indices, which serve as powerful descriptors of molecular topology. Topological indices represent numerical quantities derived from the molecular graph of a chemical compound. The molecular graph itself is a representation of the chemical structure, wherein atoms are depicted as vertices and bonds as edges. By analyzing the connectivity patterns and geometrical arrangements within these graphs, researchers can gain valuable insights into the structural features that influence the behavior of molecules in various chemical contexts[1]. Within the framework of topological indices, three main categories emerge: degree-based, distance-based, and eigenvalue-based indices. Each category offers unique perspectives on molecular topology, with degree-based indices being particularly prominent due to their simplicity and effectiveness in capturing essential structural information. One of the cornerstone degree-based indices is the Zagreb indices, comprising the first and second Zagreb indices. The first Zagreb index, denoted as M1M1[2], quantifies the sum of the squares of vertex degrees in the molecular graph, providing a measure of overall connectivity. On the other hand, the second Zagreb index, denoted as M2M2, captures the product of degrees of adjacent vertices, thus highlighting local structural motifs within the molecule[3]. Building upon the foundational concepts of degree-based indices, this paper introduces five novel topological indices rooted in the notion of neighborhood degree. The neighborhood degree of a vertex reflects the cumulative degree of its neighboring vertices, offering insights into the local structural environment of each vertex. By incorporating this concept into the design of new indices, the paper aims to enrich the repertoire of tools available for analyzing molecular graphs and uncovering subtle structural variations[4]. Beyond theoretical development, this paper also emphasizes the practical applications of topological indices to a diverse array of nanostructures. Nanostructures, characterized by their unique geometries and properties at the nanoscale, present intriguing challenges and opportunities for topological analysis. Examples of such nanostructures include hexagonal parallelogram nanotubes, benzenoid systems, dendrimers, and polyomino chains, among others. By computing the proposed indices for these nanostructures, the paper seeks to demonstrate their effectiveness in capturing the complex topology inherent in these systems.To facilitate the computation of topological indices for nanostructures, the paper employs a combination of standard computational techniques and algebraic methods for edge partitioning. These techniques not only streamline the calculation process but also enhance the accuracy and reliability of the results obtained. By leveraging computational and algebraic tools, researchers can explore the intricate details of molecular topology with greater efficiency and precision[5]. Introduction of Novel Degree-Based Topological Indices: The primary objective of this paper is to introduce five new degree-based topological indices that are based on the concept of neighborhood degree. These indices are designed to provide a more nuanced characterization of molecular graphs, with a focus on capturing local structural information. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 31 No. 2 (2024) 418 https://internationalpubls.com Application to Various Nanostructures: Another objective is to demonstrate the applicability of the proposed indices to a diverse range of nanostructures, including nanotubes, benzenoid systems, dendrimers, and polyomino chains. By computing these indices for different nanostructures, the paper aims to showcase their utility in analyzing complex molecular architectures[6,7]. Utilization of Computational and Algebraic Techniques: The paper aims to leverage standard computational techniques for the computation of topological indices, supplemented by algebraic methods for edge partitioning in nanostructures. This approach is expected to enhance the efficiency and accuracy of the calculations, facilitating more robust analysis and interpretation of the results[8]. Overall, the objectives of the paper encompass both theoretical advancements in topological index theory and practical applications to real-world nanostructures, with a focus on enhancing our understanding of molecular topology in mathematical chemistry[9,10].In this section, we consider chemical structures like hexagonal parallelogram 𝑃(π‘š, 𝑛) nanotube, triangular benzenoid 𝐺𝑛,zigzag-edge coronoid fused with starphene nanotubes 𝑍𝐢𝑆(π‘˜, 𝑙, π‘š), dominating derived networks 𝐷1, 𝐷2, 𝐷3, Porphyrin Dendrimer, Zinc-Porphyrin Dendrimer, Propyl Ether Imine Dendrimer, Poly(Ethylene amido amine Dendrimer, PAMAM dendrimers(𝑃𝐷1,𝑃𝐷2,𝐷𝑆1), linear polyomino chain 𝐿𝑛, 𝑍𝑛, 𝐡𝑛 1(𝑛 β‰₯ 3), 𝐡𝑛 2(𝑛 β‰₯ 3) and triangular, hourglass, and jagged-rectangle benzenoid systems [2,3,4,5]. For notations and terminology used in this paper are taken from. 2. Related Works Topological indices have got importance due to its applications in chemistry as well as in life science. Recently, Hosamani et al. [11], have put forward the following new degree- based topological indices: 𝑆1(𝐺) = βˆ‘ 𝑑(𝑣𝑖) |𝑑(𝑣𝑖)| π‘£π‘–βˆˆπ‘‰ (1) 𝑆2(𝐺) = βˆ‘ (𝑑(𝑣𝑖)|𝑑(𝑣𝑖)| π‘£π‘–π‘£π‘—βˆˆπΈ + 𝑑(𝑣𝑗)|𝑑(𝑣𝑗)|) (2) 𝑆3(𝐺) = βˆ‘ (𝑑(𝑣𝑖)|𝑑(𝑣𝑗)| π‘£π‘–π‘£π‘—βˆˆπΈ + 𝑑(𝑣𝑗)|𝑑(𝑣𝑖)|) (3) 𝑆4(𝐺) = βˆ‘ (𝑑(𝑣𝑖)|𝑑(𝑣𝑖)| π‘£π‘–π‘£π‘—βˆˆπΈ + 𝑑(𝑣𝑗)|𝑑(𝑣𝑗)|) (4) 𝑆5(𝐺) = βˆ‘ (𝑑(𝑣𝑖)|𝑑(𝑣𝑗)| π‘£π‘–π‘£π‘—βˆˆπΈ + 𝑑(𝑣𝑗)|𝑑(𝑣𝑖)|) (5) 3. Methodology Motivated by the inverse degree of a vertex and the above-mentioned topological indices, here we introduced the following topological indices in the field of chemical graph theory. 𝑅𝑆1(𝐺) = βˆ‘ 1 𝑑(𝑣𝑖)|𝑑(𝑣𝑖)|π‘£π‘–βˆˆπ‘‰ (6) 𝑅𝑆2(𝐺) = βˆ‘ 1 𝑑(𝑒)|𝑑(𝑒)|+𝑑(𝑣)|𝑑(𝑣)|π‘’π‘£βˆˆπΈ (7) 𝑅𝑆3(𝐺) = βˆ‘ 1 𝑑(𝑒)|𝑑(𝑣)|+𝑑(𝑣)|𝑑(𝑒)|π‘’π‘£βˆˆπΈ (8) 𝑅𝑆4(𝐺) = βˆ‘ 1 𝑑(𝑒)|𝑑(𝑒)|𝑑(𝑣)|𝑑(𝑣)|π‘’π‘£βˆˆπΈ (9) Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 31 No. 2 (2024) 419 https://internationalpubls.com 𝑅𝑆5(𝐺) = βˆ‘ 1 𝑑(𝑒)|𝑑(𝑣)|𝑑(𝑣)|𝑑(𝑒)|π‘’π‘£βˆˆπΈ (10) In this paper, we consider their chemical structures like hexagonal parallelogram 𝑃(π‘š, 𝑛) nanotube, triangular benzenoid 𝐺𝑛, zigzag-edge coronoid fused with starphene nanotubes 𝑍𝐢𝑆(π‘˜, 𝑙, π‘š), dominating derived networks 𝐷1, 𝐷2, 𝐷3, Porphyrin Dendrimer, Zinc-Porphyrin Dendrimer, Propyl Ether Imine Dendrimer, Poly(Ethylene amido amine Dendrimer, PAMAM dendrimers(𝑃𝐷1,𝑃𝐷2,𝐷𝑆1), linear polyomino chain 𝐿𝑛, 𝑍𝑛, 𝐡𝑛 1(𝑛 β‰₯ 3), 𝐡𝑛 2(𝑛 β‰₯ 3) and triangular, hourglass, and jagged-rectangle benzenoid systems which are depicted in the following figures 2.1, 2.2, 2.3, 2.4, 2.5 and 2.6 respectively: Figure 2.1: hexagonal parallelogram . Figure 2.2: Triangular benzenoid . Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 31 No. 2 (2024) 420 https://internationalpubls.com Figure 2.3: The zigzag-edge coronoid fused with starphene. Figure 2.4: Dominating derived network. Figure 2.5: Porphyrin dendrimer. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 31 No. 2 (2024) 421 https://internationalpubls.com Figure 2.6: Benzoid hourglass system. 4. Results and Discussion Theorem 1. Let 𝐺 denotes the line graph of subdivision graph of the hexagonal parallelogram, then 𝑅𝑆2(𝐺) = 1 2 π‘šπ‘› + 1145 3348 (π‘š + 𝑛) + 1087 1674 (11) 𝑅𝑆3(𝐺) = 1 6 π‘šπ‘› + 823 1836 (π‘š + 𝑛) + 401 918 (12) 𝑅𝑆4(𝐺) = 1 81 π‘šπ‘› + 929 5832 (π‘š + 𝑛) + 611 1458 (13) 𝑅𝑆5(𝐺) = 1 81 π‘šπ‘› + 1037 5832 (π‘š + 𝑛) + 557 1458 (14) Proof. Let (π‘š,);,βˆˆβ„€+ be a hexagonal parallelogram of order 2(π‘š+ 𝑛+ π‘šπ‘›i and size (3π‘šπ‘›+ 2π‘š+ 2𝑛+ 1) respectively. Let 𝐺= 𝐿(𝑆(𝑃(π‘š,𝑛))) denotes the line graph of subdivision graph of 𝑃(π‘š,𝑛);π‘š,π‘›βˆˆβ„€+ then clearly, the order and size of 𝐺are 2(3mn+2m+2n+1) and 9π‘šπ‘›+ 4π‘š+ 4𝑛+ 5 respectively. The edge set of 𝐺 can be partitioned into three disjoint sets πœ€2,2,πœ€2,3 andi πœ€3,3, where πœ€(𝐿(𝑆(𝑃(π‘š,𝑛)))) =πœ€2,2βˆͺπœ€2,3βˆͺπœ€3,3. Further, βˆ£πœ€2,2∣ = 2(π‘š+𝑛+4), βˆ£πœ€2,3∣ = 4(π‘š+π‘›βˆ’2), βˆ£πœ€3,3∣ = 9π‘šπ‘›βˆ’2π‘šβˆ’2π‘›βˆ’5. Such that βˆ£πœ€(𝐿(𝑆(𝑃(π‘š,𝑛))))∣ = βˆ£πœ€2,2∣+βˆ£πœ€2,3∣+βˆ£πœ€3,3∣ = 9π‘šπ‘›+4π‘š+4𝑛+5. Thus, with this background by employing equations (1)-(5) and (6)-(10), we get the required results. Theorem 2. Let ((𝐺𝑛)) denotes their line graphic of subdivision graph of the hexagonal parallelogram, then 𝑅𝑆2(𝐿(𝑆(𝐺𝑛))) = 83 1000 𝑛2 + 3 5 𝑛 + 41 50 (15) 𝑅𝑆3(𝐿(𝑆(𝐺𝑛))) = 9 108 𝑛2 + 19 25 𝑛 βˆ’ 9 100 (16) 𝑅𝑆4(𝐿(𝑆(𝐺𝑛))) = 9 1458 𝑛2 + 1 4 𝑛 + 3 25 (17) 𝑅𝑆5(𝐿(𝑆(𝐺𝑛))) = 9 1458 𝑛2 + 27 100 𝑛 + 47 100 (18) Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 31 No. 2 (2024) 422 https://internationalpubls.com Proof. Let 𝐺𝑛;βˆˆβ„€+ be a triangular benzenoid of order 𝑛2+ 4𝑛+ 1 and size 3 2 𝑛(𝑛 + 3)respectively. Let (𝑆(𝐺𝑛))) denotes the line graph of subdivision graph of 𝐺𝑛 then clearly, the order and size of 𝐿(𝑆(𝐺𝑛))) are 3𝑛(𝑛+ 3) and 3(3𝑛2+7𝑛+2) 2 respectively. The edge set of (𝑆(𝐺𝑛))) can be partitioned into three disjoint sets πœ€2,2,πœ€2,3 and πœ€3,3, where (𝐿(𝑆(𝐺𝑛)))) = πœ€2,2 βˆͺπœ€2,3 βˆͺπœ€3,3. Further, βˆ£πœ€2,2∣ = 3(𝑛+ 3), βˆ£πœ€2,3∣ = 6(π‘›βˆ’ 1), βˆ£πœ€3,3∣ = 3(3𝑛2+π‘›βˆ’4) 2 . Such that |πœ€ (𝐿(𝑆(𝐺𝑛)))| = |πœ€2,2| + |πœ€2,3| + |πœ€3,3| = 3(3𝑛2 + 7𝑛 + 2) 2 . Thus, with thisbackground by employing equations (1)-(5) and (6)-(10), we get the required results. Theorem 3. Let ((𝐼)) be the line graph of the subdivision graph of zigzag-edges coronoid fused with starphene nanotubes 𝑍𝐢𝑆(π‘˜,𝑙,π‘š) for π‘˜= 𝑙= π‘š= 4. Then 𝑅𝑆2(𝐿(𝑆(𝐼))) = 3 2 (π‘˜ + 𝑙 + π‘š) βˆ’ 355 1116 (19) 𝑅𝑆3(𝐿(𝑆(𝐼))) = 1129 612 (π‘˜ + 𝑙 + π‘š) βˆ’ 941 100 (20) 𝑅𝑆4(𝐿(𝑆(𝐼))) = 103 200 (π‘˜ + 𝑙 + π‘š) βˆ’ 271 100 (21) 𝑅𝑆5(𝐿(𝑆(𝐼))) = 57 100 (π‘˜ + 𝑙 + π‘š) βˆ’ 31 10 (22) Proof. Let be zizag-edge coronoid fused with starphene nanotubes (π‘˜,,) for π‘˜= 𝑙= π‘š= 4 of order 36π‘˜+ 54 and size 15(π‘˜+ 𝑙+ π‘š) βˆ’ 63 respectively. Let ((𝐼)) be the line graphic of the subdivision graph of zigzag-edge coronoid fused with starphene nanotubes (π‘˜,,π‘š) for π‘˜= 𝑙= π‘š= 4. Theni clearly, the order and size of ((𝐼)) are 30(π‘˜+𝑙+π‘š126) and 39(π‘˜+𝑙+π‘š)+153 respectively. The edge set of 𝐿(𝑆(𝐼)) can be partitioned into three disjoint sets πœ€2,2,πœ€2,3 and πœ€3,3,where πœ€(𝐿(𝑆(𝐼))) = πœ€2,2i βˆͺπœ€2,3 βˆͺπœ€3,3. Further, βˆ£πœ€2,2∣ = 6(π‘˜+ 𝑙+π‘šβˆ’ 5), βˆ£πœ€2,3∣ = 12(π‘˜+ 𝑙+ π‘šβˆ’ 7), βˆ£πœ€3,3∣ = 21(π‘˜+ 𝑙+ π‘š) βˆ’ 39. Such that ∣(𝐿(𝑆(𝐼)))∣ = βˆ£πœ€2,2∣ + βˆ£πœ€2,3∣ + βˆ£πœ€3,3∣ = 39(π‘˜+ 𝑙+ π‘š) + 153. Thus, with this background by employing equations (1)-(5) and (6)-(10),we get the required results. Theorem 4. Let 𝐷1(𝑛) be the dominating derived network of 1st type. Then 𝑅𝑆2(𝐷1(𝑛)) = 9 25 𝑛2 + 1 5 𝑛 + 3 100 (23) 𝑅𝑆3(𝐷1(𝑛)) = 49 100 𝑛2 + 19 25 𝑛 βˆ’ 8 25 (24) 𝑅𝑆4(𝐷1(𝑛)) = 9 500 𝑛2 + 29 100 𝑛 βˆ’ 21 500 (25) 𝑅𝑆5(𝐷1(𝑛)) = 1 50 𝑛2 + 39 10 𝑛 βˆ’ 11 100 (26) Proof. Let 𝐷1(𝑛) be the dominating derived network of 1st type. The edge set of 𝐷1(𝑛) can be partitioned into six disjoint sets πœ€2,2,πœ€2,3,πœ€2,4,πœ€3,3,πœ€3,4 and πœ€4,4, where πœ€(𝐷1(𝑛)) = Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 31 No. 2 (2024) 423 https://internationalpubls.com πœ€2,2βˆͺπœ€2,3 βˆͺπœ€2,4 βˆͺπœ€3,3 βˆͺπœ€3,4 βˆͺπœ€4,4. Further, βˆ£πœ€2,2∣ = 4𝑛, βˆ£πœ€2,3∣ = 4π‘›βˆ’ 4, βˆ£πœ€2,4∣ = 28𝑛 16 βˆ£πœ€3,3∣ = 9𝑛2 βˆ’ 13𝑛+ 5, βˆ£πœ€3,4∣ = 36𝑛2 βˆ’ 56𝑛+ 24 and βˆ£πœ€4,4∣ = 36𝑛2βˆ’ 52𝑛+20. Such that βˆ£πœ€(𝐷1(𝑛))∣ = βˆ£πœ€2,2βˆ£βˆ£πœ€2,3∣ + βˆ£πœ€2,4∣ + βˆ£πœ€3,3∣ +i βˆ£πœ€3,4∣+ βˆ£πœ€4,4∣. Thus, with this background by employing equations (1)-(5) and (6)-(10), we get the required results. Theorem 5. Let 𝐷2(𝑛) be the dominating derived network of 2nd type. Then 𝑅𝑆2(𝐷2(𝑛)) = 79 100 𝑛2 βˆ’ 2 5 𝑛 + 13 50 (27) 𝑅𝑆3(𝐷2(𝑛)) = 69 50 𝑛2 βˆ’ 41 100 𝑛 + 3 50 (28) 𝑅𝑆4(𝐷2(𝑛)) = 17 100 𝑛2 + 13 200 𝑛 + 11 250 (29) 𝑅𝑆5(𝐷2(𝑛)) = 13 50 𝑛2 + 21 500 𝑛 + 13 500 (30) Proof. Let 𝐷2(𝑛) be the dominating derived network of 2nd type. The edge set of 𝐷1(𝑛) can be partitioned into five disjoint sets πœ€2,2,πœ€2,3,πœ€2,4,πœ€3,4 and πœ€4,4, where (𝐷2(𝑛)) =πœ€2,2 βˆͺπœ€2,3 βˆͺπœ€2,4 βˆͺπœ€3,4 βˆͺπœ€4,4. Further, βˆ£πœ€2,2∣ = 4𝑛, βˆ£πœ€2,3∣ = 18𝑛2 βˆ’22𝑛+6,i βˆ£πœ€2,4∣= 28π‘›βˆ’16, βˆ£πœ€3,4∣ = 36𝑛2 βˆ’ 56𝑛+ 24 and βˆ£πœ€4,4∣ = 36𝑛2 βˆ’52𝑛+ 20. Such that ∣(𝐷2(𝑛))∣ = βˆ£πœ€2,2∣ + βˆ£πœ€2,3∣ + βˆ£πœ€2,4∣ + βˆ£πœ€3,4∣ + βˆ£πœ€4,4∣. Thus, with this background by employing equations(1)-(5) and (6)-(10), we get the required results. Theorem 6. Let 𝐷3(𝑛) be the dominating derived network of 3rd type. Then 𝑅𝑆2(𝐷3(𝑛)) = 7 25 𝑛2 + 21 100 𝑛 + 17 200 (31) 𝑅𝑆3(𝐷3(𝑛)) = 127 100 𝑛2 βˆ’ 17 50 𝑛 + 43 500 (32) 𝑅𝑆4(𝐷3(𝑛)) = 9 250 𝑛2 + 23 100 𝑛 + 7 1000 (33) 𝑅𝑆5(𝐷3(𝑛)) = 141 1000 𝑛2 + 17 100 𝑛 + 7 1000 (34) Proof. Let 𝐷3(𝑛 ) be the dominating derived network of 3rd type. The edge set of 𝐷1(𝑛) can be partitioned into three disjoint sets πœ€2,2,πœ€2,4 and πœ€4,4, where πœ€(𝐷3(𝑛)) = πœ€2,2 βˆͺπœ€2,4 βˆͺ πœ€4,4. Further, βˆ£πœ€2,2∣ = 4𝑛, βˆ£πœ€2,4∣ = 36𝑛2 βˆ’ 20𝑛 and βˆ£πœ€4,4∣ = 72𝑛2 βˆ’ 108𝑛+ 44. Such that ∣(𝐷3(𝑛))∣ = βˆ£πœ€2,2∣ + βˆ£πœ€2,4∣ + βˆ£πœ€4,4∣. Thus, with this background by employing equations (1)-(5) and (6)-(10), we get the required results. Theorem 7. Let 𝐷𝑛𝑃𝑛 be the prophyrin dendrimer. Then 𝑅𝑆2(𝐷𝑛𝑃𝑛) = 323 100 𝑛 βˆ’ 41 50 (35) 𝑅𝑆3(𝐷𝑛𝑃𝑛) = 967 100 𝑛 βˆ’ 49 50 (36) 𝑅𝑆4(𝐷𝑛𝑃𝑛) = 63 50 𝑛 βˆ’ 37 100 (37) Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 31 No. 2 (2024) 424 https://internationalpubls.com 𝑅𝑆5(𝐷𝑛𝑃𝑛) = 399 50 𝑛 βˆ’ 79 200 (38) Proof. Let 𝐷𝑛𝑃𝑛be the prophyrin dendrimer of order 96π‘›βˆ’10 and size 105π‘›βˆ’11 respectively. The edge set of 𝐷𝑛𝑃𝑛 can be partitioned into six disjoint sets πœ€1,3,πœ€1,4,πœ€2,2,πœ€2,3,πœ€3,3 and πœ€3,4, where πœ€(𝐷𝑛𝑃𝑛) = πœ€1,3 βˆͺπœ€1,4 βˆͺπœ€2,2 βˆͺπœ€2,3 βˆͺπœ€3,3βˆͺπœ€3,4. Further, βˆ£πœ€1,3∣= 2𝑛, βˆ£πœ€1,4∣ = 24𝑛, βˆ£πœ€2,2∣= 10π‘›βˆ’ 5, βˆ£πœ€2,3∣ = 48π‘›βˆ’ 6, βˆ£πœ€3,3∣ = 13𝑛 and βˆ£πœ€3,4∣ = 8𝑛. Such that ∣(𝐷𝑛𝑃𝑛)∣ = βˆ£πœ€1,3∣ + βˆ£πœ€1,4∣ +βˆ£πœ€2,2∣ βˆ£πœ€2,3∣ + βˆ£πœ€3,3∣ + βˆ£πœ€3,4∣ = 105π‘›βˆ’ 11. Thus, with this background by employing equations (1)-(5) and (6)-(10), we get the required results. Theorem 8. Let 𝐷𝑃𝑍𝑛 be the Zinc-Porphyrin dendrimer. Then 𝑅𝑆2(𝐷𝑃𝑍𝑛) = 343 100 2𝑛 βˆ’ 13 10 (39) 𝑅𝑆3(𝐷𝑃𝑍𝑛) = 9 2 2𝑛 βˆ’ 171 100 (40) 𝑅𝑆4(𝐷𝑃𝑍𝑛) = 69 50 2𝑛 βˆ’ 21 50 (41) 𝑅𝑆5(𝐷𝑃𝑍𝑛) = 8 5 2𝑛 βˆ’ 1 2 (42) Proof. Let 𝐷𝑃𝑍𝑛 be the Zinc-Porphyrin dendrimer. of order 96π‘›βˆ’10 and size 105π‘›βˆ’11 respectively. The edge set of 𝐷𝑃𝑍𝑛can be partitioned into four disjoint sets πœ€2,2,πœ€2,3,πœ€3,3 and πœ€3,4, where πœ€(𝐷𝑃𝑍𝑛) = πœ€2,2 βˆͺπœ€2,3 βˆͺπœ€3,3 βˆͺπœ€3,4. Further, βˆ£πœ€2,2∣ = 16 β‹… 2π‘›βˆ’ 4, βˆ£πœ€2,3∣ = 40 β‹… 2π‘›βˆ’ 16, βˆ£πœ€3,3∣ = 8 β‹… 2π‘›βˆ’ 16i and βˆ£πœ€3,4∣ = 4. Such that ∣(𝐷𝑃𝑍𝑛)∣ = βˆ£πœ€2,2∣ + βˆ£πœ€2,3∣ + βˆ£πœ€3,3∣ + βˆ£πœ€3,4∣ = 105π‘›βˆ’ 11.Thus,with this background by employing equations (1)-(5) and (6)-(10),we get the required results. Theorem 9. For the PAMAM dendrimers 𝑃𝐷1, we have 𝑅𝑆2(𝑃𝐷1) = 37 10 2𝑛 βˆ’ 81 50 (43) 𝑅𝑆3(𝑃𝐷1) = 599 100 2𝑛 βˆ’ 13 5 (44) 𝑅𝑆4(𝑃𝐷1) = 23 10 2𝑛 βˆ’ 39 50 (45) 𝑅𝑆5(𝑃𝐷1) = 59 12 2𝑛 βˆ’ 173 100 (46) Proof. Let 𝑃𝐷1 denote PAMAM dendrimers with trifunctional core unit generated by 𝐺𝑛 with 𝑛 growth stages. The edge set of 𝑃𝐷1 can be partitioned into four disjoint sets πœ€1,2,πœ€1,3,πœ€2,2 and πœ€2,3, where πœ€(𝑃𝐷1) = πœ€1,2βˆͺπœ€1,3 βˆͺπœ€2,2 βˆͺπœ€2,3. Further, βˆ£πœ€1,2∣ = 3 β‹… 2𝑛,βˆ£πœ€,3∣ = 6 β‹… 2π‘›βˆ’ 3, βˆ£πœ€2,2∣ = 18 β‹… 2π‘›βˆ’ 9 and βˆ£πœ€2,3∣ = 21 β‹… 2π‘›βˆ’ 12. Such that ∣(𝑃𝐷1)∣ = βˆ£πœ€1,2∣ + βˆ£πœ€1,3∣ + βˆ£πœ€2,2∣ + βˆ£πœ€2,3. Thus, with this background by employing equations (1)-(5) and (6)-(10), we get the required results. Theorem 10. For their PAMAM dendrimers 𝑃𝐷2, we have 𝑅𝑆2(𝑃𝐷2) = 499 100 2𝑛 βˆ’ 49 25 (47) 𝑅𝑆3(𝑃𝐷2) = 399 50 2𝑛 βˆ’ 16 5 (48) 𝑅𝑆4(𝑃𝐷2) = 61 20 2𝑛 βˆ’ 24 25 (49) 𝑅𝑆5(𝑃𝐷2) = 59 9 2𝑛 βˆ’ 11 5 (50) Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 31 No. 2 (2024) 425 https://internationalpubls.com Proof. Let 𝑃𝐷2i denote PAMAM dendrimers with different core unit generated by dendrimer 𝐺𝑛 with 𝑛 growth stages. The edge set of 𝑃𝐷2i can be partitioned into four disjoint sets πœ€1,2,πœ€1,3,πœ€2,2 and πœ€2,3, where πœ€(𝑃𝐷2) = πœ€1,2i βˆͺπœ€1,3 βˆͺπœ€2,2 βˆͺπœ€2,3. Further, βˆ£πœ€1,2∣ = 4 β‹… 2𝑛, βˆ£πœ€1,3∣ =i8 β‹… 2π‘›βˆ’ 4, βˆ£πœ€2,2∣ = 24 β‹… 2π‘›βˆ’ 11 and βˆ£πœ€2,3∣ = 28 β‹… 2π‘›βˆ’ 14. Such that ∣(𝑃𝐷2)∣ = βˆ£πœ€1,2∣ + βˆ£πœ€1,3∣ + βˆ£πœ€2,2∣ + βˆ£πœ€2,3. Thus, with this background by employing equations (1)-(5) and (6)-(10), we get the required results. Theorem 11. For their PAMAM dendrimers 𝐷𝑆1, we have 𝑅𝑆2(𝐷𝑆1) = 32 25 3𝑛 βˆ’ 253 200 (51) 𝑅𝑆3(𝐷𝑆1) = 87 40 3𝑛 βˆ’ 11 8 (52) 𝑅𝑆3(𝐷𝑆1) = 165 256 3𝑛 βˆ’ 161 256 (53) 𝑅𝑆2(𝐷𝑆1) = 105 64 3𝑛 βˆ’ 16 25 (54) Proof. Let 𝐷𝑆1i denote PAMAM dendrimers with different core unit generated by dendrimer 𝐺𝑛 with 𝑛 growth stages. The edge set of 𝐷𝑆1 can be partitioned into three disjoint sets πœ€1,4,πœ€2,2 and πœ€2,4, where πœ€(𝐷𝑆1) = πœ€1,4i βˆͺπœ€2,2 βˆͺπœ€2,4. Further, βˆ£πœ€1,4∣ = 4 β‹… 3𝑛, βˆ£πœ€2,2∣ =10β‹…3π‘›βˆ’10, and βˆ£πœ€2,4∣ = 4β‹…3π‘›βˆ’4. Such that ∣(𝐷𝑆1)∣ = βˆ£πœ€1,4∣+βˆ£πœ€2,2∣+βˆ£πœ€2,4∣. Thus, with this background by employing equations (1)-(5) and (6)-(10), we get the required results. Theorem 12. For a linear polyomino chain 𝐿𝑛we have 𝑅𝑆2(𝐿𝑛) = 1 18 𝑛 + 143 500 (55) 𝑅𝑆3(𝐿𝑛) = 1 18 𝑛 + 393 1000 (56) 𝑅𝑆4(𝐿𝑛) = 1 243 𝑛 + 31 200 (57) 𝑅𝑆5(𝐿𝑛) = 1 243 𝑛 + 873 500 (58) Proof. Let 𝐿𝑛be their polyomino chain with 𝑛squares where 𝑙1 = I 𝑛and π‘š= 1. The edge set of 𝐿𝑛can be partitioned into three disjoint sets πœ€2,2,πœ€2,3 and πœ€3,3, I where πœ€(𝐿𝑛) = πœ€2,2i βˆͺπœ€2,3 βˆͺπœ€3,3. Further, βˆ£πœ€2,2∣ = 2,i βˆ£πœ€2,3∣ = 4, and βˆ£πœ€3,3∣ = 3π‘›βˆ’ 5. Such that ∣(𝐿𝑛)∣ = βˆ£πœ€2,2∣ + βˆ£πœ€2,3∣ + βˆ£πœ€3,3∣. Thus, with this background by employing equations (1)-(5) and (6)-(10), we get the required results. Theorem 13. Let 𝑍𝑛be zigzag polyomino chain with 𝑛 squares such that 𝑙= 2 and π‘š= π‘›βˆ’ 1. Then 𝑅𝑆2(𝑍𝑛) = 63 16640 π‘š + 3 512 𝑛 + 37 100 (59) 𝑅𝑆3(𝑍𝑛) = 15 256 π‘š + 3 512 𝑛 + 43 100 (60) 𝑅𝑆4(𝑍𝑛) = 63 32768 π‘š + 3 65536 𝑛 + 4 25 (61) Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 31 No. 2 (2024) 426 https://internationalpubls.com 𝑅𝑆5(𝑍𝑛) = 255 32768 π‘š + 3 65536 𝑛 + 17 100 (62) Proof Let 𝑍𝑛be zigzag polyomino chain with 𝑛squares such that 𝑙= 2 and π‘š= π‘›βˆ’1. Polyomino chain consists of a sequence of segments 𝑆1,2,β‹…β‹…β‹…,π‘†π‘šand 𝑙(𝑆) = 𝑙where π‘šβ‰₯ 1 and ∈ {1,2,β‹…β‹…β‹…,π‘š}. The edge set of 𝑍𝑛can be partitioned into five disjoint sets πœ€2,2,πœ€2,3, πœ€2,4, πœ€3,4 and πœ€4,4, where πœ€(𝑍𝑛) = πœ€2,2i βˆͺπœ€2,3 βˆͺπœ€2,4 βˆͺπœ€3,4 βˆͺπœ€4,4. Further, βˆ£πœ€2,2∣ = 2, βˆ£πœ€2,3∣ = 4, βˆ£πœ€2,4∣ = 2(π‘šβˆ’ 1), βˆ£πœ€3,4∣ = 2 and βˆ£πœ€4,4∣ = 3π‘›βˆ’ 2π‘šβˆ’ 5. Such that ∣(𝑍𝑛)∣ =βˆ£πœ€2,2∣ + βˆ£πœ€2,3∣ + βˆ£πœ€2,4∣ + βˆ£πœ€3,4∣ +i βˆ£πœ€4,4∣. Thus, with this background by employing equations (1)-(5) and (6)-(10), we get the required results. Theorem 14. For the polyomino chain with 𝑛 squares and of π‘š segments 𝑆1 and 𝑆2i satisfying 𝑙1 = 2 and 𝑙2 = π‘›βˆ’ 1, 𝐡𝑛 1(𝑛β‰₯ 3) we have the following: 𝑅𝑆2(𝐡𝑛 1) = 1 18 𝑛 + 6 25 (63) 𝑅𝑆3(𝐡𝑛 1) = 1 18 𝑛 + 41 100 (64) 𝑅𝑆4(𝐡𝑛 1) = 1 243 𝑛 + 4 25 (65) 𝑅𝑆5(𝐡𝑛 1) = 1 243 𝑛 + 9 50 (66) Proof. Let 𝐡𝑛 1(𝑛β‰₯ 3) be the polyomino chain with 𝑛squares and π‘šsegments 𝑆1i and 𝑆2i satisfying 𝑙1 = 2 and 𝑙2 = π‘›βˆ’ 1. The edge set of 𝐡𝑛 1(𝑛β‰₯ 3) can be partitioned into five disjoint sets πœ€ 2,2,πœ€2,3, πœ€2,4, πœ€3,3i and πœ€3,4, whereπœ€(𝐡𝑛 1(𝑛 β‰₯ 3)) = πœ€22 βˆͺ πœ€23 βˆͺ πœ€24 βˆͺ πœ€33 βˆͺ πœ€34. Further, βˆ£πœ€2,2∣ = 2, βˆ£πœ€2,3∣ = 5, βˆ£πœ€2,4∣ = 1, βˆ£πœ€3,3∣ = 3π‘›βˆ’ 10 and βˆ£πœ€3,4∣ = 3. Such that ∣(𝐡𝑛 1(𝑛β‰₯ 3)) βˆ£πœ€2,2∣ + βˆ£πœ€2,3∣ + βˆ£πœ€2,4∣ + βˆ£πœ€3,3∣ + βˆ£πœ€3,4∣. Thus, with this background by employing equations (1)-(5) and (6)- (10), we get the required results. Theorem 15. For their polyomino chain with 𝑛 squares and of π‘š segments 𝑆1,2,β‹…β‹…β‹…π‘ π‘šsatisfying 𝑙1 = π‘™π‘š= 2 and 𝑙2,𝑙3,β‹…β‹…β‹…,β‰₯ 3 𝐡𝑛 2(𝑛β‰₯ 4) we have the following: 𝑅𝑆2(𝐡𝑛 2) = βˆ’ 2543 78957 π‘š + 1 18 𝑛 + 29 100 (67) 𝑅𝑆3(𝐡𝑛 2) = 17 500 π‘š + 1 18 𝑛 + 33 100 (68) 𝑅𝑆4(𝐡𝑛 2) = 1 100 π‘š + 1 243 𝑛 + 13 100 (69) 𝑅𝑆5(𝐡𝑛 2) = 1 50 π‘š + 1 243 𝑛 + 13 100 (70) Proof. Let 𝐡𝑛 2(𝑛β‰₯4) be the polyomino chain with 𝑛squares and π‘šsegments π‘šsegments 𝑆1,𝑆2,β‹…β‹…β‹…π‘ π‘šsatisfying 𝑙1 = π‘™π‘š= 2 and 𝑙2,𝑙3,β‹…β‹…β‹…,β‰₯ 3. The edge set of 𝐡𝑛 2(𝑛β‰₯4) can be partitioned into five disjoint sets πœ€2,2,πœ€2,3, πœ€2,4, πœ€3,3 and πœ€3,4 where πœ€(𝐡𝑛 2(𝑛 β‰₯ 3)) = πœ€22 βˆͺ πœ€23 βˆͺ πœ€24 βˆͺ πœ€33 βˆͺ πœ€34.Further, βˆ£πœ€2,2∣ = 2, βˆ£πœ€2,3∣ = 2π‘š, βˆ£πœ€2,4∣ = 2, βˆ£πœ€3,3∣ = 3π‘›βˆ’6π‘š+3 and βˆ£πœ€3,4∣ = 4π‘šβˆ’6. Such that ∣(𝐡𝑛 2(𝑛β‰₯ 3))∣ = βˆ£πœ€2,2∣+βˆ£πœ€2,3∣+βˆ£πœ€2,4∣+βˆ£πœ€3,3∣+βˆ£πœ€3,4∣. Thus, with this background by employing equations (1)-(5) and (6)-(10), we get the required results. Theorem 16. Let 𝑇𝑝be a triangular benzenoid where 𝑝i shows the number of hexagons in the base graphic and total number of hexagons in 𝑇𝑝 is 𝑝(𝑝+1) 2 . Then Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 31 No. 2 (2024) 427 https://internationalpubls.com 𝑅𝑆2(𝑇𝑝) = 1 36 𝑝2 + 185 1116 𝑝 + 69 124 (71) 𝑅𝑆3(𝑇𝑝) = 1 36 𝑝2 + 199 612 𝑝 + 27 68 (72) 𝑅𝑆4(𝑇𝑝) = 1 486 𝑝2 + 13 243 𝑝 + 23 72 (73) 𝑅𝑆5(𝑇𝑝) = 1 486 𝑝2 + 79 972 𝑝 + 7 24 (74) Proof. Let 𝑇𝑝 be a triangular benzenoid where 𝑝shows the number of hexagons in the base graphic and total number of hexagons in 𝑇𝑝 is 𝑝(𝑝+1) 2 . The edge set of 𝑇𝑝 can be partitioned into three disjoint sets πœ€2,2,πœ€2,3i and πœ€3,3 where πœ€(𝑇𝑝) = πœ€2,2βˆͺπœ€2,3βˆͺπœ€3,3. Further, βˆ£πœ€2,2∣ = 6, βˆ£πœ€2,3∣ = 6(π‘βˆ’ 1) and |πœ€33| = 3𝑝(π‘βˆ’1) 2 . Such that ∣(𝑇𝑝)∣ = βˆ£πœ€2,2∣ + βˆ£πœ€2,3∣ + βˆ£πœ€3,3∣. Thus, with this background by employing equations (1)-(5) and (6)-(10), we get the required results. Theorem 17. Let 𝑋𝑝 be a benzenoid hourglass. Then 𝑅𝑆2(𝑋𝑝) = 1 18 𝑝2 + 185 558 𝑝 + 467 837 (75) 𝑅𝑆3(𝑋𝑝) = 1 18 𝑝2 + 199 306 𝑝 + 61 459 (76) 𝑅𝑆4(𝑋𝑝) = 1 243 𝑝2 + 26 243 𝑝 + 521 1458 (77) 𝑅𝑆5(𝑋𝑝) = 1 243 𝑝2 + 79 486 𝑝 + 413 1458 (78) Proof. Let 𝑋𝑝be a benzenoid hourglass. The edge set of 𝑋𝑝can be partitioned into three disjoint sets πœ€2,2,πœ€2,3i and πœ€3,3i where πœ€(𝑋𝑝) = πœ€2,2 βˆͺπœ€2,3i βˆͺπœ€3,3. Further, βˆ£πœ€2,2∣ = 8, βˆ£πœ€2,3∣ = 4(3π‘βˆ’4) and βˆ£πœ€3,3∣ = 3𝑝2βˆ’3𝑝+4. Such that ∣(𝑋𝑝)∣ = βˆ£πœ€2,2∣+βˆ£πœ€2,3∣+βˆ£πœ€3,3∣. Thus, with this background by employing equations (1)-(5) and (6)-(10), we get the required results. Theorem 18. Let 𝐡𝑝,be denote a jagged rectangle benzenoid system for all 𝑝,π‘žβˆˆπ‘βˆ’1. Then 𝑅𝑆2(𝐡𝑝,π‘ž) = 1 9 π‘π‘ž + 247 1674 𝑝 + 959 3348 π‘ž + 497 1674 (79) 𝑅𝑆3(𝐡𝑝,π‘ž) = 1 9 π‘π‘ž + 233 918 𝑝 + 721 1836 π‘ž + 175 918 (80) 𝑅𝑆4(𝐡𝑝,π‘ž) = 2 243 π‘π‘ž + 26 729 𝑝 + 905 5832 π‘ž + 605 2916 (81) 𝑅𝑆5(𝐡𝑝,π‘ž) = 2 243 π‘π‘ž + 79 1458 𝑝 + 1013 5832 π‘ž + 551 2916 (82) Proof. Let 𝐡𝑝,be denotes a jagged rectangle benzenoid system for all 𝑝,π‘žβˆˆπ‘βˆ’ 1. The edge set of 𝐡𝑝,π‘žcan be partitioned into three disjoint sets πœ€2,2,πœ€2,3 and πœ€3,3 where πœ€(𝐡𝑝,π‘ž)= πœ€2,2 βˆͺπœ€2,3 βˆͺπœ€3,3. Further, βˆ£πœ€2,2∣ = 2π‘ž+4, βˆ£πœ€2,3∣ = 4𝑝+4π‘žβˆ’4 and βˆ£πœ€3,3∣ =6π‘π‘ž+π‘βˆ’5π‘žβˆ’4. Such that ∣(𝐡𝑝,π‘ž)∣ = βˆ£πœ€2,2∣ + βˆ£πœ€2,3∣ + βˆ£πœ€3,3∣. Thus, with this background by employing equations (1)-(5) and (6)- (10), we get the required results. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 31 No. 2 (2024) 428 https://internationalpubls.com Conclusion In this paper, we have computed the topological index values of chemical structures like hexagonal parallelogram 𝑃(π‘š, 𝑛) nanotube, triangular benzenoid 𝐺𝑛,zigzag-edge coronoid fused with starphene nanotubes 𝑍𝐢𝑆(π‘˜, 𝑙, π‘š), dominating derived networks 𝐷1, 𝐷2, 𝐷3 , Porphyrin Dendrimer, Zinc-Porphyrin Dendrimer, Propyl Ether Imine Dendrimer, Poly(Ethylene amido amine Dendrimer, PAMAM dendrimers(𝑃𝐷1,𝑃𝐷2,𝐷𝑆1), linear polyomino chain 𝐿𝑛, 𝑍𝑛, 𝐡𝑛 1(𝑛 β‰₯ 3), 𝐡𝑛 2(𝑛 β‰₯ 3) and triangular, hourglass, and jagged- rectangle benzenoid systems. References [1] M.S. Ahmad, W. Nazeer, S.M. Kang, M. Imran, and W. Gao, β€œCalculating degree-based topological indices of dominating David derived networks”, Open Physics, vol. 15, no. 1, pp. 1015-1021, 2017. [2] W. Gao, M.K. Jamil, A. Javed, M.R. Farahani, and M. 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