# An Analysis of Eccentricity-Based Invariants for Biochemical Hypernetworks

Authors: Muhammad Aamer Rashid; Sarfraz Ahmad; Muhammad Kamran Siddiqui; Shazia Manzoor; Mlamuli Dhlamini
Journal: Complexity
 (2021)

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## Abstract

Biological proceedings are well characterized by solid illustrations for communication networks. The framework of biological networks has to be considered together with the expansion of infectious diseases like coronavirus. Also, the graph entropies have established themselves as the information theoretic measure to evaluate the architectural information of biological networks. In this article, we examined conclusive biochemical networks liket-level hypertrees along with the corona product of hypertrees with path. We computed eccentricity-based indices for the depiction of aforementioned theoretical frameworks of biochemical networks. Furthermore, explicit depiction of the graph entropies with these indices is also measured.


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## Body

## 1. Introduction

Chemical graph theory is the developed mathematical field to study the problems of chemical networks. This field has extensive applications in computer sciences, mathematics, sociology, biology, medicine, and physics [1, 2]. The biological entities such as proteins, RNA, DNA, metabolites, and graphs are used to grab the association between these entities [3, 4]. Topological analysis of wide-ranging protein association network can bring intuition into repetition which can be used to predict protein functions [5, 6]. Furthermore, regulation approaches for contagious diseases generally rely on graph theoretic networks [7]. Schnitzler and Grass investigated initial analysis of neurological [8].The obtained results are applied for decision control measures [9]. Kucharski et al. [10] investigated the fluctuations in transmission rates to analyze the efficiency of the control measures. Roosa et al. [11] illustrated phenomenological models to anticipate the dynamic of COVID-19. In [12], artificial intelligence approach is presented to find the top-quality prognostic models for the investigation of infectious diseases. Wan et al. [13] estimated risk-recognition for doubtful COVID-19 cases with the help of the graph embedding method. These complex networks have key role in communication systems, Internet, the World Wide Web, environment, and public health. Due to the extensive applications of complex networks, epidemiological and ecological researchers have chased their consideration to network analysis.A tree in which one vertex has been nominated as the root and each edge is extended away from root is known as hyper tree. Different biological organisms like DNA sequences or different species could be represented by the vertices of a rooted tree. Aforementioned rooted trees of biological concern are termed as evolutionary trees of phytogenetic trees. A hypertree is a network topology and is a mixture of the hypercube concept and the binary tree. Artificial intelligence and machine learning approaches have demonstrated that when contact tracing is comprehensively exercised, one can alleviate the outbreak of the pandemic by cracking the existing sequence of spread of the coronavirus and consequently supporting to decrease the rate of current epidemic [14].ConsiderG=GV,GE be a graph in which GV and GE are used to represent the vertex set and the edge set of G, respectively. The degree of any vertex l is termed as the number of edges associated to it and is denoted by ℘l. The maximum distance between l and any other vertex of G is termed as eccentricity of l and is denoted by ϱl. Also, if lm∈GE, then ℘l and ℘m denote the degrees of vertex l and m, respectively. In QSPR/QSAR studies, a lot of molecular descriptors are employed to correlate different biological and physico-chemical activities. In this study, we will talk about some eccentricity-based and degree-based indices.Uncertainty is prevailing. It turns up as a consequence of insufficient information than the whole information required to identify its circumferences. In 1948, Shannon [15] established a criterion to guess the uncertainty identified as entropy. The entropy measure has identified comprehensive employment in physical sciences [16]. In the literature, numerous graph entropies are estimated by eccentricity of the vertices and characteristic polynomials [17]. Manzoor et al. talked about few relations between the complexity of graphs and Hosoya entropy [18, 19].In 2014, Chen et al. [17] established the description of the entropy in equation (1) as follows:(1)ENTψG=−∑l′m′∈GEψl′m′∑lm∈GEψlmlogψl′m′∑lm∈GEψlm.Also, the compact form of some eccentricity-based topological indices is depicted in Table1, and some degree-based topological indices are depicted in Table 2.Table 1
Eccentricity-based topological indices along with their respective edge weightψlm of the edge lm.
Eccentricity-based topological indicesEdge weightψlm of the edge lmEntropiesThe fourth geometric arithmetic eccentricity index [20]2ϱlϱm/ϱl+ϱmThe fourth geometric arithmetic eccentricity entropyThe first Zagreb eccentric index [20]ϱl+ϱmThe first Zagreb eccentric entropyThe second Zagreb eccentric index [20]ϱl⋅ϱmThe second Zagreb eccentric entropyEccentric atom bond connectivity index [21]ϱl+ϱm−2/ϱl×ϱmEccentric atom bond connectivity entropyTable 2
Degree-based topological indices along with their respective edge weightψlm of the edge lm.
Degree-based topological indicesEdge weightψlm of the edge lmEntropiesThe hyper Zagreb index [22]℘l+℘m2The hyper Zagreb entropy [23–25]The forgotten index [26]℘l2+℘m2The forgotten entropy [23–25]The atom bond connectivity index [27]℘l+℘m−2/℘l×℘mThe atom bond connectivity entropy [19, 23, 24]


## 2. Methodology

To enumerate our findings, we will exert the approach of combinatorial computing, edge partition technique, analytic methods, degree enumerating technique, and graph theoretic tools. Additionally, we will utilize Matlab and maple software for mathematical computing. For plotting our obtained results, we will use Microsoft Excel.


## 3. Structure of Complete Hypertree

A complete binary tree is termed as hypertree; we will denote it byCBTt with t levels where level k, 0≤k≤t, includes 2k vertices. The vertices of CBTt are designated in the following way: the label of root node is 1 and it is at level 0. For any vertex l, the children of l are tagged with 2l and 2l+1 [28]. In a hypertree, extra edges are horizontal, where in the same level k, 1≤k≤t, any two vertices are attached by an edge (see Figure 1). Consider the hypertree CBT3 in Figure 1 (see [28]) as an illustration to deduce distinct topological indices and their respective entropies. To demonstrate our main findings, we form a partition of edges of the hypertree CBTt for t levels established on eccentricity of end vertices in Tables 3 and 4 representing the edge partition of CBTt.Figure 1
An illustration of the hypertreeCBTt for t=3 levels [28].Table 3
Edge partition ofCBTt for t-levels.
ϱl,ϱmNumber of repetitionRange oft and kt,t3t≥3t+k−1,t+k2k+1t≥3, 1≤k≤t−1t+k,t+k2kt≥3, 1≤k≤t−1Table 4
Edge partition ofCBTt with t-levels.
℘l,℘mNumber of repetitionKinds of edges2,22t−1E12,42E24,22tE34,42t+1−2t−1−5E4The quantitative structure activity relationship research of dendrimers could then be assisted by the distinct topological indices and their respective entropies acquired in this study for hypertrees [29]. In addition, current development of topological indices examined in [30] has substantial consequences in complex networks of material and molecular systems in which larger atoms and many other huge elements are presented [31]. For such systems, the relativistic consequences are very significant.


### 3.1. Eccentricity-Based Entropies ofCBTt

In this segment, we measure the eccentricity-based entropies of the complete hypertreeCBTt.


#### 3.1.1. The Fourth Geometric Arithmetic Eccentric Entropy

Now, using Tables1 and 3, the fourth geometric arithmetic eccentric index is calculated in [28] as follows:(2)GA4CBT=1+2t+∑k=1t−12k+2t2+k2+2tk−t−k2t+k−1.We computedENTGA4 as follows:(3)ENTGA4CBT=logGA4−1GA4∑i=13∑lm∈EiCBT2ϱlϱmϱl+ϱmlog2ϱlϱmϱl+ϱm,ENTGA4CBTt=log1+2t+∑k=1t−12k+2−t+2tk+t2+k2−k2t+k−1−∑k=1t−12k+2t2+k2+2tk−t−k/2t+k−1log∑k=1t−12k+2t2+k2+2tk−t−k/2t+k−11+2t+∑k=1t−12k+2t2+k2+2tk−t−k/2t+k−1.


#### 3.1.2. The First Zagreb Eccentric Entropy

The first Zagreb eccentric index by using Tables1 and 3 is calculated in [28] as follows:(4)MM1CBT=12t−14×2t−6t+16.We computedENTMM1 as follows:(5)ENTMM1CBT=logMM1−1MM1∑i=13∑lm∈EiCBTϱl+ϱmlogϱl+ϱm,ENTMM1CBT=log12t−14×2t−6t+16−6tlog2t12t−14×2t−6t+16−∑k=1t−12k+12k+2t−1log∑k=1t−12k+2t−112t−14×2t−6t+16−∑k=1t−12k2k=2tlog∑k=1t−12k+2t12t−14×2t−6t+16=log12t−14×2t−6t+16−6tlog2t12t−14×2t−6t+16−8t−102t−8t+12log3t2−4t+112t−14×2t−6t+16−4t−42t−4t+4log3t/2t−112t−14×2t−6t+16.


#### 3.1.3. The Second Zagreb Eccentric Entropy

The second Zagreb eccentric index by using Tables1 and 3 is calculated in [28] as follows:(6)MM2CBT=12t2−28t+22×2t−3t2+16t−22.We computedENTMM2 as follows:(7)ENTMM2CBT=logMM2−1MM2∑i=13∑lm∈EiCBTϱl+ϱmlogϱl+ϱm,ENTMM2CBTt=log12t2−28t+22×2t−3t2+16t−22−3t2logt212t2−28t+22×2t−3t2+16t−22−∑k=1t−12k+1t2+k2+2tk−t−klog∑k=1t−1t2+k2+2tk−t−k12t2−28t+22×2t−3t2+16t−22−∑k=1t−12kt+k2log∑k=1t−1t+k212t2−28t+22×2t−3t2+16t−22=log12t2−28t+22×2t−3t2+16t−22−3t2logt212t2−28t+22×2t−3t2+16t−22−8t2−20t+162t−4t2+12t−16log7/3t3−4t2+5/3t12t2−28t+22×2t−3t2+16t−22−4t2−8t+62t−2t2+4t−6log7/3t3−5/2t2+1/6t12t2−28t+22×2t−3t2+16t−22.


#### 3.1.4. Eccentric Atom Bond Connectivity Entropy

The eccentric atom bond connectivity index by using Tables1 and 3 is calculated in [28] as follows:(8)ABC5CBT=32t−2t+∑k=1t−12k+12t+2k−3t+k−1t+k+∑k=1t−12k2t+k−2t+k.We computedENTABC5 as follows:(9)ENTABC5CBT=logABC5−1ABC5∑i=13∑lm∈EiCBTϱl+ϱm−2ϱl×ϱmlogϱl+ϱm−2ϱl×ϱm,ENTABC5CBTt=log32t−2t+∑k=1t−12k+12t+2k−3t+k−1t+k+∑k=1t−12k2t+k−2t+k−32t−2/tlog2t−2/t32t−2/t+∑k=1t−12k+12t+2k−3/t2+k2+2tk−t−k+∑k=1t−12k2t+k−2/t+k−∑k=1t−12k+12t+2k−3/t2+k2+2tk−t−klog∑k=1t−12t+2k−3/t2+k2+2tk−t−k32t−2/t+∑k=1t−12k+12t+2k−3/t2+k2+2tk−t−k+∑k=1t−12k2t+k−2/t+k−∑k=1t−12k2t+k−2/t+klog∑k=1t−12t+k−2/t+k32t−2/t+∑k=1t−12k+12t+2k−3/t2+k2+2tk−t−k+∑k=1t−12k2t+k−2/t+k.


### 3.2. Degree-Based Entropies ofCBTt

In this segment, we measure the degree-based entropies of the hypertreeCBTt.


#### 3.2.1. The Hyper Zagreb Entropy

Now, using Tables1 and 4, the hyper Zagreb index is calculated in [28] as follows:(10)HMCBT=104×2t−248.We computedENTHM as follows:(11)ENTHMCBT=logHM−1HM∑i=14∑lm∈EiCBT℘l+℘m2log℘l+℘m2,ENTHMCBTt=log104×2t−248−2t+3log16104×2t−248−362+2tlog36104×2t−248−2t+7−2t+5−320log64104×2t−248.


#### 3.2.2. The Forgotten Entropy

Now, using Tables1 and 4, the forgotten index is calculated in [28] as follows:(12)FCBT=76×2t−120.We computedENTF as follows:(13)ENTFCBT=logF−1F∑i=14∑lm∈EiCBT℘l2+℘m2log℘l2+℘m2,ENTFCBT=log76×2t−120−2t+3log876×2t−120−40+2tlog2076×2t−120−2t+6−2t+4−160log6476×2t−120.


#### 3.2.3. The Atom Bond Connectivity Entropy

Now, using Tables1 and 4, the atom bond connectivity index is calculated in [28] as follows:(14)ABCCBT=324+3682t+21−534.We computedENTABC as follows:(15)ENTABCCBT=logABC−1ABC∑i=14∑lm∈EiCBT℘l+℘m−2℘l×℘mlog℘l+℘m−2℘l×℘m,ENTABCCBT=log324+3682t+21−534−2t+2t−1+2log1/232/4+36/82t+21−53/4−2t+1−2t−1−5log6/432/4+36/82t+21−53/4.


## 3.1. Eccentricity-Based Entropies ofCBTt

In this segment, we measure the eccentricity-based entropies of the complete hypertreeCBTt.


### 3.1.1. The Fourth Geometric Arithmetic Eccentric Entropy

Now, using Tables1 and 3, the fourth geometric arithmetic eccentric index is calculated in [28] as follows:(2)GA4CBT=1+2t+∑k=1t−12k+2t2+k2+2tk−t−k2t+k−1.We computedENTGA4 as follows:(3)ENTGA4CBT=logGA4−1GA4∑i=13∑lm∈EiCBT2ϱlϱmϱl+ϱmlog2ϱlϱmϱl+ϱm,ENTGA4CBTt=log1+2t+∑k=1t−12k+2−t+2tk+t2+k2−k2t+k−1−∑k=1t−12k+2t2+k2+2tk−t−k/2t+k−1log∑k=1t−12k+2t2+k2+2tk−t−k/2t+k−11+2t+∑k=1t−12k+2t2+k2+2tk−t−k/2t+k−1.


### 3.1.2. The First Zagreb Eccentric Entropy

The first Zagreb eccentric index by using Tables1 and 3 is calculated in [28] as follows:(4)MM1CBT=12t−14×2t−6t+16.We computedENTMM1 as follows:(5)ENTMM1CBT=logMM1−1MM1∑i=13∑lm∈EiCBTϱl+ϱmlogϱl+ϱm,ENTMM1CBT=log12t−14×2t−6t+16−6tlog2t12t−14×2t−6t+16−∑k=1t−12k+12k+2t−1log∑k=1t−12k+2t−112t−14×2t−6t+16−∑k=1t−12k2k=2tlog∑k=1t−12k+2t12t−14×2t−6t+16=log12t−14×2t−6t+16−6tlog2t12t−14×2t−6t+16−8t−102t−8t+12log3t2−4t+112t−14×2t−6t+16−4t−42t−4t+4log3t/2t−112t−14×2t−6t+16.


### 3.1.3. The Second Zagreb Eccentric Entropy

The second Zagreb eccentric index by using Tables1 and 3 is calculated in [28] as follows:(6)MM2CBT=12t2−28t+22×2t−3t2+16t−22.We computedENTMM2 as follows:(7)ENTMM2CBT=logMM2−1MM2∑i=13∑lm∈EiCBTϱl+ϱmlogϱl+ϱm,ENTMM2CBTt=log12t2−28t+22×2t−3t2+16t−22−3t2logt212t2−28t+22×2t−3t2+16t−22−∑k=1t−12k+1t2+k2+2tk−t−klog∑k=1t−1t2+k2+2tk−t−k12t2−28t+22×2t−3t2+16t−22−∑k=1t−12kt+k2log∑k=1t−1t+k212t2−28t+22×2t−3t2+16t−22=log12t2−28t+22×2t−3t2+16t−22−3t2logt212t2−28t+22×2t−3t2+16t−22−8t2−20t+162t−4t2+12t−16log7/3t3−4t2+5/3t12t2−28t+22×2t−3t2+16t−22−4t2−8t+62t−2t2+4t−6log7/3t3−5/2t2+1/6t12t2−28t+22×2t−3t2+16t−22.


### 3.1.4. Eccentric Atom Bond Connectivity Entropy

The eccentric atom bond connectivity index by using Tables1 and 3 is calculated in [28] as follows:(8)ABC5CBT=32t−2t+∑k=1t−12k+12t+2k−3t+k−1t+k+∑k=1t−12k2t+k−2t+k.We computedENTABC5 as follows:(9)ENTABC5CBT=logABC5−1ABC5∑i=13∑lm∈EiCBTϱl+ϱm−2ϱl×ϱmlogϱl+ϱm−2ϱl×ϱm,ENTABC5CBTt=log32t−2t+∑k=1t−12k+12t+2k−3t+k−1t+k+∑k=1t−12k2t+k−2t+k−32t−2/tlog2t−2/t32t−2/t+∑k=1t−12k+12t+2k−3/t2+k2+2tk−t−k+∑k=1t−12k2t+k−2/t+k−∑k=1t−12k+12t+2k−3/t2+k2+2tk−t−klog∑k=1t−12t+2k−3/t2+k2+2tk−t−k32t−2/t+∑k=1t−12k+12t+2k−3/t2+k2+2tk−t−k+∑k=1t−12k2t+k−2/t+k−∑k=1t−12k2t+k−2/t+klog∑k=1t−12t+k−2/t+k32t−2/t+∑k=1t−12k+12t+2k−3/t2+k2+2tk−t−k+∑k=1t−12k2t+k−2/t+k.


## 3.1.1. The Fourth Geometric Arithmetic Eccentric Entropy

Now, using Tables1 and 3, the fourth geometric arithmetic eccentric index is calculated in [28] as follows:(2)GA4CBT=1+2t+∑k=1t−12k+2t2+k2+2tk−t−k2t+k−1.We computedENTGA4 as follows:(3)ENTGA4CBT=logGA4−1GA4∑i=13∑lm∈EiCBT2ϱlϱmϱl+ϱmlog2ϱlϱmϱl+ϱm,ENTGA4CBTt=log1+2t+∑k=1t−12k+2−t+2tk+t2+k2−k2t+k−1−∑k=1t−12k+2t2+k2+2tk−t−k/2t+k−1log∑k=1t−12k+2t2+k2+2tk−t−k/2t+k−11+2t+∑k=1t−12k+2t2+k2+2tk−t−k/2t+k−1.


## 3.1.2. The First Zagreb Eccentric Entropy

The first Zagreb eccentric index by using Tables1 and 3 is calculated in [28] as follows:(4)MM1CBT=12t−14×2t−6t+16.We computedENTMM1 as follows:(5)ENTMM1CBT=logMM1−1MM1∑i=13∑lm∈EiCBTϱl+ϱmlogϱl+ϱm,ENTMM1CBT=log12t−14×2t−6t+16−6tlog2t12t−14×2t−6t+16−∑k=1t−12k+12k+2t−1log∑k=1t−12k+2t−112t−14×2t−6t+16−∑k=1t−12k2k=2tlog∑k=1t−12k+2t12t−14×2t−6t+16=log12t−14×2t−6t+16−6tlog2t12t−14×2t−6t+16−8t−102t−8t+12log3t2−4t+112t−14×2t−6t+16−4t−42t−4t+4log3t/2t−112t−14×2t−6t+16.


## 3.1.3. The Second Zagreb Eccentric Entropy

The second Zagreb eccentric index by using Tables1 and 3 is calculated in [28] as follows:(6)MM2CBT=12t2−28t+22×2t−3t2+16t−22.We computedENTMM2 as follows:(7)ENTMM2CBT=logMM2−1MM2∑i=13∑lm∈EiCBTϱl+ϱmlogϱl+ϱm,ENTMM2CBTt=log12t2−28t+22×2t−3t2+16t−22−3t2logt212t2−28t+22×2t−3t2+16t−22−∑k=1t−12k+1t2+k2+2tk−t−klog∑k=1t−1t2+k2+2tk−t−k12t2−28t+22×2t−3t2+16t−22−∑k=1t−12kt+k2log∑k=1t−1t+k212t2−28t+22×2t−3t2+16t−22=log12t2−28t+22×2t−3t2+16t−22−3t2logt212t2−28t+22×2t−3t2+16t−22−8t2−20t+162t−4t2+12t−16log7/3t3−4t2+5/3t12t2−28t+22×2t−3t2+16t−22−4t2−8t+62t−2t2+4t−6log7/3t3−5/2t2+1/6t12t2−28t+22×2t−3t2+16t−22.


## 3.1.4. Eccentric Atom Bond Connectivity Entropy

The eccentric atom bond connectivity index by using Tables1 and 3 is calculated in [28] as follows:(8)ABC5CBT=32t−2t+∑k=1t−12k+12t+2k−3t+k−1t+k+∑k=1t−12k2t+k−2t+k.We computedENTABC5 as follows:(9)ENTABC5CBT=logABC5−1ABC5∑i=13∑lm∈EiCBTϱl+ϱm−2ϱl×ϱmlogϱl+ϱm−2ϱl×ϱm,ENTABC5CBTt=log32t−2t+∑k=1t−12k+12t+2k−3t+k−1t+k+∑k=1t−12k2t+k−2t+k−32t−2/tlog2t−2/t32t−2/t+∑k=1t−12k+12t+2k−3/t2+k2+2tk−t−k+∑k=1t−12k2t+k−2/t+k−∑k=1t−12k+12t+2k−3/t2+k2+2tk−t−klog∑k=1t−12t+2k−3/t2+k2+2tk−t−k32t−2/t+∑k=1t−12k+12t+2k−3/t2+k2+2tk−t−k+∑k=1t−12k2t+k−2/t+k−∑k=1t−12k2t+k−2/t+klog∑k=1t−12t+k−2/t+k32t−2/t+∑k=1t−12k+12t+2k−3/t2+k2+2tk−t−k+∑k=1t−12k2t+k−2/t+k.


## 3.2. Degree-Based Entropies ofCBTt

In this segment, we measure the degree-based entropies of the hypertreeCBTt.


### 3.2.1. The Hyper Zagreb Entropy

Now, using Tables1 and 4, the hyper Zagreb index is calculated in [28] as follows:(10)HMCBT=104×2t−248.We computedENTHM as follows:(11)ENTHMCBT=logHM−1HM∑i=14∑lm∈EiCBT℘l+℘m2log℘l+℘m2,ENTHMCBTt=log104×2t−248−2t+3log16104×2t−248−362+2tlog36104×2t−248−2t+7−2t+5−320log64104×2t−248.


### 3.2.2. The Forgotten Entropy

Now, using Tables1 and 4, the forgotten index is calculated in [28] as follows:(12)FCBT=76×2t−120.We computedENTF as follows:(13)ENTFCBT=logF−1F∑i=14∑lm∈EiCBT℘l2+℘m2log℘l2+℘m2,ENTFCBT=log76×2t−120−2t+3log876×2t−120−40+2tlog2076×2t−120−2t+6−2t+4−160log6476×2t−120.


### 3.2.3. The Atom Bond Connectivity Entropy

Now, using Tables1 and 4, the atom bond connectivity index is calculated in [28] as follows:(14)ABCCBT=324+3682t+21−534.We computedENTABC as follows:(15)ENTABCCBT=logABC−1ABC∑i=14∑lm∈EiCBT℘l+℘m−2℘l×℘mlog℘l+℘m−2℘l×℘m,ENTABCCBT=log324+3682t+21−534−2t+2t−1+2log1/232/4+36/82t+21−53/4−2t+1−2t−1−5log6/432/4+36/82t+21−53/4.


## 3.2.1. The Hyper Zagreb Entropy

Now, using Tables1 and 4, the hyper Zagreb index is calculated in [28] as follows:(10)HMCBT=104×2t−248.We computedENTHM as follows:(11)ENTHMCBT=logHM−1HM∑i=14∑lm∈EiCBT℘l+℘m2log℘l+℘m2,ENTHMCBTt=log104×2t−248−2t+3log16104×2t−248−362+2tlog36104×2t−248−2t+7−2t+5−320log64104×2t−248.


## 3.2.2. The Forgotten Entropy

Now, using Tables1 and 4, the forgotten index is calculated in [28] as follows:(12)FCBT=76×2t−120.We computedENTF as follows:(13)ENTFCBT=logF−1F∑i=14∑lm∈EiCBT℘l2+℘m2log℘l2+℘m2,ENTFCBT=log76×2t−120−2t+3log876×2t−120−40+2tlog2076×2t−120−2t+6−2t+4−160log6476×2t−120.


## 3.2.3. The Atom Bond Connectivity Entropy

Now, using Tables1 and 4, the atom bond connectivity index is calculated in [28] as follows:(14)ABCCBT=324+3682t+21−534.We computedENTABC as follows:(15)ENTABCCBT=logABC−1ABC∑i=14∑lm∈EiCBT℘l+℘m−2℘l×℘mlog℘l+℘m−2℘l×℘m,ENTABCCBT=log324+3682t+21−534−2t+2t−1+2log1/232/4+36/82t+21−53/4−2t+1−2t−1−5log6/432/4+36/82t+21−53/4.


## 4. Corona Product of Complete Hypertree and a PathCBTt⊙Pn

LetG˜1=n1,m1 and G˜2=n2,m2 be two graphs, then corona product of these graphs is outlined as the graph acquired by picking one copy of G˜1 and n1 copies of G˜2 and afterwards associating the ith vertex of G˜1 with an edge to each vertex in the ith copy of G˜2. It develops from the description of the corona product of two graphs that VG˜1⊙G˜2=n1n2+1 and EG˜1⊙G˜2=m1+n1m2+n2 (see details in [28, 32]). It is noted that corona product of two graphs is no commutative. We demonstrate the corona product of hypertree CBTt and path Pn for t=3 and n=3 in Figure 2.Figure 2
Depiction of corona product of complete hypertree and pathCBT3⊙P3[28].Consider the corona product of complete hypertree and pathCBT3⊙P3 in Figure 2 as an illustration to deduce different topological indices and their respective entropies. To describe our main findings, we form a partition of edges of the corona product of hypertree and path CBTt⊙Pn for t,n≥2 established on eccentricity of end vertices in seven sets shown in Tables 5 and 6 representing the edge partition of CBTt⊙Pn. Also, if lm∈GE, then ℘l and ℘m denote the degrees of vertex l and m, respectively.Table 5
Edge partition ofCBTt⊙Pn grounded on eccentricity of end vertices of every edge, n≥2.
ϱl,ϱmFrequencyRange oft and kt+1,t+13t≥2t+k,t+k+12+n2k1≤k≤t−1, t≥22t,2t+12t×n1≤k≤t−1, t≥2t+1,t+2n1≤k≤t−1, t≥2t+k+1,t+k+1n−12k1≤k≤t, t≥2t+k+1,t+k+12k1≤k≤t−1, t≥2t+2,t+2n−1t≥2Table 6
Edge partition ofCBTt⊙Pn for t,n≥2.
℘l,℘mFrequencyTypes of edgesn+2,n+22t−1E1n+2,n+42+2tE2n+4,n+42t−1−1+∑j=1t−22j+1E3n+2,222t+1E4n+2,3n−22t+1E5n+4,2∑j=1t−12j+1E6n+4,3n−2∑j=1t−12jE72,32t+2−2E83,3n−32t−1E9


### 4.1. Eccentricity-Based Entropies ofCBTt⊙Pn

In this segment, we measure the eccentricity-based entropies of the corona product of hypertree and a pathCBTt⊙Pn.


#### 4.1.1. The Fourth Geometric Arithmetic Eccentric Entropy

Now, using Tables1 and 5, the fourth geometric arithmetic eccentric index is as follows:(16)5GA4CBTt⊙Pn=2t+n+n−12t+1−2+2nt2+3t+22t+3+n×2t+14t2+2t4t+1+n+2∑k=1t−12k+1t+k2+t+k2t+k+1.We computedENTGA4 as follows:(17)ENTGA4CBTt⊙Pn=logGA4−1GA4∑i=17∑lm∈EiCBTt⊙Pn2ϱlϱmϱl+ϱmlog2ϱlϱmϱl+ϱmENTGA4CBTt⊙Pn=logGA4−n+2GA4∑k=1t−12k+1t2+k2+2tk+t+k2t+k+1log∑k=1t−12t2+k2+2tk+t+k2t+k+1−n×2t+14t2+2tGA44t+1log24t2+2t4t+1−2nt+1t+2GA42t+3log2t+1t+22t+3.


#### 4.1.2. The First Zagreb Eccentric Entropy

The first Zagreb eccentric index by using Tables1 and 5 is calculated in [28] as follows:(18)MM1CBTt⊙Pn=16nt+4t−2n−8×2t−4nt+9n−4t+6.We computedENTMM1 as follows:(19)ENTMM1CBTt⊙Pn=logMM1−1MM1∑i=17∑lm∈EiCBTt⊙Pnϱl+ϱmlogϱl+ϱm,ENTMM1CBTt⊙Pn=log16nt+4t−2n−8×2t−4nt+9n−4t+6−6t+1log2t+2MM1−n+2MM14t−32t+2−4tlog3t2−2t−1−n×2tMM14t+1log4t+1−n2t+3MM1log2t+3−n−1MM18t×2t−4tlogt+12+2tt+1−t−1−4t−22t−4tMM1log3t2−t−2−n−1MM12t+4log2t+4.


#### 4.1.3. The Second Zagreb Eccentric Entropy

The second Zagreb eccentric index by using Tables1 and 5 is calculated in [28] as follows:(20)MM2CBTt⊙Pn=16nt2−4nt+4t2+8n−16t+72t−2nt3+9nt−2t2−2n+6t−9.We computedENTMM2 as follows:(21)ENTMM2CBTt⊙Pn=logMM2−1MM2∑i=17∑lm∈EiCBTt⊙Pnϱl×ϱmlogϱl×ϱm,ENTMM2CBTt⊙Pn=logMM2−3t+12MM2logt+12−n×2t+1MM22t2+tlog4t2+2t−2+nMM24t2−6t+42t−2t2+2t−4log7t33−4t3−t2−n−1MM2t+22logt+22−nt2+3t+2MM2logt2+3t−n−1MM28t2+42t−2t2−4log73t3+92t2+132t−1MM24t2−4t+32t−2t2−4log73t3+12t2−116t−1.


#### 4.1.4. Eccentric Atom Bond Connectivity Entropy

The eccentric atom bond connectivity index by using Tables1 and 5 is calculated in [28] as follows:(22)ABC5CBTt⊙Pn=32tt+1+2+n∑k=1t−12k2t+2k−1t2+k2+2tk+t+k+n×2t4t−14t2+2t+n×2t+1t2+3t+2+n−1∑k=1t2k2k+2tt+k+1+∑k=1t−12k2k+2tt+k+1+n−12t+2t+2.We computedENTABC5 as follows:(23)ENTABC5CBTt⊙Pn=logABC5−1ABC5∑i=17∑lm∈EiCBTt⊙Pnϱl+ϱm−2ϱl×ϱmlogϱl+ϱm−2ϱl×ϱm,ENTABC5CBTt⊙Pn=logABC5−3ABC52tt+1log2tt+1−4⋅2tABC5⋅4t−14t2+2tlog4t−14t2+2t−2+nABC5∑k=1t−12k2t+2k−1t2+k2+2tk+t+klog∑k=1t−12t+2k−1t2+k2+2tk+t+k−nABC52t+1t2+3t+2log2t+1t2+3t+2−n−1ABC5∑k=1t2k2k+2tt+k+1log∑k=1t2k+2tt+k+1−1ABC5∑k=1t−12k2k+2tt+k+1log∑k=1t−12k+2tt+k+1−n−1ABC5⋅2t+2t+2log2t+2t+2.


### 4.2. Degree-Based Entropies ofCBTt⊙Pn

In this segment, we measure the degree-based entropies of the corona product of hypertree and pathCBTt⊙Pn.


#### 4.2.1. The Hyper Zagreb Entropy

Now, using Tables1 and 6, the hyper Zagreb index is as follows:(24)HMCBTt⊙Pn=2n3+34n2+185n−662t−n3−26n2−199n+32.We computedENTHM as follows:(25)ENTHMCBTt⊙Pn=logHM−1HM∑i=19∑lm∈EiCBTt⊙Pn℘l+℘m2log℘l+℘m2,ENTHMCBTt⊙Pn=logHM−2t−1HM2n+42log2n+42−2+2tHM2n+62log2n+62−2n+82HM2t−1−1∑j=1t−22j+1log2n+82−n+42HM2t+1+2logn+42−n+52HMn−22t+1logn+52−n+62HM2t+1−4logn+62−n+72HMn−22t−2logn+72−252t+2−2HMlog25−36n−3HM2t+1−1log36.


#### 4.2.2. The Forgotten Entropy

Now, using Tables1 and 6, the forgotten index is as follows:(26)FCBTt⊙Pn=2n3+18n2+114n−42t−n3−18n2−111n−82.We computedENTF as follows:(27)ENTFCBTt⊙Pn=logF−1F∑i=19∑lm∈EiCBTt⊙Pn℘l2+℘m2log℘l2+℘m2,ENTFCBTt⊙Pn=logF−2tFn+22log2n+22−2+22F2n2+12n+20log2n2+12n+20−2n+42F2t−1−1+∑j=1t−12j+1log2n+42+2t+1+2Fn2+4n+8logn2+4n+8−2t+1Fn−2n2+4n+13logn2+4n+13−2t+1−4Fn2+8n+20logn2+8n+20−n−2F2t−2n2+8n+25logn2+8n+25−13F2t+2−2log13−18Fn−32t+1−1log18.


#### 4.2.3. The Atom Bond Connectivity Entropy

Now, using Tables1 and 6, the atom bond connectivity index is as follows:(28)ABCCBTt⊙Pn=2t−1⋅2n+2n+2+2+2t2n+4+2t−1+2t−52n+6n+4+122t+3−4+n−22t+1n+33n+6+n−22t−2n+53n+4+23n−32t+1−1.We computedENTABC as follows:(29)ENTABCCBTt⊙Pn=logABC−1ABC∑i=19∑lm∈EiCBTt⊙Pn℘l+℘m−2℘l×℘mlog℘l+℘m−2℘l×℘m,ENTABCCBTt⊙Pn=logABC−2t−1ABC⋅2n+2n+2log2n+2n+2−2+2tABC⋅2n+4log2n+4−2t−1+2t−5ABC⋅2n+6n+4log2n+6n+4−2t+3−42ABClog12−2n−32t+1−13ABClog23−n−22t+1ABC⋅n+33n+6logn+33n+6−n−22t−2ABC⋅n+53n+4logn+53n+4.


## 4.1. Eccentricity-Based Entropies ofCBTt⊙Pn

In this segment, we measure the eccentricity-based entropies of the corona product of hypertree and a pathCBTt⊙Pn.


### 4.1.1. The Fourth Geometric Arithmetic Eccentric Entropy

Now, using Tables1 and 5, the fourth geometric arithmetic eccentric index is as follows:(16)5GA4CBTt⊙Pn=2t+n+n−12t+1−2+2nt2+3t+22t+3+n×2t+14t2+2t4t+1+n+2∑k=1t−12k+1t+k2+t+k2t+k+1.We computedENTGA4 as follows:(17)ENTGA4CBTt⊙Pn=logGA4−1GA4∑i=17∑lm∈EiCBTt⊙Pn2ϱlϱmϱl+ϱmlog2ϱlϱmϱl+ϱmENTGA4CBTt⊙Pn=logGA4−n+2GA4∑k=1t−12k+1t2+k2+2tk+t+k2t+k+1log∑k=1t−12t2+k2+2tk+t+k2t+k+1−n×2t+14t2+2tGA44t+1log24t2+2t4t+1−2nt+1t+2GA42t+3log2t+1t+22t+3.


### 4.1.2. The First Zagreb Eccentric Entropy

The first Zagreb eccentric index by using Tables1 and 5 is calculated in [28] as follows:(18)MM1CBTt⊙Pn=16nt+4t−2n−8×2t−4nt+9n−4t+6.We computedENTMM1 as follows:(19)ENTMM1CBTt⊙Pn=logMM1−1MM1∑i=17∑lm∈EiCBTt⊙Pnϱl+ϱmlogϱl+ϱm,ENTMM1CBTt⊙Pn=log16nt+4t−2n−8×2t−4nt+9n−4t+6−6t+1log2t+2MM1−n+2MM14t−32t+2−4tlog3t2−2t−1−n×2tMM14t+1log4t+1−n2t+3MM1log2t+3−n−1MM18t×2t−4tlogt+12+2tt+1−t−1−4t−22t−4tMM1log3t2−t−2−n−1MM12t+4log2t+4.


### 4.1.3. The Second Zagreb Eccentric Entropy

The second Zagreb eccentric index by using Tables1 and 5 is calculated in [28] as follows:(20)MM2CBTt⊙Pn=16nt2−4nt+4t2+8n−16t+72t−2nt3+9nt−2t2−2n+6t−9.We computedENTMM2 as follows:(21)ENTMM2CBTt⊙Pn=logMM2−1MM2∑i=17∑lm∈EiCBTt⊙Pnϱl×ϱmlogϱl×ϱm,ENTMM2CBTt⊙Pn=logMM2−3t+12MM2logt+12−n×2t+1MM22t2+tlog4t2+2t−2+nMM24t2−6t+42t−2t2+2t−4log7t33−4t3−t2−n−1MM2t+22logt+22−nt2+3t+2MM2logt2+3t−n−1MM28t2+42t−2t2−4log73t3+92t2+132t−1MM24t2−4t+32t−2t2−4log73t3+12t2−116t−1.


### 4.1.4. Eccentric Atom Bond Connectivity Entropy

The eccentric atom bond connectivity index by using Tables1 and 5 is calculated in [28] as follows:(22)ABC5CBTt⊙Pn=32tt+1+2+n∑k=1t−12k2t+2k−1t2+k2+2tk+t+k+n×2t4t−14t2+2t+n×2t+1t2+3t+2+n−1∑k=1t2k2k+2tt+k+1+∑k=1t−12k2k+2tt+k+1+n−12t+2t+2.We computedENTABC5 as follows:(23)ENTABC5CBTt⊙Pn=logABC5−1ABC5∑i=17∑lm∈EiCBTt⊙Pnϱl+ϱm−2ϱl×ϱmlogϱl+ϱm−2ϱl×ϱm,ENTABC5CBTt⊙Pn=logABC5−3ABC52tt+1log2tt+1−4⋅2tABC5⋅4t−14t2+2tlog4t−14t2+2t−2+nABC5∑k=1t−12k2t+2k−1t2+k2+2tk+t+klog∑k=1t−12t+2k−1t2+k2+2tk+t+k−nABC52t+1t2+3t+2log2t+1t2+3t+2−n−1ABC5∑k=1t2k2k+2tt+k+1log∑k=1t2k+2tt+k+1−1ABC5∑k=1t−12k2k+2tt+k+1log∑k=1t−12k+2tt+k+1−n−1ABC5⋅2t+2t+2log2t+2t+2.


## 4.1.1. The Fourth Geometric Arithmetic Eccentric Entropy

Now, using Tables1 and 5, the fourth geometric arithmetic eccentric index is as follows:(16)5GA4CBTt⊙Pn=2t+n+n−12t+1−2+2nt2+3t+22t+3+n×2t+14t2+2t4t+1+n+2∑k=1t−12k+1t+k2+t+k2t+k+1.We computedENTGA4 as follows:(17)ENTGA4CBTt⊙Pn=logGA4−1GA4∑i=17∑lm∈EiCBTt⊙Pn2ϱlϱmϱl+ϱmlog2ϱlϱmϱl+ϱmENTGA4CBTt⊙Pn=logGA4−n+2GA4∑k=1t−12k+1t2+k2+2tk+t+k2t+k+1log∑k=1t−12t2+k2+2tk+t+k2t+k+1−n×2t+14t2+2tGA44t+1log24t2+2t4t+1−2nt+1t+2GA42t+3log2t+1t+22t+3.


## 4.1.2. The First Zagreb Eccentric Entropy

The first Zagreb eccentric index by using Tables1 and 5 is calculated in [28] as follows:(18)MM1CBTt⊙Pn=16nt+4t−2n−8×2t−4nt+9n−4t+6.We computedENTMM1 as follows:(19)ENTMM1CBTt⊙Pn=logMM1−1MM1∑i=17∑lm∈EiCBTt⊙Pnϱl+ϱmlogϱl+ϱm,ENTMM1CBTt⊙Pn=log16nt+4t−2n−8×2t−4nt+9n−4t+6−6t+1log2t+2MM1−n+2MM14t−32t+2−4tlog3t2−2t−1−n×2tMM14t+1log4t+1−n2t+3MM1log2t+3−n−1MM18t×2t−4tlogt+12+2tt+1−t−1−4t−22t−4tMM1log3t2−t−2−n−1MM12t+4log2t+4.


## 4.1.3. The Second Zagreb Eccentric Entropy

The second Zagreb eccentric index by using Tables1 and 5 is calculated in [28] as follows:(20)MM2CBTt⊙Pn=16nt2−4nt+4t2+8n−16t+72t−2nt3+9nt−2t2−2n+6t−9.We computedENTMM2 as follows:(21)ENTMM2CBTt⊙Pn=logMM2−1MM2∑i=17∑lm∈EiCBTt⊙Pnϱl×ϱmlogϱl×ϱm,ENTMM2CBTt⊙Pn=logMM2−3t+12MM2logt+12−n×2t+1MM22t2+tlog4t2+2t−2+nMM24t2−6t+42t−2t2+2t−4log7t33−4t3−t2−n−1MM2t+22logt+22−nt2+3t+2MM2logt2+3t−n−1MM28t2+42t−2t2−4log73t3+92t2+132t−1MM24t2−4t+32t−2t2−4log73t3+12t2−116t−1.


## 4.1.4. Eccentric Atom Bond Connectivity Entropy

The eccentric atom bond connectivity index by using Tables1 and 5 is calculated in [28] as follows:(22)ABC5CBTt⊙Pn=32tt+1+2+n∑k=1t−12k2t+2k−1t2+k2+2tk+t+k+n×2t4t−14t2+2t+n×2t+1t2+3t+2+n−1∑k=1t2k2k+2tt+k+1+∑k=1t−12k2k+2tt+k+1+n−12t+2t+2.We computedENTABC5 as follows:(23)ENTABC5CBTt⊙Pn=logABC5−1ABC5∑i=17∑lm∈EiCBTt⊙Pnϱl+ϱm−2ϱl×ϱmlogϱl+ϱm−2ϱl×ϱm,ENTABC5CBTt⊙Pn=logABC5−3ABC52tt+1log2tt+1−4⋅2tABC5⋅4t−14t2+2tlog4t−14t2+2t−2+nABC5∑k=1t−12k2t+2k−1t2+k2+2tk+t+klog∑k=1t−12t+2k−1t2+k2+2tk+t+k−nABC52t+1t2+3t+2log2t+1t2+3t+2−n−1ABC5∑k=1t2k2k+2tt+k+1log∑k=1t2k+2tt+k+1−1ABC5∑k=1t−12k2k+2tt+k+1log∑k=1t−12k+2tt+k+1−n−1ABC5⋅2t+2t+2log2t+2t+2.


## 4.2. Degree-Based Entropies ofCBTt⊙Pn

In this segment, we measure the degree-based entropies of the corona product of hypertree and pathCBTt⊙Pn.


### 4.2.1. The Hyper Zagreb Entropy

Now, using Tables1 and 6, the hyper Zagreb index is as follows:(24)HMCBTt⊙Pn=2n3+34n2+185n−662t−n3−26n2−199n+32.We computedENTHM as follows:(25)ENTHMCBTt⊙Pn=logHM−1HM∑i=19∑lm∈EiCBTt⊙Pn℘l+℘m2log℘l+℘m2,ENTHMCBTt⊙Pn=logHM−2t−1HM2n+42log2n+42−2+2tHM2n+62log2n+62−2n+82HM2t−1−1∑j=1t−22j+1log2n+82−n+42HM2t+1+2logn+42−n+52HMn−22t+1logn+52−n+62HM2t+1−4logn+62−n+72HMn−22t−2logn+72−252t+2−2HMlog25−36n−3HM2t+1−1log36.


### 4.2.2. The Forgotten Entropy

Now, using Tables1 and 6, the forgotten index is as follows:(26)FCBTt⊙Pn=2n3+18n2+114n−42t−n3−18n2−111n−82.We computedENTF as follows:(27)ENTFCBTt⊙Pn=logF−1F∑i=19∑lm∈EiCBTt⊙Pn℘l2+℘m2log℘l2+℘m2,ENTFCBTt⊙Pn=logF−2tFn+22log2n+22−2+22F2n2+12n+20log2n2+12n+20−2n+42F2t−1−1+∑j=1t−12j+1log2n+42+2t+1+2Fn2+4n+8logn2+4n+8−2t+1Fn−2n2+4n+13logn2+4n+13−2t+1−4Fn2+8n+20logn2+8n+20−n−2F2t−2n2+8n+25logn2+8n+25−13F2t+2−2log13−18Fn−32t+1−1log18.


### 4.2.3. The Atom Bond Connectivity Entropy

Now, using Tables1 and 6, the atom bond connectivity index is as follows:(28)ABCCBTt⊙Pn=2t−1⋅2n+2n+2+2+2t2n+4+2t−1+2t−52n+6n+4+122t+3−4+n−22t+1n+33n+6+n−22t−2n+53n+4+23n−32t+1−1.We computedENTABC as follows:(29)ENTABCCBTt⊙Pn=logABC−1ABC∑i=19∑lm∈EiCBTt⊙Pn℘l+℘m−2℘l×℘mlog℘l+℘m−2℘l×℘m,ENTABCCBTt⊙Pn=logABC−2t−1ABC⋅2n+2n+2log2n+2n+2−2+2tABC⋅2n+4log2n+4−2t−1+2t−5ABC⋅2n+6n+4log2n+6n+4−2t+3−42ABClog12−2n−32t+1−13ABClog23−n−22t+1ABC⋅n+33n+6logn+33n+6−n−22t−2ABC⋅n+53n+4logn+53n+4.


## 4.2.1. The Hyper Zagreb Entropy

Now, using Tables1 and 6, the hyper Zagreb index is as follows:(24)HMCBTt⊙Pn=2n3+34n2+185n−662t−n3−26n2−199n+32.We computedENTHM as follows:(25)ENTHMCBTt⊙Pn=logHM−1HM∑i=19∑lm∈EiCBTt⊙Pn℘l+℘m2log℘l+℘m2,ENTHMCBTt⊙Pn=logHM−2t−1HM2n+42log2n+42−2+2tHM2n+62log2n+62−2n+82HM2t−1−1∑j=1t−22j+1log2n+82−n+42HM2t+1+2logn+42−n+52HMn−22t+1logn+52−n+62HM2t+1−4logn+62−n+72HMn−22t−2logn+72−252t+2−2HMlog25−36n−3HM2t+1−1log36.


## 4.2.2. The Forgotten Entropy

Now, using Tables1 and 6, the forgotten index is as follows:(26)FCBTt⊙Pn=2n3+18n2+114n−42t−n3−18n2−111n−82.We computedENTF as follows:(27)ENTFCBTt⊙Pn=logF−1F∑i=19∑lm∈EiCBTt⊙Pn℘l2+℘m2log℘l2+℘m2,ENTFCBTt⊙Pn=logF−2tFn+22log2n+22−2+22F2n2+12n+20log2n2+12n+20−2n+42F2t−1−1+∑j=1t−12j+1log2n+42+2t+1+2Fn2+4n+8logn2+4n+8−2t+1Fn−2n2+4n+13logn2+4n+13−2t+1−4Fn2+8n+20logn2+8n+20−n−2F2t−2n2+8n+25logn2+8n+25−13F2t+2−2log13−18Fn−32t+1−1log18.


## 4.2.3. The Atom Bond Connectivity Entropy

Now, using Tables1 and 6, the atom bond connectivity index is as follows:(28)ABCCBTt⊙Pn=2t−1⋅2n+2n+2+2+2t2n+4+2t−1+2t−52n+6n+4+122t+3−4+n−22t+1n+33n+6+n−22t−2n+53n+4+23n−32t+1−1.We computedENTABC as follows:(29)ENTABCCBTt⊙Pn=logABC−1ABC∑i=19∑lm∈EiCBTt⊙Pn℘l+℘m−2℘l×℘mlog℘l+℘m−2℘l×℘m,ENTABCCBTt⊙Pn=logABC−2t−1ABC⋅2n+2n+2log2n+2n+2−2+2tABC⋅2n+4log2n+4−2t−1+2t−5ABC⋅2n+6n+4log2n+6n+4−2t+3−42ABClog12−2n−32t+1−13ABClog23−n−22t+1ABC⋅n+33n+6logn+33n+6−n−22t−2ABC⋅n+53n+4logn+53n+4.


## 5. Physical Interpretation of Computed Results

In QSPR/QSAR deliberations, topological indices are utilized to associate the biological functions of the frameworks with their substantial properties like distortion, strain energy, stability, and melting point [33]. These assessments can be executed by using degree-based indices because these indices have clarity of decision and rapidity [34]. In this section, we talked about some degree-based entropies. We proposed a new approach to estimate the entropy by estimating its topological indices. The forgotten and the hyper Zagreb indices are employed to form the physico-chemical characteristics such as density, volume, entropy, and acentric factor of the underlying structure [35]. The degree-based entropy can also be employed to structural chemistry, social network, biology, ecological networks, and national security. Entropy function is monotonic as in all situations. It can be viewed from Tables 7 and 8. These numerical tables show the behaviours of the computed results. The graphical representation of these results is observed in Figures 3 and 4.Table 7
Comparison of degree-based entropiesENTHM, ENTF, and ENTABC for CBTt.
tENTHMENTFENTABC22.12463.58421.908932.95124.06992.788343.71434.71453.564154.44185.39154.296465.15206.07825.008675.85366.76855.711186.55097.46036.40997.24628.15287.1044107.94048.84567.7987Table 8
Comparison of degree-based entropiesENTHM, ENTF, and ENTABC for CBTt⊙Pn.
n,tENTHMENTFENTABC2,23.24033.22633.39683,34.40334.16094.55764,45.37935.03225.56055,56.35776.01256.48376,67.25806.80997.36017,77.91937.60308.20588,88.71188.35019.03019,99.49119.06389.838610,1010.260910.037610.6349Figure 3
Comparison of entropies for hypertreeCBTt.Figure 4
Comparison of entropies for corona product of hypertree and a pathCBTt⊙Pn.Numerous employment of complex networks stranded on the entropy correlated with structural information were issued. In [36, 37], many algorithms were recommended to examine the structural complexity. However, the entropy approach is reviewed to be the most substantial approach to distinguish biological networks. Furthermore, eccentricity-based indices have vigorous role due to having the potential of computing pharmaceutical properties. Therefore, we have listed mathematically some eccentricity-based entropies for little considerations of parameters for CBTt and CBTt⊙Pn. Also, we produce tables with the help of Matlab for small estimations for eccentricity of CBTt and CBTt⊙Pn. From Tables 9 and 10, we can note that all the evaluation of entropy are in growing request as the values of parameters are expanded. The graphical representation of computed findings is demonstrated in Figures 5 and 6 for certain measurements of nandt.Table 9
Comparison of eccentricity-based entropiesENTGA4, ENTMM1, ENTMM2, and ENTABC5 for CBTt.
tENTGA4ENTMM1ENTMM2ENTABC532.65012.67312.44382.446843.12453.05462.85932.763253.63933.50723.34543.155064.18664.00743.87263.605174.75844.54014.42644.098385.34825.09594.99874.623495.95185.66895.58475.1722106.56616.25526.18155.7392117.18876.85206.78696.3204127.81827.45747.39956.9129Table 10
Comparison of eccentricity-based entropiesENTGA4, ENTMM1, ENTMM2, and ENTABC5 for CBTt⊙Pn.
n,tENTGA4ENTMM1ENTMM2ENTABC52,23.21733.01863.53773.26693,34.00583.5284.71793.97254,44.72344.0015.76494.65225,55.41104.46376.72675.33906,66.07904.91787.63286.03447,76.73185.36328.50126.73588,87.37165.80049.34277.44069,98.00046.229910.16448.191210,108.61976.652410.97098.8548Figure 5
Graphical comparison of eccentricity-based entropies for hypertreeCBTt.Figure 6
Graphical comparison of eccentricity-based entropies for corona product of hypertree and a pathCBTt⊙Pn.


## 6. Conclusion

In this paper, we have acquired some degree-based and eccentricity-based indices for the depiction of the specific graph theoretical system of biochemical concern. We have acquired aforementioned topological indices for severalt level hypertrees and corona product of hypertrees and path. We have also computed the respective entropies. These entropies associate particular physico-chemical characteristics like distortion, stability, melting points, and strain energy of chemical compounds. The mathematical findings for these graphs are helpful for the chemist to understand the biochemical utilization of these structures.



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