Exploring the Topological Aspects of Connection-Based Nanostar Dendrimers

Abstract

Topological indices (TIs) have been found to be extensively useful in describing and simulating the chemical structure of diverse molecular compounds, including dendrimers, nanotubes, and neural networks. Dendrimers represent a distinct class of well-defined, highly branched macromolecules characterized by their symmetrical, tree-like architecture. This review provides a comprehensive overview of dendrimer synthesis, structure, properties, and diverse applications in nanoscience. Currently, the field of chemistry is actively exploring a mathematical approach that involves using topological techniques and numerical graph invariants to characterize molecular structures. Out of all the established descriptors, connection-based Zagreb indices are generally regarded as more efficient than the traditional indices. This manuscript presents the overarching outcome for calculating the Zagreb connection indices, specifically, harmonic connection index (HCI), augmented connection index (ACI), symmetric division connection index (SDCI), geometric arithmetic connection index (GACI), hyper Zagreb connection index (HZCI), inverse sum connection index (ISCI), and atom bond connectivity connection index (ABCCI). Furthermore, we compare the numerical and graphical values with each other to assess their relative superiority.

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Arshad, A. , Shabbir, M. , Zainab, S. , Sattar, A. and Javaid, M. (2025) Exploring the Topological Aspects of Connection-Based Nanostar Dendrimers. American Journal of Computational Mathematics, 15, 1-15. doi: 10.4236/ajcm.2025.151001.

1. Introduction

Dendrimers are highly branched, three-dimensional macromolecules with well-defined structures. They were first introduced by Donald A. Tomalia in the early 1980s. The term “dendrimer” is derived from the Greek word “dendron,” which means tree. They belong to a special family of nanoscale materials that have several uses in industries, including catalysis, drug delivery, imaging, and nanotechnology.

Dendrimers can be synthesized using two methods, the divergent approach and the convergent approach. In contemporary times, dendrimers stand out as prominently engineered macromolecules with wide-ranging applications in the field of biomedical science. These include gene transfection, drug delivery, tissue engineering, contrast enhancement for magnetic resonance imaging, and immunology. For further information [1]-[3].

Using numerical graphs descriptors, Researchers are attempting to define the chemical attributes of molecular structures. The popular method in computational and mathematical chemistry for characterizing the molecular structures is through numerical graph descriptors (topological indices).

Topological indices are numerical values derived from the molecular structure of chemical compounds, representing their connectivity and shape. These indices are crucial in cheminformatics and QSAR (quantitative structure-activity relationship) modeling to predict molecules’ physicochemical properties and biological activities. Topological indices reflect molecules’ size, volume, and surface area, which influence properties like boiling point and solubility. Higher branching in a molecule often increases the value of certain indices, correlating with reduced boiling points and densities. Some indices, like the Wiener and Zagreb indices, relate to molecular polarity and hydrophobicity, affecting solubility and partition coefficients. Indices can predict the stability of molecular structures by quantifying electron delocalization and resonance effects, influencing reactivity and chemical stability. Topological indices help model drug-likeness, permeability, and bioavailability by correlating with biological activity.

The current field of study uses TIs to mathematically characterize chemical structures. TI is a numerical measure that helps to correlate the topology of chemical compounds and is associated with graphs. TIs are useful in establishing correlations between many physiochemical characteristics of molecular structures, such as density, strain energy, melting point, volatility, stability, and flammability. Numerous TI that are potential candidates for measuring the physical and chemical properties of chemical compounds may be found in the literature.

The innovative idea of distance-based TI was first proposed by Wiener [4]. The first degree-based Zagreb index (ZI) was established by Gutman and Trinajstic [5]. After this invention, researchers used a variety of degree and distance based TIs to predict the topological characteristics of various substances.

In 1998, Estrada et al. [6] conducted a study on a noteworthy topological index known as the atom bond connectivity (ABC) index. Following this, Ghorbani et al. [7] introduced an updated version of the ABC index. Additionally, in 2009, Vukicevic and Furtula [8] introduced another significant index known as the geometric arithmetic (GA) index.

Additionally, Garaovoc et al. [9] provided the fifth iteration of the GA index, which he used to verify the chemical characteristics of dendrimers. In 2010, Vukicevic [8] introduced the novel idea of the symmetric division degree (SDD) index. The augmented Zagreb index (AZI) was first presented by Furtula et al. [10]. Furthermore, Fajtlowicz [11] proposed the concept of harmonic index (HI). The idea of the inverse sum (IS) index was introduced by Vukicevic and Gasperov [12]. Shirdel et al. provided the definition of hyper ZI (HZI) [13].

Ali and Trinajstic [14] have introduced a novel approach to investigate the psycho-chemical characteristics of compounds. They achieved this by introducing a concept known as the connection number (CN) of a vertex and initiating the Zagreb connection indices (ZCIs). The connection number of a vertex is defined as the count of vertices that are exactly two edges away from that specific vertex.

They found that the recently suggested connection-based ZIs as compared to the traditional ZIs, are more applicable for predicting the physiochemical features of different molecular structures. Numerous researchers began investigating novel connection-based indices following the development of CN. Haoer et al. [15] studied multiplicative leap ZIs. Recently Arshad et al. [16] [17] calculated connection base Zagreb indices of path, cycle and complete graphs.

Nanostar dendrimers are a nanoscale polymer structure with star like architecture, consisting of multiple dendrimer branches radiating from a central core. Their highly branched and symmetric structure gives them unique physicochemical properties, which render them useful in pharmaceutical applications such as drug delivery, nanomedicine, and material science. The relative surface area to volume ratio of nanostar dendrimers allows multiple functional groups for drug conjugation, targeting ligands, or imaging agents. Their nanoscale size (typically 1 - 10 nm) enables efficient penetration of biological membranes. The hydrophilic or hydrophobic nature of dendrimers can be tuned by modifying surface functional groups, enhancing solubility in aqueous or organic solvents. They exhibit high chemical and thermal stability, ensuring longevity in harsh environments. Nanostar dendrimers are synthesized with precise control over size and shape, resulting in monodisperse populations that ensure reproducible behavior in biological systems. The internal pores of nanostar dendrimers enable encapsulation for hydrophobic drugs, and the outer surface can be functionalized for specific targeting such as activation. They modulate drug release to enable sustained drug delivery and targeted drug release to mitigate side effects. Surface modification (e.g., PEGylation) enhances biocompatibility and decreases cytotoxicity, rendering them suitable for biomedical applications. Nanostar dendrimers have low immunogenicity, enabling their safe use in vivo. The star-like architecture offers several attachment points that increase interactions with biological targets and improve binding affinity in both diagnostics and therapeutics.

Recently, Sattar and Javaid [18] derived general expressions for calculating the MZCI of dendrimer nanostars. In addition, Ye and Qureshi [19] computed the ZCIs for nanotubes and a regular hexagonal lattice.

Bokhary and Imran [20] investigated the topological characteristics of certain nanostars, while Gharibi et al. [21] introduced the concept of Zagreb polynomials for nanocones and nanotubes.

A few days ago, Aiman and Aqsa [22] recently calculated the ZCIs for a PPEI and PPIO dendrimers.

To find additional information, we suggest that readers refer to [23] [24].

This paper introduces a comprehensive expression for calculating various ZCIs for significant types of dendrimer nanostar networks, including the Harmonic Connection Index (HCI), Augmented Zagreb Connection Index (AZCI), Symmetric Division Connection Index (SDCI), Geometric Arithmetic Connection Index (GACI), Hyper Zagreb Connection Index (HZCI), Inverse Sum Connection Index (ISCI), and Atom Bond Connectivity Connection Index (ABCCI).

Section 2 covers some fundamental definitions. In Section 3, we present the general result for calculating the ZCIs of the dendrimer network, including HCI, AZCI, SDCI, AGCI, HZCI, ISCI, and ABCCI. Section 4 contains the primary results for ZCIs computations in the dendrimer network. Sections 5 and 6 offer a numerical and graphical comparison of the dendrimer network based on the computed results, concluding the article.

Table 1 provides a list of acronyms used in this paper 1.

Table 1. List of acronyms.

Name

Acronyms

Connection numbers

CN

Topological index

TI

Zagreb connection index

ZCI

Harmonic connection index

HCI

Augmented Zagreb connection index

AZCI

Symmetric division connection index

SDCI

Geometric arithmetic connection index

GACI

Hyper Zagreb connection index

HZCI

Inverse sum connection index

ISCI

Atom bond connectivity connection index

ABCCI

2. Preliminaries

Consider a network ϖ=( A( ϖ ),B( ϖ ) ) with B( ϖ ) as a edge set and A( ϖ ) as the set of vertex. The degree of a vertex is defined as the count of vertices at a distance of one from it. The connection number of a specific vertex is the count of vertices at a distance of two from it.

We introduce the connection-based ZI, as proposed by Javaid and Sattar [18] [25].

Definition 2.1 For a network ϖ , the HCI is defined as;

HCI( ϖ )= d,kB( ϖ ) 2 β( d )+β( k ) ,

β( d ) and β( k ) represent the CNs of vertices d and k , respectively.

Definition 2.2 For a network ϖ , the AZCI is defined as;

AZCI( ϖ )= d,kB( ϖ ) [ β( d )×β( k ) β( h )+β( k )2 ] 3 ,

β( d ) and β( k ) represent the CNs of vertices d and k , respectively.

Definition 2.3 For a network ϖ , the SDCI is defined as;

SDCI( ϖ )= d,kB( ϖ ) [ min( β( d ),β( k ) ) max( β( d ),β( k ) ) + max( β( d ),β( k ) ) min( β( d ),β( k ) ) ],

where min( β( d ),β( k ) ) is the minimum of β( d ) and β( k ) and max( β( d ),β( k ) ) is the maximum of β( d ) and β( k ) .

Definition 2.4 For a network ϖ , the GACI is defined as;

GACI( ϖ )= d,kB( ϖ ) 2 β( d )β( k ) β( d )+β( k ) ,

β( d ) and β( k ) represent the CNs of vertices d and k , respectively.

Definition 2.5 For a network ϖ , the HZCI is defined as;

HZCI( ϖ )= d,kB( ϖ ) [ β( d )+β( k ) ] 2 ,

β( d ) and β( k ) represent the CNs of vertices d and k , respectively.

Definition 2.6 For a network ϖ , the ISCI is defined as;

ISCI( ϖ )= d,kB( ϖ ) [ β( d )×β( k ) β( h )+β( k ) ],

β( d ) and β( k ) represent the CNs of vertices d and k , respectively.

Definition 2.7 For a network ϖ , the ABCCI is defined as;

ABCCI( ϖ )= d,kB( ϖ ) β( d )+β( k )2 β( d )×β( k ) ,

β( d ) and β( k ) represent the CNs of vertices d and k , respectively.

3. Connection-Based ZIs of Nanostar Dendrimers

In this portion, we calculate the connection-based ZIs, such as HCI, AZCI, SDCI, GACI, HZCI, ISCI, and ABCCI for Nanostar dendrimers with molecular structures D[m] for m = 1, 2, and 3, you need to use the information provided in Figure 1, Figure 2, and Figure 3, which includes the connection numbers of each vertex.

Figure 1. D[m] together with CN is 2, 3, 4.

Figure 2. D[m] together with CN is 2, 3, 4, 6.

Figure 3. D[m] together with CN is 2, 3, 4, 6.

Now, let’s discuss the total number of edges across all hexagons.

Table 2. Total number of edge on CN base.

S.R

B ( β( d ),β( k ) ) ( ϖ )

Number of edges

B ( 2,2 ) ( ϖ )

6( 2 m1 )

B ( 2,3 ) ( ϖ )

6( 2 m1 )

B ( 3,3 ) ( ϖ )

12( 2 m1 )12

B ( 3,4 ) ( ϖ )

30( 2 m1 )24

B ( 4,4 ) ( ϖ )

9( 2 m1 )6

B ( 4,6 ) ( ϖ )

3( 2 m1 )3

4. Main Results

Theorem 4.1 HCI of a network ϖ is given by

HCI= 2 m1 ( 20.8214 )12.9571.

Proof. By using Definition 2.1 and Table 2, we get

HCI( ϖ )= d,kB( ϖ ) [ 2 β( d )+β( k ) ] =| B ( 2,2 ) ( ϖ ) |[ 2 β( d )+β( k ) ]+| B ( 2,3 ) ( ϖ ) |[ 2 β( d )+β( k ) ] +| B ( 3,3 ) ( ϖ ) |[ 2 β( d )+β( k ) ]+| B ( 3,4 ) ( ϖ ) |[ 2 β( d )+β( k ) ] +| B ( 4,4 ) ( ϖ ) |[ 2 β( d )+β( k ) ]+| B ( 4,6 ) ( ϖ ) |[ 2 β( d )+β( k ) ] =6( 2 m1 )( 2 2+2 )+6( 2 m1 )( 2 2+3 ) +( 12( 2 m1 )12 )( 2 3+3 )+( 30( 2 m1 )24 )( 2 3+4 ) +( 9( 2 m1 )6 )( 2 4+4 )+( 3( 2 m1 )3 )( 2 4+6 ) =3( 2 m1 )+2.4( 2 m1 )+[ 4( 2 m1 )4 ]+[ 8.5714( 2 m1 )6.8571 ] +[ 2.25( 2 m1 )1.5 ]+[ 0.6( 2 m1 )0.6 ] = 2 m1 ( 3+2.4+5714+2.25+0.6 )+( 46.85711.50.6 ) = 2 m1 ( 20.8214 )12.9571.

Theorem 4.2 AZCI of a network ϖ is given by

AZCI= 2 m1 ( 899.0742 )663.2413.

Proof. By using Definition 2.2 and Table 2, we get

AZCI( ϖ )= d,kB( ϖ ) [ β( d )×β( k ) β( d )+β( k )2 ] 3 =| B ( 2,2 ) ( ϖ ) | [ β( d )×β( k ) β( d )+β( k )2 ] 3 +| B ( 2,3 ) ( ϖ ) | [ β( d )×β( k ) β( d )+β( k )2 ] 3 +| B ( 3,3 ) ( ϖ ) | [ β( d )×β( k ) β( d )+β( k )2 ] 3 +| B ( 3,4 ) ( ϖ ) | [ β( d )×β( k ) β( d )+β( k )2 ] 3 +| B ( 4,4 ) ( ϖ ) | [ β( d )×β( k ) β( d )+β( k )2 ] 3 +| B ( 4,6 ) ( ϖ ) | [ β( d )×β( k ) β( d )+β( k )2 ] 3 =6( 2 m1 ) ( 2×2 2+22 ) 3 +6( 2 m1 ) ( 2×3 2+32 ) 3 +( 12( 2 m1 )12 ) ( 3×3 3+32 ) 3 +( 30( 2 m1 )24 ) ( 3×4 3+42 ) 3 +( 9( 2 m1 )6 ) ( 4×4 4+42 ) 3 +( 3( 2 m1 )3 ) ( 4×6 4+62 ) 3 =6( 2 m1 ) 2 3 +6( 2 m1 ) 2 3 +( 12( 2 m1 )12 ) ( 9 4 ) 3 +( 30( 2 m1 )24 ) ( 12 5 ) 3 +( 9( 2 m1 )6 ) ( 8 3 ) 3 +( 3( 2 m1 )3 ) 3 3 = 2 m1 ( 48+48+136.6875+414.72+170.667 ) +( 136.6875331.776113.777881 ), = 2 m1 ( 899.0742 )663.2413.

Theorem 4.3 SDCI of a network ϖ is given by

SDCI= 2 m1 ( 135.999 )92.5.

Proof. By using Definition 2.3 and Table 2, we get

SDCI( ϖ )= d,kB( ϖ ) [ min( β( d ),β( k ) ) max( β( d ),β( k ) ) + max( β( d ),β( k ) ) min( β( d ),β( k ) ) ] =| B ( 2,2 ) ( ϖ ) |[ min( β( d ),β( k ) ) max( β( d ),β( k ) ) + max( β( d ),β( k ) ) min(β( d ),β( k ) ] +| B ( 2,3 ) ( ϖ ) |[ min( β( d ),β( k ) ) max( β( d ),β( k ) ) + max( β( d ),β( k ) ) min( β( d ),β( k ) ) ] +| B ( 3,3 ) ( ϖ ) |[ min( β( d ),β( k ) ) max( β( d ),β( k ) ) + max( β( d ),β( k ) ) min(β( d ),β( k ) ] +| B ( 3,4 ) ( ϖ ) |[ min( β( d ),β( k ) ) max( β( d ),β( k ) ) + max( β( d ),β( k ) ) min( β( d ),β( k ) ) ] +| B ( 4,4 ) ( ϖ ) |[ min( β( d ),β( k ) ) max( β( d ),β( k ) ) + max( β( d ),β( k ) ) min( β( d ),β( k ) ) ] +| B ( 4,6 ) ( ϖ ) |[ min( β( d ),β( k ) ) max( β( d ),β( k ) ) + max( β( d ),β( k ) ) min( β( d ),β( k ) ) ]

=6( 2 k1 )( min( 2,2 ) max( 2,2 ) + max( 2,2 ) min( 2,2 ) ) +6( 2 k1 )( min( 2,3 ) max( 2,3 ) + max( 2,3 ) min( 2,3 ) ) +( 12( 2 k1 )12 )( min( 3,3 ) max( 3,3 ) + max( 3,3 ) min( 3,3 ) ) +( 30( 2 k1 )24 )( min( 3,4 ) max( 3,4 ) + max( 3,4 ) min( 3,4 ) ) +( 9( 2 k1 )6 )( min( 4,4 ) max( 4,4 ) + max( 4,4 ) min( 4,4 ) ) +( 3( 2 k1 )3 )( min( 4,6 ) max( 4,6 ) + max( 4,6 ) min( 4,6 ) ) =6( 2 m1 )( 2 2 + 2 2 )+6( 2 m1 )( 2 3 + 3 2 ) +( 12( 2 m1 )12 )( 3 3 + 3 3 )+( 30( 2 m1 )24 )( 3 4 + 4 3 ) +( 9( 2 m1 )6 )( 4 4 + 4 4 )+( 3( 2 m1 )3 )( 4 6 + 6 4 ) =6( 2 m1 )( 2 )+6( 2 m1 )( 13 )+[ 24( 2 m1 )24 ] +[ 62.499( 2 m1 )50 ]+[ 18( 2 m1 )12 ]+[ 6.5( 2 m1 )6.5 ] = 2 m1 ( 12+13+24+62.499+18+6.5 )+( 2450126.5 ) = 2 m1 ( 136 )92.5.

Theorem 4.4 GACI of a network ϖ is given by

GACI= 2 m1 ( 65.5102 )44.6931.

Proof. By using Definition 2.4 and Table 2, we get

GACI( ϖ )= d,kB( ϖ ) 2 β( d )β( k ) β( d )+β( k ) =| B ( 2,2 ) ( ϖ ) | 2 β( d )β( k ) β( d )+β( k ) +| B ( 2,3 ) ( ϖ ) | 2 β( d )β( k ) β( d )+β( k ) +| B ( 3,3 ) ( ϖ ) | 2 β( d )β( k ) beta( d )+beta( k ) +| B ( 3,4 ) ( ϖ ) | 2 β( d )β( k ) β( d )+β( k ) +| B ( 4,4 ) ( ϖ ) | 2 β( d )β( k ) β( d )+β( k ) +| B ( 4,6 ) ( ϖ ) | 2 β( d )β( k ) β( d )+β( k ) =6( 2 m1 ) 2 2×2 2+2 +6( 2 m1 ) 2 2×3 2+3 +( 12( 2 m1 )12 ) 2 3×3 3+3 +( 30( 2 m1 )24 ) 2 3×4 3+4 +( 9( 2 m1 )6 ) 2 4×4 4+4 +( 3( 2 m1 )3 ) 2 4×6 4+6

=6( 2 m1 ) 4 4 +6( 2 m1 ) 2 6 2 +( 12( 2 m1 )12 ) 6 6 +( 30( 2 m1 )24 ) 4 3 7 +( 9( 2 m1 )6 ) 8 8 +( 3( 2 m1 )3 ) 4 6 10 = 2 m1 ( 6+5.8787+12+29.29.6922+9+2.9393 ) +( 1223.753862.9393 ), = 2 m1 ( 65.5102 )44.6931.

Theorem 4.5 HZCI of a network ϖ is given by

HZCI= 2 m1 ( 3124 )2292.

Proof. By using Definition 2.5 and Table 2, we get

HZCI( ϖ )= d,kB( ϖ ) [ β( d )+β( k ) ] 2 =| B ( 2,2 ) ( ϖ ) | [ β( d )+β( k ) ] 2 +| B ( 2,3 ) ( ϖ ) | [ β( d )+β( k ) ] 2 +| B ( 3,3 ) ( ϖ ) | [ β( d )+β( k ) ] 2 +| B ( 3,4 ) ( ϖ ) | [ β( d )+β( k ) ] 2 +| B ( 4,4 ) ( ϖ ) | [ β( d )+β( k ) ] 2 +| B ( 4,6 ) ( ϖ ) | [ β( d )+β( k ) ] 2 =6( 2 m1 ) ( 2+2 ) 2 +6( 2 m1 ) ( 2+3 ) 2 +( 12( 2 m1 )12 ) ( 3+3 ) 2 +( 30( 2 m1 )24 ) ( 3+4 ) 2 +( 12( 2 m1 )12 ) ( 4+4 ) 2 +( 3( 2 m1 )3 ) ( 4+6 ) 2 = 2 m1 ( 96+150+432+1470+576+300 ) +( 4321176384300 ) = 2 m1 ( 3124 )2292.

Theorem 4.6 ISCI of a network ϖ is given by

ISCI= 2 m1 ( 107.8285 )66.3428.

Proof. By using Definition 2.6 and Table 2, we get

ISCI( ϖ )= d,kB( ϖ ) [ β( d )×β( k ) ( β( d )+β( k ) ) ] =| B ( 2,2 ) ( ϖ ) |[ β( d )×β( k ) ( β( d )+β( k ) ) ]+| B ( 2,3 ) ( ϖ ) |[ β( d )×β( k ) ( β( d )+β( k ) ) ] +| B ( 3,3 ) ( ϖ ) |[ β( d )×β( k ) ( β( d )+β( k ) ) ]+| B ( 3,4 ) ( ϖ ) |[ β( d )×β( k ) ( β( d )+β( k ) ) ] +| B ( 4,4 ) ( ϖ ) |[ β( d )×β( k ) ( β( d )+β( k ) ) ]+| B ( 4,6 ) ( ϖ ) |[ β( d )×β( k ) ( β( d )+β( k ) ) ] =6( 2 m1 )( 2×2 2+2 )+6( 2 m1 )( 2×3 2+3 ) +( 12( 2 m1 )12 )( 3×3 3+3 )+( 30( 2 m1 )24 )( 3×4 3+4 )

+( 9( 2 m1 )6 )( 4×4 4+4 )+( 3( 2 m1 )3 )( 4×6 4+6 ) = 2 m1 ( 6+7.2+18+51.4285+18+7.2 ) +( 1841.1428127.2 ) = 2 m1 ( 107.8285 )66.3428.

Theorem 4.7 ABCCI of a network ϖ is given by

ABCCI= 2 m1 ( 41.3614 )28.8861.

Proof. By using Definition 2.7 and Table 2, we get

ABCCI( ϖ )= d,kB( ϖ ) β( d )+β( k )2 β( d )×β( k ) =| B ( 2,2 ) ( ϖ ) | β( d )+β( k )2 β( d )×β( k ) +| B ( 2,3 ) ( ϖ ) | β( d )+β( k )2 β( d )×β( d ) +| B ( 3,3 ) ( ϖ ) | β( d )+β( k )2 β( d )×β( k ) +| B ( 3,4 ) ( ϖ ) | β( d )+β( k )2 β( d )×β( k ) +| B ( 4,4 ) ( ϖ ) | β( d )+β( k )2 β( d )×β( k ) +| B ( 4,6 ) ( ϖ ) | β( d )+β( k )2 β( d )×β( k ) =6( 2 m1 ) 2+22 2×2 +6( 2 m1 ) 2+32 2×3 +[ 12( 2 m1 )12 3+32 3×3 ]+[ 30( 2 m1 )24 3+42 3×4 ] +[ 9( 2 m1 )6 4+42 4×4 ]+[ 3( 2 m1 )3 4+62 4×6 ] =6( 2 m1 ) 1 2 +6( 2 m1 ) 1 2 +( 12( 2 m1 )12 ) 4 9 +( 30( 2 m1 )24 ) 5 12 +( 9( 2 m1 )6 ) 6 16 +( 3( 2 m1 )3 ) 1 3 = 2 m1 ( 4.2426+4.2426+8+19.3649+5.5113+1.7320 ) +( 815.49193.67421.7320 ) = 2 m1 ( 41.3614 )28.8861.

5. Comparative Analysis

5.1. Comparison among Nanostar Dendrimer of ZCIs

In this section, we will analyze the graphical and numerical comparisons of Nanostar dendrimers using connection-based ZIs, including HCI, AZCI, SDCI, AGCI, HZCI, ISCI, and ABCCI. We will refer to Table 3 for the numerical data, and the graphical representation is shown in Figure 4.

By examining both Table 3 and Figure 4, it becomes evident that the nanostar dendrimers and HZCI consistently achieve the highest values within this network. The graphical representation in Figure 4 illustrates that HZCI has a higher line than all the other ZCIs within the dendrimers network.

Table 3. Calculated connection-based ZIs values of Graph ( ϖ ) from m=1,2,3,,8 .

ZCIs

m=1

m=2

m=3

m=4

m=5

m=6

m=7

m=8

HCI

7.8643

28.6857

70.3285

153.6141

320.1853

653.27

1319.61

2652.18

AZCI

226.83

111.6907

2897.0556

6457.3523

13577.94

27819.13

56301.50

113266.25

SDCI

43.499

179.498

451.496

995.492

2083.48

4259.46

8611.43

17315.37

GACI

20.8171

86.3273

217.3477

479.3885

1003.47

2051.63

4147.95

8340.61

HZCI

832

3956

10204

22700

47692

97676

197644

397580

ISCI

41.4857

149.3142

364.9712

796.2852

1658.91

3384.16

3498.68

3735.70

ABCCI

12.4753

53.8367

136.5595

302.0051

632.89

1294.67

2618.24

5265.37

Figure 4. Graph ( ϖ ) for values of m ranging from 1,2,3,,8 .

5.2. Comparison between Nanostar Dendrimer and PPEI Dendrimer

In this section, we numerically compare connection-based ZIs values of nanostar dendrimer and PPEI dendrimer.

Table 4. Calculated connection-based ZIs values of Graph (Ω) from m=1,2,3,,8 [22].

ZCIs

m=1

m=2

m=3

m=4

m=5

m=6

m=7

m=8

ISCI(Ω)

24.86

77.93

184.06

396.33

820.86

1669.93

3368.07

6764.35

GACI(Ω)

31.29

80.45

178.79

375.47

768.82

155.52

3128.93

6275.75

HCI(Ω)

11.06

32.53

75.46

161.33

333.06

676.53

1363.47

2737.35

ABCCI(Ω)

21.83

52.51

113.76

236.26

481.25

971.23

1951.20

3911.14

HZCI(Ω)

752

2332

5492

11812

24452

49732

100292

201412

SDCI(Ω)

53

153

353

753

1553

3153

6353

8681

In Table 3, we calculated all ZCI values of Nanostar dendrimer and in Table 4 calculated ZCI values of PPEI dendrimer. So, we compare ZCI values (ISCI, GACI, HCI, ABCCI, HZCI, and SDCI and AZCI) of both dendrimers. We finalize the results of these dendrimers. The first ISCI has the highest value of PPEI dendrimer, followed by the Nanostar dendrimer. The GACI is the highest values of Nanostar dendrimer, HCI is the highest values of PPEI dendrimer, ABCCI is the highest value of Nanostar dendrimer, HZCI is the highest value of Nanostar dendrimer, SDCI is the highest value of Nanostar dendrimer and the last one AZCI single dendrimer highest value because PPEI denderimer could not find the indices. So, we observed that the HZCI has the highest value of both dendrimers. However, this indicates that the Nanostar dendrimer exhibits better chemical applicability compared to the PPEI dendrimer.

6. Concluding Remarks

We conclude our discussion with the following remarks.

1) This article presents the derived general expression for computing nanostar dendrimers using ZCIs, specifically HCI, AZCI, SDCI, GACI, HZCI, ISCI, and ABCCI. Furthermore, we have conducted a comparison of the aforementioned ZCIs of Nanostar dendrimer, and also numerically comparison of Nanostar dendrimer and PPEI dendrimer.

2) By examining using Table 3 and Figure 4, HZCI is the highest value numerically and the highest line through graphically in Nanostar dendrimer. After numerically comparsion of Nanostar dendrimer and PPEI dendrimer, the Nanostar dendrimer has better chemical applicability compared to the PPEI dendrimer.

Future Directions

Advancement of nanostar dendrimers in targeted drug delivery, cancer therapy and diagnostics is their future. Their architecture increases biocompatibility, regulates drug release, and increases imaging. Other potential uses include antimicrobial agents, gene delivery, and tissue engineering. If the current research works out, nanostar dendrimers could change the course of nanomedicine, catalysis and environmental solutions by overcoming the limitations of scalability, toxicity and cost.

Data Availability

The data used to support the findings of this study are included in this article. However, the reader may contact the corresponding author for more details on the data.

Conflicts of Interest

The authors have no conflict of interest regarding this article.

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