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Introduction

All graphs considered in this paper are finite, simple and undirected. In particular, these graphs do not have loops. Let G = (V, E) be a graph with the vertex set V(G) = {v1, v2, v3, ⋯, vn} and the edge set E(G) = {e1, e2, e3, ⋯, em}, that is |V(G)| = n and |E(G)| = m. The vertex u and v are adjacent if uvE(G). The open(closed) neighborhood of a vertex vV(G) is N(v) = {u : uvE(G)} and N[v] = N(v) ∪ {v} respectively. The degree of a vertex vV(G) is denoted by dG(v) and is defined as dG(v) = |N(v)|. A vertex vV(G) is pendant if |N(v)| = 1 and is called supporting vertex if it is adjacent to pendant vertex. Any vertex vV(G) with |N(v)| > 1 is called internal vertex. If dG(v) = r for every vertex vV(G), where r ∈ ℤ+ then G is called r-regular. If r = 2 then it is called cycle graph Cn and for r = 3 it is called the cubic graph. A graph G is unicyclic if |V| = |E|. A graph G is called a block graph, if every block in G is a complete graph. For undefined terminologies we refer the reader to [16].

A subset DV(G) is called dominating set if N[D] = V(G). The minimum cardinality of such a set D is called the domination number γ(G) of G. A dominating set D is connected if the subgraph induced by D is connected. The minimum cardinality of connected dominating set D is called the connected dominating number γc(G) of G [27].

The energy E(G) of a graph G is equal to the sum of the absolute values of the eigenvalues of the adjacency matrix of G. This quantity, introduced almost 30 years ago [13] and having a clear connection to chemical problems [15], has in newer times attracted much attention of mathematicians and mathematical chemists [3, 8, 9, 10, 11, 12, 20,22, 23, 24, 28, 30, 31].

In connection with energy (that is defined in terms of the eigenvalues of the adjacency matrix), energy-like quantities were considered also for the other matrices: Laplacian [15], distance [17], incidence [18], minimum covering energy [1] etc. Recall that a great variety of matrices has so far been associated with graphs [4, 5, 10, 29].

Recently in [25] the authors have studied the dominating matrix which is defined as:

Let G = (V, E) be a graph with V(G) = {v1, v2, ⋯, vn} and let DV(G) be a minimum dominating set of G. The minimum dominating matrix of G is the n × n matrix defined by AD(G) = (aij), where aij = 1 if vivjE(G) or vi = vjD, and aij = 0 if vivjE(G).

The characteristic polynomial of AD(G) is denoted by fn(G, μ) := det(μIAD(G)).

The minimum dominating eigenvalues of a graph G are the eigenvalues of AD(G). Since AD(G) is real and symmetric, its eigenvalues are real numbers and we label them in non-increasing order μ1μ2 ≥ ⋯ ≥ μn. The minimum dominating energy of G is then defined as

ED(G)=i=1n|μi|. $$\begin{array}{} \displaystyle E_{D}(G) = \sum \limits _{i=1}^n |\mu_i|. \end{array}$$

Motivated by dominating matrix, here we define the minimum connected dominating matrix abbreviated as (c-dominating matrix). The c-dominating matrix of G is the n × n matrix defined by ADc(G) = (aij), where

aij=1,ifvivjE;1,ifi=jand viDc;0,otherwise. $$\begin{array}{} \displaystyle a_{ij} = \left\{ \begin{array}{ll} 1, ~ \hbox{if}~~ v_{i}v_{j} \in E; \\[2mm] 1, ~ \hbox{if}~~i = j~~ \text{and }~~v_{i} \in D_{c}; \\[2mm] 0, ~ \hbox{otherwise.} \end{array} \right. \end{array}$$

The characteristic polynomial of ADc(G) is denoted by fn(G, λ) := det(λ IADc(G)).

The c-dominating eigenvalues of a graph G are the eigenvalues of ADc(G). Since ADc(G) is real and symmetric, its eigenvalues are real numbers and we label them in non-increasing order λ1λ2 ≥ ⋯ ≥ λn. The c-dominating energy of G is then defined as

EDc(G)=i=1n|λi|. $$\begin{array}{} \displaystyle E_{D_c}(G) = \sum \limits _{i=1}^n |\lambda_i|. \end{array}$$

To illustrate this, consider the following examples:

Figure 1

Example 1

Let G be the 5-vertex path P5, with vertices v1, v2, v3, v4, v5 and let its minimum connected dominating set be Dc = {v2, v3, v4}. Then

ADc(G)=0100011100011100011100010 $$\begin{array}{} A_{D_{c}}(G) = \left( \begin{array}{ccccc} 0 & 1 & 0 & 0 & 0 \\ 1 & 1 & 1 & 0 & 0 \\ 0 & 1 & 1 & 1 & 0 \\ 0 & 0 & 1 & 1 & 1 \\ 0 & 0 & 0 & 1 & 0 \\ \end{array} \right) \end{array}$$

The characteristic polynomial of ADc(G) is λ5 – 3λ4λ3 + 5λ2 + λ – 1 = 0. The minimum connected dominating eigenvalues are λ1 = 2.618, λ2 = 1.618, λ3 = 0.382, λ4 = –1.000 and λ5 = –0.618.

Therefore, the minimum connected dominating energy is EDc(P5) = 6.236.

Example 2

Consider the following graph

Figure 2

Let G be a tree T as shown above and let its minimum connected dominating set be Dc = {b, d, e, f, g, h}. Then

ADc(G)=0100000000111100000001000000000101100000000111000000001110000000011101000000111000000001000000001000 $$\begin{array}{} A_{D_{c}}(G) = \left( \begin{array}{cccccccccc} 0 &1& 0& 0& 0& 0& 0& 0& 0& 0 \\ 1 &1& 1& 1& 0& 0& 0& 0& 0& 0 \\ 0 &1& 0& 0& 0& 0& 0& 0& 0& 0\\ 0 &1& 0& 1& 1& 0& 0& 0& 0& 0 \\ 0 &0& 0& 1& 1& 1& 0& 0& 0& 0\\ 0 &0& 0& 0& 1& 1& 1& 0& 0& 0 \\ 0 &0& 0& 0& 0& 1& 1& 1& 0& 1 \\ 0 &0& 0& 0& 0& 0& 1& 1& 1& 0 \\ 0 &0& 0& 0& 0& 0& 0& 1& 0& 0 \\ 0 &0& 0& 0& 0& 0& 1& 0& 0& 0 \\ \end{array} \right) \end{array}$$

By direct calculation, we get the minimum connected dominating eigenvalues are λ1 = 2.945, λ2 = 2.596, λ3 = 1.896, λ4 = 1.183, λ5 = –1.263, λ6 = –1.152, λ7 = 0.579, λ8 = 0.000, λ9 = –0.268 and λ10 = –0.516.

Therefore, the minimum connected dominating energy is EDc(T) = 12.398.

Example 3

The c-dominating energy of the following graphs can be calculated easily:

EDc(Kn) = (n – 2) + n(n2)+5 $\begin{array}{} \sqrt{n(n-2) + 5} \end{array}$, where Kn is the complete graph of order n.

EDc(K1,n–1) = 4n3 $\begin{array}{} \sqrt{4n-3} \end{array}$ where K1,n–1 is the star graph.

EDc(Kn×2) = (2n – 3) + 4n(n1)9 $\begin{array}{} \sqrt{4n(n-1)-9} \end{array}$, where Kn×2 is the coctail party graph.

In this paper, we are interested in studying the mathematical aspects of the c-dominating energy of a graph. This paper has organized as follows: The section 1, contains the basic definitions and background of the current topic. In section 2, we show the chemical applicability of c-dominating energy for molecular graphs G. The section 3, contains the mathematical properties of c-dominating energy. In the last section, we have characterized, trees, unicyclic graphs and cubic graphs and block graphs with equal minimum dominating energy and c-dominating energy. Finally, we conclude this paper by posing an open problem.

Chemical Applicability of EDc(G)

We have used the c-dominating energy for modeling eight representative physical properties like boiling points(bp), molar volumes(mv) at 20C, molar refractions(mr) at 20C, heats of vaporization (hv) at 25C, critical temperatures(ct), critical pressure(cp) and surface tension (st) at 20C of the 74 alkanes from ethane to nonanes. Values for these properties were taken from http://www.moleculardescriptors.eu/dataset.htm. The c-dominating energy EDc(G) was correlated with each of these properties and surprisingly, we can see that the EDc has a good correlation with the heats of vaporization of alkanes with correlation coefficient r = 0.995.

The following structure-property relationship model has been developed for the c-dominating energy EDc(G).

hv=10EDc(G)±5. $$\begin{array}{} \displaystyle hv = 10 E_{D_{c}}(G) \pm 5. \end{array}$$

Figure 3

Correlation of EDc(G) with heats of vaporization of alkanes.

Mathematical Properties of c-Dominating Energy of Graph

We begin with the following straightforward observations.

Observation 1

Note that the trace of ADc(G) = γc(G).

Observation 2

Let G = (V, E) be a graph with γc-set Dc. Let fn(G, λ) = c0λn + c1λn–1 + ⋯ + cn be the characteristic polynomial of G. Then

c0 = 1,

c1 = –|Dc| = –γc(G).

Theorem 3

If λ1, λ2, ⋯, λn are the eigenvalues of ADc(G), then

i=1nλi=γc(G) $\begin{array}{} \displaystyle \sum\limits_{i=1}^n \lambda_i = \gamma_c(G) \end{array}$

i=1nλi2=2m+γc(G). $\begin{array}{} \displaystyle \sum\limits_{i=1}^n \lambda^2_i = 2m+\gamma_c(G). \end{array}$

Proof

Follows from Observation 1.

The sum of squares of the eigenvalues of ADc(G) is just the trace of ADc(G)2. Therefore

i=1nλi2=i=1nj=1naijaji=2i<j(aij)2+i=1n(aii)2=2m+γc(G). $$\begin{array}{} \begin{split} \displaystyle \sum\limits_{i=1}^n \lambda^2_i &=& \sum\limits_{i=1}^n \sum\limits_{j =1}^n a_{ij}a_{ji} \\ &=& 2\sum\limits_{i \lt j}(a_{ij})^2+\sum\limits_{i =1}^n(a_{ii})^2 \\ &=& 2m + \gamma_c(G). \end{split} \end{array}$$

We now obtain bounds for EDc(G) of G, similar to McClelland’s inequalities [21] for graph energy.

Theorem 4

Let G be a graph of order n and size m with γc(G) = k. Then

EDc(G)n(2m+k). $$\begin{array}{} \begin{split} \displaystyle E_{D_c}(G) & \le & \sqrt{n(2m+k)}. \end{split} \end{array}$$

Proof

Let λ1λ2 ≥ ⋯ ≥ λn be the eigenvalues of ADc(G). Bearing in mind the Cauchy-Schwarz inequality,

(i=1naibi)2(i=1nai)2(i=1nbi)2 $$\begin{array}{} \displaystyle \bigg(\sum\limits_{i=1}^n a_i b_i \bigg)^2 \le \bigg(\sum\limits_{i=1}^n a_i \bigg)^2 \bigg(\sum\limits_{i=1}^n b_i \bigg)^2 \end{array}$$

we choose ai = 1 and bi = |λi|, which by Theorem 3 implies

EDc2=(i=1n|λi|)2n(i=1n|λi|2)=ni=1nλi2=2(2m+k). $$\begin{array}{} \begin{split} \displaystyle E_{D_c}^2 &=& \bigg(\sum\limits_{i=1}^n|\lambda_i| \bigg)^2 \\ & \leq & n\bigg(\sum\limits_{i=1}^n|\lambda_i|^2 \bigg) \\ &=& n \sum\limits_{i=1}^n \lambda^2_i \\ &=& 2(2m + k). \end{split} \end{array}$$

Theorem 5

Let G be a graph of order n and size m with γc(G) = k. Let λ1λ2 ≥ ⋯ ≥ λn be a non-increasing arrangement of eigenvalues of ADc(G). Then

EDc(G)2mn+nkα(n)(|λ1||λn|)2 $$\begin{array}{} \begin{split} \displaystyle E_{D_c}(G) & \ge & \sqrt{2mn+nk-\alpha(n)(|\lambda_1|-|\lambda_n|)^2} \end{split} \end{array}$$

where α(n)=n[n2](11n[n2]) $\begin{array}{} \alpha(n) = n [\frac{n}{2}](1-\frac{1}{n}[\frac{n}{2}]) \end{array}$, where [x] denotes the integer part of a real number k.

Proof

Let a1, a2, ⋯, an and b1, b2, ⋯, bn be real numbers for which there exist real constants a, b, A and B, so that for each i, i = 1, 2, ⋯, n, aaiA and bbiB. Then the following inequality is valid (see [6]).

ni=1naibii=1naii=1nbiα(n)(Aa)(Bb), $$\begin{array}{} \begin{split} \displaystyle \mid n\sum\limits_{i =1}^n a_ib_i-\sum\limits_{i =1}^n a_i \sum\limits_{i=1}^n b_i \mid & \le & \alpha(n)(A-a)(B-b), \end{split} \end{array}$$

where α(n)=n[n2](11n[n2]) $\begin{array}{} \alpha(n) = n [\frac{n}{2}](1-\frac{1}{n}[\frac{n}{2}]) \end{array}$. Equality holds if and only if a1 = a2 = ⋯ = an and b1 = b2 = ⋯ = bn.

We choose ai := |λi|, bi := |λi|, a = b := |λn| and A = B := |λ1|, i = 1, 2, ⋯, n, inequality (4) becomes

|ni=1n|λi|2(i=1n|λi|)2|α(n)(|λ1||λn|)2. $$\begin{array}{} \begin{split} \displaystyle |n \sum\limits_{i=1}^{n}|\lambda_{i}|^2-\bigg(\sum\limits_{i=1}^n|\lambda_i| \bigg)^2| & \le & \alpha(n)(|\lambda_1|-|\lambda_n|)^2. \end{split} \end{array}$$

Since EGc(G)=i=1n|λi|,i=1n|λi|2=i=1n|λi|2=2m+k $\begin{array}{} \displaystyle E_{G_c}(G) = \sum\limits_{i=1}^n|\lambda_i|,~ \sum\limits_{i=1}^n |\lambda_i|^2 = \sum\limits_{i=1}^n |\lambda_{i}|^2 = 2m+k \end{array}$ and EDc(G)n(2m+k), $\begin{array}{} \displaystyle E_{D_c}(G) \le \sqrt{n(2m+k)}, \end{array}$ the inequality (5) becomes

n(2m+k)(EDc)2α(n)(|λ1||λn|)2(EDc)22mn+nkα(n)(|λ1||λn|)2. $$\begin{array}{} \begin{split} \displaystyle n(2m+k)-(E_{D_c})^2 & \le & \alpha(n)(|\lambda_1|-|\lambda_n|)^2 \\ (E_{D_c})^2 & \ge & 2mn+nk-\alpha(n)(|\lambda_1|-|\lambda_n|)^2. \end{split} \end{array}$$

Hence equality holds if and only if λ1 = λ2 = ⋯ = λn.□

Corollary 6

Let G be a graph of order n and size m with γc(G) = k. Let λ1λ2 ≥ ⋯ ≥ λn be a non-increasing arrangement of eigenvalues of ADc(G). Then

EDc(G)2mn+nkn24(|λ1||λn|)2. $$\begin{array}{} \begin{split} \displaystyle E_{D_c}(G) & \geq & \sqrt{2mn+nk-\frac{n^2}{4}(|\lambda_1|-|\lambda_n|)^2}. \end{split} \end{array}$$

Proof

Since α(n)=n[n2](11n[n2])n24 $\begin{array}{} \alpha(n) = n [\frac{n}{2}](1-\frac{1}{n}[\frac{n}{2}]) \le \frac{n^2}{4} \end{array}$, therefore by (3), result follows.□

Theorem 7

Let G be a graph of order n and size m with γc(G) = k. Let λ1λ2 ≥ ⋯ ≥ λn be a non-increasing arrangement of eigenvalues of ADc(G). Then

EGc(G)|λ1||λ2|n+2m+k|λ1|+|λn|. $$\begin{array}{} \begin{split} \displaystyle E_{G_c}(G) & \geq & \frac{|\lambda_1||\lambda_2|n+2m+k}{|\lambda_1|+|\lambda_n|}. \end{split} \end{array}$$

Proof

Let a1, a2, ⋯, an and b1, b2, ⋯, bn be real numbers for which there exist real constants r and R so that for each i, i = 1, 2, ⋯, n holds raibiRai. Then the following inequality is valid (see [11]).

i=1nbi2+rRi=1nai2(r+R)i=1naibi. $$\begin{array}{} \begin{split} \displaystyle \sum\limits_{i=1}^n b^2_i + rR\sum\limits_{i=1}^n a^2_i & \le & (r+R)\sum\limits_{i=1}^n a_i b_i. \end{split} \end{array}$$

Equality of (8) holds if and only if, for at least one i, 1 ≤ in holds rai = bi = Rai.

For bi := |λi|, ai := 1 r := |λn| and R := |λ1|, i = 1, 2, ⋯, n inequality (8) becomes

i=nn|λi|2+|λ1||λn|i=1n1(|λ1|+|λn|)i=1n|λi|. $$\begin{array}{} \begin{split} \displaystyle \sum\limits_{i=n}^{n}|\lambda_i|^2+|\lambda_1||\lambda_n|\sum\limits_{i=1}^{n}1 \le (|\lambda_1|+|\lambda_n|)\sum\limits_{i=1}^n|\lambda_i|. \end{split} \end{array}$$

Since i=1n|λi|2=i=1nλi2=2m+k,i=1n|λi|=EDc(G), $\begin{array}{} \displaystyle \sum\limits_{i=1}^{n}|\lambda_i|^2 = \sum\limits_{i=1}^{n}\lambda_i^2 = 2m+k,~ \sum\limits_{i=1}^n|\lambda_i| = E_{D_c}(G), \end{array}$ from inequality (9),

2m+k+|λ1||λn|n(λ1+λn)EDc(G) $$\begin{array}{} \begin{split} \displaystyle 2m+k+|\lambda_1||\lambda_n|n & \le & (\lambda_1+\lambda_n)E_{D_c}(G) \end{split} \end{array}$$

Hence the result.□

Theorem 8

Let G be a graph of order n and size m with γc(G) = k. If ξ = |detADc(G)|, then

EDc(G)2m+k+n(n1)ξ2n. $$\begin{array}{} \begin{split} \displaystyle E_{D_c}(G) & \ge & \sqrt{2m+k+n(n-1)\xi^\frac{2}{n}}. \end{split} \end{array}$$

Proof

(EDc(G))2=(i=1n|λi|)2=i=1n|λi|2+ij|λi||λj|. $$\begin{array}{} \begin{split} \displaystyle (E_{D_c}(G))^2 &=& \bigg(\sum\limits_{i=1}^n |\lambda_i| \bigg)^2 \\ &=& \sum\limits_{i=1}^n |\lambda_i|^2+\sum\limits_{i \ne j} |\lambda_i||\lambda_j|. \end{split} \end{array}$$

Employing the inequality between the arithmetic and geometric means, we obtain

1n(n1)ij|λi||λj|(ij|λi||λj|)1n(n1). $$\begin{array}{} \begin{split} \displaystyle \frac{1}{n(n-1)} \sum\limits_{i \ne j} |\lambda_i||\lambda_j| & \ge & \bigg(\prod\limits_{i \ne j} |\lambda_i||\lambda_j| \bigg)^{\frac{1}{n(n-1)}}. \end{split} \end{array}$$

Thus,

(EDG)2i=1n|λi|2+n(n1)(ij|λi||λj|)1n(n1)i=1n|λi|2+n(n1)(ij|λi|2(n1))1n(n1)=2m+k+n(n1)ξ2n. $$\begin{array}{} \begin{split} \displaystyle (E_{D_G})^2 & \ge & \sum\limits_{i=1}^n |\lambda_i|^{2}+n(n-1)\bigg(\prod\limits_{i \ne j} |\lambda_i||\lambda_j| \bigg)^{\frac{1}{n(n-1)}} \\ & \ge & \sum\limits_{i=1}^n|\lambda_i|^{2}+n(n-1)\bigg(\prod\limits_{i \ne j} |\lambda_i|^{2(n-1)} \bigg)^{\frac{1}{n(n-1)}} \\ &=& 2m+k+n(n-1)\xi^{\frac{2}{n}}. \end{split} \end{array}$$

Lemma 9

If λ1(G) is the largest minimum connected dominating eigenvalue of ADc(G), then λ12m+γc(G)n. $\begin{array}{} \lambda_1 \ge \frac{2m+\gamma_c(G)}{n}. \end{array}$

Proof

Let X be any non-zero vector. Then we have λ1(A)=maxX0{XAXXX}, $\begin{array}{} \lambda_1(A) = max_{_{X \ne 0}} \{\frac{X' A X}{X' X}\}, \end{array}$ see [16]. Therefore, λ1(ADc(G)) ≥ JAJJJ=2m+γc(G)n. $\begin{array}{} \frac{J'AJ}{J'J} = \frac{2m+\gamma_c(G)}{n}. \end{array}$

Next, we obtain Koolen and Moulton’s [19] type inequality for EDc(G).

Theorem 10

If G is a graph of order n and size m and 2m + γC(G) ≥ n, then

EDc(G)2m+γc(G)n+(n1)[(2m+γc(G))(2m+γc(G)n)2]. $$\begin{array}{} \begin{split} \displaystyle E_{D_c}(G) & \le & \frac{2m+\gamma_c(G)}{n}+\sqrt{(n-1)\bigg[(2m+\gamma_c(G))-\bigg(\frac{2m+\gamma_c(G)}{n}\bigg)^{2} \bigg]}. \end{split} \end{array}$$

Proof

Bearing in mind the Cauchy-Schwarz inequality,

(i=1naibi)2(i=1nai)2(i=1nbi)2. $$\begin{array}{} \displaystyle \bigg(\sum\limits_{i=1}^n a_i b_i \bigg)^2 \le \bigg(\sum\limits_{i=1}^{n}a_i \bigg)^2 \bigg(\sum\limits_{i=1}^n b_i \bigg)^2. \end{array}$$

Put ai = 1 and bi = |λi| then

(i=2naibi)2(n1)(i=2nbi)2(EDc(G)λ1)2(n1)(2m+γc(G)λ12)EDc(G)λ1+(n1)(2m+γc(G)λ12). $$\begin{array}{} \begin{split} \displaystyle \bigg(\sum\limits_{i=2}^n a_i b_i \bigg)^2 & \le & (n-1)\bigg(\sum\limits_{i=2}^n b_i \bigg)^2 \\ (E_{D_c}(G)-\lambda_1)^2 & \le &(n-1)(2m+\gamma_c(G)-\lambda^2_1) \\ E_{D_c}(G) & \le & \lambda_1+\sqrt{(n-1)(2m+\gamma_c(G)-\lambda^2_1)}. \end{split} \end{array}$$

Let

f(x)=x+(n1)(2m+γc(G)x2). $$\begin{array}{} \begin{split} \displaystyle f(x) &=& x+\sqrt{(n-1)(2m+\gamma_c(G)-x^2)}. \end{split} \end{array}$$

For decreasing function

f(x)01x(n1)(n1)(2m+γc(G)x2)0x2m+γc(G)n. $$\begin{array}{} \begin{split} \displaystyle f'(x) & \le & 0 \\ \Rightarrow 1-\frac{x(n-1)}{\sqrt{(n-1)(2m+\gamma_c(G)-x^2)}} & \le & 0 \\ x & \ge & \sqrt{\frac{2m+\gamma_c(G)}{n}}. \end{split} \end{array}$$

Since (2m + k) ≥ n, we have 2m+γc(G)n2m+γc(G)nλ1. $\begin{array}{} \sqrt{\frac{2m+\gamma_{c}(G)}{n}} \le \frac{2m+\gamma_c(G)}{n} \le \lambda_1. \end{array}$ Also f(λ1)f(2m+γc(G)n). $\begin{array}{} f(\lambda_1) \le f\bigg(\frac{2m+\gamma_c(G)}{n} \bigg). \end{array}$

i.eEDc(G)f(λ1)f(2m+γc(G)n).i.eEDc(G)f(2m+γc(G)n) $$\begin{array}{c} \displaystyle \text{i.e}~~ E_{D_c}(G) \le f(\lambda_1) \le f\bigg( \frac{2m+\gamma_c(G)}{n} \bigg). \\\displaystyle \text{i.e}~~ E_{D_c}(G) \le f\bigg( \frac{2m+\gamma_c(G)}{n} \bigg) \end{array}$$

Hence by (12), the result follows.□

Graphs with equal Dominating and c-Dominating Energy

Its a natural question to ask that for which graphs the dominating energy and c-dominating energy are equal. To answer this question, we characterize graphs with equal dominating energy and c-dominating energy. The graphs considered in this section are trees, cubic graphs, unicyclic graphs, block graphs and cactus graphs.

Theorem 11

Let G = T be a tree with at least three vertices, then ED(G) = EDc(G) if and only if every internal vertex of T is a support vertex.

Proof

Let G = T be a tree of order at least 3. Let F = {u1, u2, ⋯, uk} be the set of internal vertices of T. Then clearly F is the minimal dominating set of G. Therefore in AD(G) the values of ui = 1 in the diagonal entries. Further, observe that 〈F〉 is connected. Hence F is the minimal connected dominating set. Therefore, AD(G) = ADc(G). In general, AD(G) = ADc(G) is true if every minimum dominating set is connected. In other words, AD(G) = ADc(G) if γ(G) = γc(G). Therefore, the result follows from Theorem 2.1 in [2].□

In the next three theorems we characterize unicyclic graphs with AD(G) = ADc(G). Since, AD(G) = ADc(G) if γ(G) = γc(G). Therefore, the proof of our next three results follows from Theorem 2.2, Theorem 2.4 and Theorem 2.5 in [2].

Theorem 12

Let G be a unicyclic graph with cycle C = u1u2 ⋯, unu1 n ≥ 5 and let X = {vC : dG(v) ≥ 2}. Then ED(G) = EDc(G) if the following conditions hold:

(a). Every vVN[X] with dG(V) ≥ 2 is a support vertex.

(b). 〈Xis connected and |X| ≤ 3.

(c). IfX〉 = P1 or P3, both vertices in N(X) of degree at least 3 are supports and ifX〉 = P2, at least one vertex in N(X) of degree at least three is a support.

Theorem 13

Let G be unicyclic graph with |V(G)| ≥ 4 containing a cycle C = C3, and let X = {vC : dG(v) = 2}. Then ED(G) = EDc(G) if the following conditions hold:

(a). Every vVN[X] with dG(V) ≥ 2 is a support vertex.

(b). There exists some unique vC with dG(v) ≥ 3 or for every vC of dG(v) ≥ 3 is a support.

Theorem 14

Let G be unicyclic graph with |V(G)| ≥ 5 containing a cycle C = C4, and let X = {vC : dG(v) = 2}. Then ED(G) = EDc(G) if the following conditions hold:

(a). Every vVN[X] with dG(V) ≥ 2 is a support vertex.

(b). If |X| = 1, all the three remaining vertices of C are supports and if |X| ≥ 2, C contains at least one support.

Theorem 15

Let G be a connected cubic graph of order n, Then ED(G) = EDc(G) if GK4, C6,K3,3, G1 or G2 where G1 and G2 are given in Fig. 4.

Theorem 16

Let G be a block graph of with l ≥ 2. Then ED(G) = EDc(G) if every cutvertex of G is an end block cutvertex.

Proof

Since ED(G) = EDc(G) if γ(G) = γc(G). Therefore, the result follows from Theorem 2 in [7].□

We conclude this paper by posing the following open problem for the researchers:

Open Problem: Construct non- cospectral graphs with unequal domination and connected domination numbers having equal dominating energy and c-dominating energy.

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