The metric dimension of a graph \(\Gamma = (V, E)\), denoted by \( \operatorname{dim}(\Gamma) \), is the least cardinality of a set of vertices in \(\Gamma\) such that each vertex in \(\Gamma\) is determined uniquely by its vector of distances to the vertices of the chosen set. The topological distance between an edge \(\varepsilon = yz \in E\) and a vertex \( k \in V \) is defined as \( d(\varepsilon, k) = \min\{d(z, k), d(y, k)\} \). A subset of vertices \( R_{\Gamma} \) in \( V \) is called an edge resolving set for \(\Gamma\) if for each pair of different edges \( e_{1} \) and \( e_{2} \) in \( E \), there is a vertex \( j \in R_{\Gamma} \) such that \( d(e_{1}, j) \neq d(e_{2}, j) \). An edge resolving set with minimum cardinality is called the edge metric basis for \(\Gamma\) and this cardinality is the edge metric dimension of \(\Gamma\), denoted by \( \operatorname{dim}_{E}(\Gamma) \). In this article, we show that the cardinality of the minimum edge resolving set is three or four for two classes of convex polytopes (\( S_{n} \) and \( T_{n} \)) that exist in the literature.
Suppose \(\Gamma=\Gamma(V,E)\) be an undirected, connected, simple, and non-trivial graph with order \(|V(\Gamma)|\) and size \(|E(\Gamma)|\). For each pair of distinct vertices \(j,k \in V\), the distance between them, denoted by \(d(j,k)\), is the number of edges in the shortest \(j-k\) path. A vertex \(p\in V(\Gamma)\) resolves (or recognize) a pair of distinct vertices \(j,k\) if \(d(j,p)\neq d(k,p)\). A subset of vertices \(R\subseteq V(\Gamma)\) recognizes \(\Gamma\) if every possible pair of different vertices in \(\Gamma\) are resolved by some vertex in \(R\), then \(R\) is known as the resolving set (or metric generator) for \(\Gamma\). For an ordered set \(R=\{h_{1}, h_{2}, h_{3},…,h_{y}\}\subseteq V\) of different vertices, the metric code (or co-ordinate) of \(v\in V\) with respect to \(R\) is the \(y\)-vector \(\gamma(v|R)=(d(v,h_{1}),d(v,h_{2}),d(v,h_{3}),…,d(v,h_{y}))\). The \(metric\) \(dimension\) of \(\Gamma\) is denoted by \(dim(\Gamma)\), where \(dim(\Gamma)=min\{|R|: R\ is\ resolving\ in\ \Gamma\}\).
The notion of resolving set for a connected simple graph was proposed by Slater [1], under the name \(locating\) \(set\); he referred to a minimum resolving set as a \(reference\) \(set\), and the minimum cardinality of such a generator for a given connected graph as the location number of a graph. These concepts were independently studied by Harary and Melter [2] under the name metric dimension. It has been extensively investigated in a number of research articles, see Sebo and Tannier [3], Sharma and Bhat [4,5], Khuller et al. [6], Chartrand et al. [7], Imran et al. [8], Javid et al. [9], Wei et al. [10], etc. It has appeared in several areas including robot navigation [6], pattern recognition and image processing [11], combinatorial optimization [3], and chemical science [12,13].
An edge metric dimension is a newly introduced (by Kelenc et al. [14]) variant of the metric dimension. Then it was further investigated by Peterin and Yero [15], Zhu et al. [16], Zubrilina [17], etc. The distance between a vertex \(k\in V\) and an edge \(e=yz\in E\) is given by \(d(e,k)=min\{d(z,k), d(y,k)\}\). For an ordered set, \(R_{\Gamma}= \{r_{1}, r_{2}, r_{3},…,r_{m}\}\) of distinct vertices in \(\Gamma\), the edge metric code (or edge code) of an edge \(e_{1} \in E\) with respect to \(R_{\Gamma}\) is the \(m\)-vector \(\gamma_{E}(e_{1}|R)=(d(e_{1},r_{1}),d(e_{1},r_{2}),d(e_{1},r_{3}),…,d(e_{1},r_{m}))\). Then, \(R_{\Gamma}\) is called the edge resolving set (ERS) for \(\Gamma\) iff for every pair of distinct edges \(e_{1}\), \(e_{2}\) of \(\Gamma\), we have \(\gamma_{E}(e_{1}|R)\neq \gamma_{E}(e_{2}|R)\). This \(R_{\Gamma}\) with minimum number vertices is called an edge metric basis of \(\Gamma\). The edge metric dimension (EMD) of \(\Gamma\) is denoted by \(dim_{E}(\Gamma)\), where \(dim_{E}(\Gamma)=min\{|R_{\Gamma}|:R_{\Gamma}\ is\ an\ EMG\ of\ \Gamma \}\).
In [14], Kelenc et al. initiated and introduced the study of the EMD in a non-trivial connected graphs with respect to identifying uniquely the edges of the graph. They have given some comparison between the EMD and the metric dimension. They particularly stated that it is possible to find graphs where the EMD equals the metric dimension, as well as other graphs \(\Gamma\) where \(dim_{E}(\Gamma)<dim(\Gamma)\) or \(dim_{E}(\Gamma)>dim(\Gamma)\). In this paper, we consider two convex polytopes graph families, namely, \(S_{n}\) and \(T_{n}\), already exists in the literature [8], and analyze such situations further by comparing the value of \(dim_{E}(\Gamma)\) and \(dim(\Gamma)\), where \(\Gamma\) represents one of the convex polytopes graph \(S_{n}\) and \(T_{n}\).
The main contribution of the paper are as follows:
The cardinality of minimum edge resolving set for \(S_{n}\) and \(T_{n}\) is three or four.
Edge metric dimension (\(S_{n}\) and \(T_{n}\)) \(\geq\) Metric dimension (\(S_{n}\) and \(T_{n}\)).
The edge resolving set for \(S_{n}\) and \(T_{n}\) are independent.
These notions of metric dimension as well as its variants have been investigated for distinctively significant graph families, for instance; planar graphs: path graph, kayak paddle graph, several ladder graphs, (ladders of pentagons, heptags, nonagons, etc), antiprism graph, mobious ladder graph, wheel graph, cycle graph, various convex polytopes, tadpole graph, and many more; chemical graphs: one-pentagonal, one heptagonal, one nonagonal carbon nanocone structures, linear heptagons structures, polycyclic aromatic compound, and linear phenylene structure, for these one can refer [17-22]. The list is long but is still incomplete, i.e., there are infinite number of distinct graph families for which the notions of resolving sets and its variants have not been discussed yet. So, to address this partially, in this paper, we consider two interesting planar graph families of convex polytopes, denoted by \(S_{n}\) & \(T_{n}\), and determine their edge metric basis as well as edge metric dimension.
The rest of this paper is organized in the following manner: Section 2 introduces some basic concepts related to the resolving and the edge resolving sets of graphs. In addition, some of the established results regarding the metric dimension of \(S_{n}\) and \(T_{n}\) are also discussed. In sections 3 and 4, we investigate the edge metric dimension of the convex polytope graphs \(S_{n}\) and \(T_{n}\), respectively. Finally, Sect. 5 discusses the conclusion and comparison of the metric dimension and the EMD of these two graphs.
In the present section, we define some necessary terminology and give some preliminary results about the metric dimension and the EMD.
Definition 1 (Independent resolving set (IRS)). [23] A subset \(R\) of distinct vertices in \(\Gamma\), is said to be an IRS for \(\Gamma\), if \(R\) is both resolving and independent set.
Definition 2 (Independent edge resolving set (IERS)). [4] A subset \(R_{E}\) of distinct vertices in \(\Gamma\), is said to be an IERS for \(\Gamma\), if \(R_{E}\) is both edge resolving and independent set.
Following are the some significant known results concerning the metric dimension and the EMD:
Proposition 1. [14] For every natural \(n\geq3\),
Graph \(P_{n}\) is a path iff \(1=dim(P_{n})=dim_{E}(P_{n})\).
\(2=dim(C_{n})=dim_{E}(C_{n})\), where \(C_{n}\) is the cycle graph of order \(n\).
\(n-1=dim(K_{n})=dim_{E}(K_{n})\), where \(K_{n}\) is the complete graph of order \(n\).
Next, suppose \(\mathbb{Y}\) be a family of simple non-trivial graphs \(\Gamma_{n}: \mathbb{Y}= (\Gamma_{n})_{n\geq1}\) relying on \(n\) as follows: the order \(\varphi(n)=|V(\Gamma)|\) and \(\lim_{n \rightarrow \infty}\varphi(n)=\infty\). If there is a constant \(U >0\) such that \(dim_{E}(\Gamma_{n})> U\) for every \(n \geq 1\) then we say that \(\mathbb{Y}\) is the family of graphs with unbounded EMD, otherwise \(\mathbb{Y}\) has a bounded EMD. If all the graphs in \(\mathbb{Y}\) have the equal EMD, then \(\mathbb{Y}\) is known as the constant EMD graphs family. In recent years, several authors have investigated the bounded and unbounded EMD for various graph families [24]. The maximum (minimum) degree in \(\Gamma\) is denoted by \(\Delta(\Gamma)\) (\(\delta(\Gamma)\)). Now, for a connected graph \(\Gamma\), the lower bounds with respect to \(\Delta(\Gamma)\) and \(\delta(\Gamma)\) for the EMD are given in the following propositions.
Proposition 2. [14] If \(\Delta(\Gamma)\) is the maximum degree in \(\Gamma\), then \(\lceil log_{2}\Delta(\Gamma) \rceil\leq dim_{E}(\Gamma)\).
Proposition 3. [25] If \(\delta(\Gamma)\) is the minimum degree in \(\Gamma\), then \(\lceil log_{2}\delta(\Gamma)\rceil+1 \leq dim_{E}(\Gamma)\).
In this work, we consider two graphs of convex polytopes \(S_{n}\) & \(T_{n}\) [8], and we obtain their EMD. Recently, the metric dimension of these two convex polytope graphs was computed. For the metric dimension of these two graphs we have the following results:
Theorem 1. [8] \(dim(S_{n})=3\), where \(n\geq6\) is a positive integer.
Theorem 2. [8] \(dim(T_{n})=3\), where \(n\geq6\) is a positive integer.
In the next section, we consider a family of convex polytope graph \(S_{n}\) for which we have \(E(S_{n})=\{j_{\bar{q}}j_{\bar{q}+1}, j_{\bar{q}}k_{\bar{q}}, k_{\bar{q}}j_{\bar{q}+1}, k_{\bar{q}}l_{\bar{q}}, l_{\bar{q}}m_{\bar{q}}, m_{\bar{q}}l_{\bar{q}+1}, m_{\bar{q}}o_{\bar{q}}, o_{\bar{q}}o_{\bar{q}+1}:1 \leq \bar{q} \leq n\}\) (see Figure 1). We denote the sets of edge metric co-ordinates for the edges of \(S_{n}\) by \(A_{1}\), \(A_{2}\), \(A_{3}\), \(A_{4}\), \(A_{5}\), \(A_{6}\), \(A_{7}\), and \(A_{8}\), where \(A_{1}=\{\gamma_{E}(j_{\bar{q}}j_{\bar{q}+1}|R_{E}): 1 \leq \bar{q} \leq n\}\), \(A_{2}=\{\gamma_{E}(j_{\bar{q}}k_{\bar{q}}|R_{E}): 1 \leq \bar{q} \leq n\}\), \(A_{3}=\{\gamma_{E}(k_{\bar{q}}j_{\bar{q}+1}|R_{E}): 1 \leq \bar{q} \leq n\}\), \(A_{4}=\{\gamma_{E}(k_{\bar{q}}l_{\bar{q}}|R_{E}): 1 \leq \bar{q} \leq n\}\), \(A_{5}=\{\gamma_{E}(l_{\bar{q}}m_{\bar{q}}|R_{E}): 1 \leq \bar{q} \leq n\}\), \(A_{6}=\{\gamma_{E}(m_{\bar{q}}l_{\bar{q}+1}|R_{E}): 1 \leq \bar{q} \leq n\}\), \(A_{7}=\{\gamma_{E}(m_{\bar{q}}o_{\bar{q}}|R_{E}): 1 \leq \bar{q} \leq n\}\), and \(A_{8}=\{\gamma_{E}(o_{\bar{q}}o_{\bar{q}+1}|R_{E}): 1 \leq \bar{q} \leq n\}\).
In this section, we study some of the basic properties and the EMD of \(S_{n}\).
The convex polytope \(S_{n}\) [8] consists of \(5n\) and \(8n\) number of vertices and edges respectively (see Figure 1). It has \(n\) cycles with \(3\)-sides, \(n\) cycles with \(6\)-sides, \(n\) cycles with \(5\)-sides, and two cycles with \(n\)-sides. The set of edges and vertices of \(S_{n}\) are denoted separately by \(E(S_{n})\) and \(V(S_{n})\), where \(E(S_{n})=\{j_{\bar{q}}j_{\bar{q}+1}, j_{\bar{q}}k_{\bar{q}}, k_{\bar{q}}j_{\bar{q}+1}, k_{\bar{q}}l_{\bar{q}}, l_{\bar{q}}m_{\bar{q}}, m_{\bar{q}}l_{\bar{q}+1}, m_{\bar{q}}o_{\bar{q}}, o_{\bar{q}}o_{\bar{q}+1}:1 \leq \bar{q} \leq n\}\) and \(V(S_{n})=\{j_{\bar{q}}, k_{\bar{q}}, l_{\bar{q}}, m_{\bar{q}}, o_{\bar{q}}:1 \leq \bar{q} \leq n\}\).
We name the vertices \(\{j_{\bar{q}}:1 \leq \bar{q} \leq n\}\) in the planar graph, \(S_{n}\) as the \(j\)-cycle vertices, the vertices \(\{k_{\bar{q}}:1 \leq \bar{q} \leq n\}\) in the planar graph, \(S_{n}\) as the \(k\)-vertices, the vertices \(\{l_{\bar{q}}:1 \leq \bar{q} \leq n\}\) in the planar graph, \(S_{n}\) as the \(l\)-vertices, the vertices \(\{m_{\bar{q}}:1 \leq \bar{q} \leq n\}\) in the planar graph, \(S_{n}\) as the \(m\)-vertices, and the vertices \(\{o_{\bar{q}}: 1 \leq \bar{q} \leq n\}\) in the planar graph, \(S_{n}\) as the \(o\)-cycle vertices. For our purpose, we can write \(j_{1}=j_{n+1}\), \(k_{1}=k_{n+1}\), \(l_{1}=l_{n+1}\), \(m_{1}=m_{n+1}\), and \(o_{1}=o_{n+1}\). In the following result, we investigate the EMD of \(S_{n}\).
Theorem 3. \(dim_{E}(S_{n})=4\), where \(n\geq6\) is a positive integer.
Proof. It is easy to check for \(6\leq n\leq 11\) that the EMD of \(S_{n}\) is 4. The position of the edge basis vertices (color in red) can be found in Figure 1, for all \(n\geq6\). Now, for \(n\geq 12\), we divide our proof into two cases i.e., when \(n\) is even (\(n \equiv 0\ (mod\ 2)\)) and when it is odd (\(n \equiv 1\ (mod\ 2)\)).
Then, for the natural \(n\), we have \(n = 2h\), where \(h \in \mathbb{N}\) and \(h \geq 6\). Suppose \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\} \subset V(S_{n})\). Next, we give edge metric representation to every edge of \(S_{n}\) concerning the set \(R_{E}\).
For the edges of \(j\)-cycle \(\{e_{\bar{q}}=j_{\bar{q}}j_{\bar{q}+1}| \bar{q}=1,2,3,…,n\}\), the edge codes are
\(\gamma_{E}(e_{\bar{q}}=j_{\bar{q}}j_{\bar{q}+1} |R_{E})\) | \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((1,1,h-\bar{q}+1,4)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2\)) | \((\bar{q}-1,1,h-\bar{q}+1,4)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(3 \leq \bar{q} \leq h\)) | \((\bar{q}-1,\bar{q}-2,h-\bar{q}+1,\bar{q}+1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((\bar{q}-1,\bar{q}-2,1,\bar{q}+1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+2 \leq \bar{q} \leq 2h\)) | \((2h-\bar{q}+1,2h-\bar{q}+2,\bar{q}-h-1,2h-\bar{q}+4)\) |
For the edges \(\{e_{\bar{q}}=j_{\bar{q}}k_{\bar{q}}, k_{\bar{q}}j_{\bar{q}+1}, k_{\bar{q}}l_{\bar{q}}, l_{\bar{q}}m_{\bar{q}}, m_{\bar{q}}l_{\bar{q}+1}, m_{\bar{q}}o_{\bar{q}}| \bar{q}=1,2,3,…,n\}\), the edge codes are
\(\gamma_{E}(e_{\bar{q}}=j_{\bar{q}}k_{\bar{q}}|R_{E})\) | \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((0,2,h,3)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2\)) | \((\bar{q}-1,0,h-\bar{q}+2,3)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(3 \leq \bar{q} \leq h\)) | \((\bar{q}-1,\bar{q}-2,h-\bar{q}+2,\bar{q}+1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((\bar{q}-1,\bar{q}-2,0,\bar{q}+1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+2\)) | \((2h-\bar{q}+2,\bar{q}-2,\bar{q}-h-1,2h-\bar{q}+4)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+3 \leq \bar{q} \leq 2h\)) | \((2h-\bar{q}+2,2h-\bar{q}+3,\bar{q}-h-1,2h-\bar{q}+4)\) |
\(\gamma_{E}(e_{\bar{q}}=k_{\bar{q}}j_{\bar{q}+1}|R_{E})\) | \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((0,1,h-\bar{q}+1,3)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2\)) | \((\bar{q},0,h-\bar{q}+1,3)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(3 \leq \bar{q} \leq h\)) | \((\bar{q},\bar{q}-1,h-\bar{q}+1,\bar{q}+1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((2h-\bar{q}+1,\bar{q}-1,0,\bar{q}+1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+2 \leq \bar{q} \leq 2h\)) | \((2h-\bar{q}+1,2h-\bar{q}+2,\bar{q}-h,2h-\bar{q}+4)\) |
\(\gamma_{E}(e_{\bar{q}}=k_{\bar{q}}l_{\bar{q}}|R_{E})\) | \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((0,2,h-\bar{q}+2,2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2\)) | \((\bar{q},0,h-\bar{q}+2,2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(3 \leq \bar{q} \leq h\)) | \((\bar{q},\bar{q}-1,h-\bar{q}+2,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((\bar{q},\bar{q}-1,0,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+2\)) | \((2h-\bar{q}+2,\bar{q}-1,\bar{q}-h,2h-\bar{q}+3)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+3\leq \bar{q} \leq 2h\)) | \((2h-\bar{q}+2,2h-\bar{q}+3,\bar{q}-h,2h-\bar{q}+3)\) |
\(\gamma_{E}(e_{\bar{q}}=l_{\bar{q}}m_{\bar{q}}|R_{E})\) | \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((1,2,h-\bar{q}+3,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2\)) | \((\bar{q}+1,1,h-\bar{q}+3,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(3 \leq \bar{q} \leq h-1\)) | \((\bar{q}+1,\bar{q},h-\bar{q}+3,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h\)) | \((\bar{q}+1,\bar{q},2,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((\bar{q}+1,\bar{q},1,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+2\leq \bar{q} \leq 2h-1\)) | \((2h-\bar{q}+3,2h-\bar{q}+4,\bar{q}-h+1,2h-\bar{q}+2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2h\)) | \((2,2h-\bar{q}+4,\bar{q}-h+1,2h-\bar{q}+2)\) |
\(\gamma_{E}(e_{\bar{q}}=m_{\bar{q}}l_{\bar{q}+1}|R_{E})\) | \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((2,1,h-\bar{q}+2,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2\)) | \((\bar{q}+2,2,h-\bar{q}+2,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(3 \leq \bar{q} \leq h-1\)) | \((\bar{q}+2,\bar{q}+1,h-\bar{q}+2,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h\)) | \((\bar{q}+2,\bar{q}+1,1,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((2h-\bar{q}+2,2h-\bar{q}+3,2,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+2\leq \bar{q} \leq 2h-1\)) | \((2h-\bar{q}+2,2h-\bar{q}+3,\bar{q}-h+2,2h-\bar{q}+2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2h\)) | \((1,2h-\bar{q}+3,\bar{q}-h+2,2h-\bar{q}+2)\) |
and
\(\gamma_{E}(e_{\bar{q}}=m_{\bar{q}}o_{\bar{q}}|R_{E})\) | \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((2,2,h-\bar{q}+3,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2\)) | \((\bar{q}+2,2,h-\bar{q}+3,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(3 \leq \bar{q} \leq h-1\)) | \((\bar{q}+2,\bar{q}+1,h-\bar{q}+3,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h\)) | \((\bar{q}+2,\bar{q}+1,2,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((2h-\bar{q}+3,\bar{q}+1,2,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+2\leq \bar{q} \leq 2h-1\)) | \((2h-\bar{q}+3,2h-\bar{q}+4,\bar{q}-h+2,2h-\bar{q}+1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2h\)) | \((2,2h-\bar{q}+4,\bar{q}-h+2,2h-\bar{q}+1)\) |
Finally, for the edges of \(o\)-cycle \(\{e_{\bar{q}}=o_{\bar{q}}o_{\bar{q}+1}| \bar{q}=1,2,3,…,n\}\), the edge codes are
\(\gamma_{E}(e_{\bar{q}}=o_{\bar{q}}o_{\bar{q}+1}|R_{E})\) | \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((\bar{q}+2,3,h-\bar{q}+2,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(2 \leq \bar{q} \leq h-1\)) | \((\bar{q}+2,\bar{q}+1,h-\bar{q}+2,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h\)) | \((\bar{q}+2,\bar{q}+1,3,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+1\leq \bar{q} \leq 2h-1\)) | \((2h-\bar{q}+2,2h-\bar{q}+3,\bar{q}-h+2,2h-\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2h\)) | \((3,2h-\bar{q}+3,\bar{q}-h+2,2h-\bar{q})\) |
From these edge codes in \(S_{n}\), we find that \(|A_{i}|=n\) (\(1\leq i \leq 8\)) and the sum of all of these cardinalities is equal to \(|E(S_{n})|\) and which is \(8n\). Moreover, all of these sets are pairwise disjoint, and so we find that no pair of two distinct edges in \(S_{n}\) are having the same edge metric coordinates, which implies that \(dim_{E}(S_{n})\leq 4\). Now, to finish the proof for this case, we prove that \(dim(S_{n})\geq 4\) by proving that there is no set \(R_{E}\) with \(|R_{E}| = 3\), which can resolve every pair of edges in \(S_{n}\). On the contrary, suppose \(dim_{E}(S_{n})=3\). Then, we have the following to be considered:
By the symmetry \(S_{n}\), other relations can be considered, and they will produce the same kind of contradictions. As a result, it can be found that \(dim_{E}(S_{n})=4\), when \(n\) is even.
Then, for the natural \(n\), we have \(n = 2h+1\), where \(h \in \mathbb{N}\) and \(h \geq 6\). Suppose \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\} \subset V(S_{n})\). Next, we give edge metric representation to every edge of \(S_{n}\) concerning the set \(R_{E}\). For the edges of \(j\)-cycle \(\{e_{\bar{q}}=j_{\bar{q}}j_{\bar{q}+1}| \bar{q}=1,2,3,…,n\}\), the edge codes are
\(\gamma_{E}(e_{\bar{q}}=j_{\bar{q}}j_{\bar{q}+1} |R_{E})\) | \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((1,1,h-\bar{q}+1,4)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2\)) | \((\bar{q}-1,1,h-\bar{q}+1,4)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(3 \leq \bar{q} \leq h\)) | \((\bar{q}-1,\bar{q}-2,h-\bar{q}+1,\bar{q}+1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((\bar{q}-1,\bar{q}-2,1,\bar{q}+1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+2\)) | \((2h-\bar{q}+2,\bar{q}-2,\bar{q}-h-1,2h-\bar{q}+5)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+3\leq \bar{q} \leq 2h+1\)) | \((2h-\bar{q}+2,2h-\bar{q}+3,\bar{q}-h-1,2h-\bar{q}+5)\) |
For the edges \(\{e_{\bar{q}}=j_{\bar{q}}k_{\bar{q}}, k_{\bar{q}}j_{\bar{q}+1}, k_{\bar{q}}l_{\bar{q}}, l_{\bar{q}}m_{\bar{q}}, m_{\bar{q}}l_{\bar{q}+1}, m_{\bar{q}}o_{\bar{q}}| \bar{q}=1,2,3,…,n\}\), the edge codes are
\(\gamma_{E}(e_{\bar{q}}=j_{\bar{q}}k_{\bar{q}}|R_{E})\) | \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((0,2,h-\bar{q}+2,3)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2\)) | \((\bar{q}-1,0,h-\bar{q}+2,3)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(3 \leq \bar{q} \leq h\)) | \((\bar{q}-1,\bar{q}-2,h-\bar{q}+2,\bar{q}+1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((\bar{q}-1,\bar{q}-2,0,\bar{q}+1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+2\)) | \((2h-\bar{q}+3,\bar{q}-2,\bar{q}-h-1,2h-\bar{q}+5)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+3 \leq \bar{q} \leq 2h+1\)) | \((2h-\bar{q}+3,2h-\bar{q}+4,\bar{q}-h-1,2h-\bar{q}+5)\) |
\(\gamma_{E}(e_{\bar{q}}=k_{\bar{q}}j_{\bar{q}+1}|R_{E})\) | \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((0,1,h-\bar{q}+1,3)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2\)) | \((\bar{q},0,h-\bar{q}+1,3)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(3 \leq \bar{q} \leq h\)) | \((\bar{q},\bar{q}-1,h-\bar{q}+1,\bar{q}+1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((\bar{q},\bar{q}-1,0,\bar{q}+1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+2 \leq \bar{q} \leq 2h+1\)) | \((2h-\bar{q}+2,2h-\bar{q}+3,\bar{q}-h,2h-\bar{q}+5)\) |
\(\gamma_{E}(e_{\bar{q}}=k_{\bar{q}}l_{\bar{q}}|R_{E})\) | \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((0,2,h-\bar{q}+2,2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2\)) | \((\bar{q},0,h-\bar{q}+2,2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(3 \leq \bar{q} \leq h\)) | \((\bar{q},\bar{q}-1,h-\bar{q}+2,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((\bar{q},\bar{q}-1,0,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+2\)) | \((2h-\bar{q}+3,\bar{q}-1,\bar{q}-h,2h-\bar{q}+4)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+3\leq \bar{q} \leq 2h+1\)) | \((2h-\bar{q}+3,2h-\bar{q}+4,\bar{q}-h,2h-\bar{q}+4)\) |
\(\gamma_{E}(e_{\bar{q}}=l_{\bar{q}}m_{\bar{q}}|R_{E})\) | \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((1,2,h-\bar{q}+3,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2\)) | \((\bar{q}+1,1,h-\bar{q}+3,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(3 \leq \bar{q} \leq h-1\)) | \((\bar{q}+1,\bar{q},h-\bar{q}+3,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h\)) | \((\bar{q}+1,\bar{q},2,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((\bar{q}+1,\bar{q},1,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+2\)) | \((2h-\bar{q}+4,\bar{q},\bar{q}-h+1,2h-\bar{q}+3)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+2\leq \bar{q} \leq 2h\)) | \((2h-\bar{q}+4,2h-\bar{q}+5,\bar{q}-h+1,2h-\bar{q}+3)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2h+1\)) | \((2,2h-\bar{q}+4,\bar{q}-h+1,2h-\bar{q}+3)\) |
\(\gamma_{E}(e_{\bar{q}}=m_{\bar{q}}l_{\bar{q}+1}|R_{E})\) | \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((2,1,h-\bar{q}+2,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2\)) | \((\bar{q}+2,2,h-\bar{q}+2,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(3 \leq \bar{q} \leq h-1\)) | \((\bar{q}+2,\bar{q}+1,h-\bar{q}+2,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h\)) | \((\bar{q}+2,\bar{q}+1,1,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((2h-\bar{q}+3,\bar{q}+1,2,\bar{q})\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+2\leq \bar{q} \leq 2h\)) | \((2h-\bar{q}+3,2h-\bar{q}+4,\bar{q}-h+2,2h-\bar{q}+3)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2h+1\)) | \((1,2h-\bar{q}+4,h+2,2h-\bar{q}+3)\) |
and
\(\gamma_{E}(e_{\bar{q}}=m_{\bar{q}}o_{\bar{q}}|R_{E})\) | \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((2,2,h-\bar{q}+3,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2\)) | \((\bar{q}+2,2,h-\bar{q}+3,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(3 \leq \bar{q} \leq h-1\)) | \((\bar{q}+2,\bar{q}+1,h-\bar{q}+3,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h\)) | \((\bar{q}+2,\bar{q}+1,2,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((\bar{q}+2,\bar{q}+1,2,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+2\leq \bar{q} \leq 2h\)) | \((2h-\bar{q}+4,2h-\bar{q}+5,\bar{q}-h+2,2h-\bar{q}+2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2h+1\)) | \((2,2h-\bar{q}+5,\bar{q}-h+2,2h-\bar{q}+2)\) |
Finally, for the edges of \(o\)-cycle \(\{e_{\bar{q}}=o_{\bar{q}}o_{\bar{q}+1}| \bar{q}=1,2,3,…,n\}\), the edge codes are
\(\gamma_{E}(e_{\bar{q}}=o_{\bar{q}}o_{\bar{q}+1}|R_{E})\) | \(R_{E} = \{k_{1}, k_{2}, k_{h+1}, o_{1}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((\bar{q}+2,3,h-\bar{q}+2,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(2 \leq \bar{q} \leq h-1\)) | \((\bar{q}+2,\bar{q}+1,h-\bar{q}+2,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h\)) | \((\bar{q}+2,\bar{q}+1,3,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((2h-\bar{q}+3,\bar{q}+1,\bar{q}-h+2,2h-\bar{q}+1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+2\leq \bar{q} \leq 2h\)) | \((2h-\bar{q}+3,2h-\bar{q}+4,\bar{q}-h+2,2h-\bar{q}+1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2h+1\)) | \((3,2h-\bar{q}+4,h+2,2h-\bar{q}+1)\) |
From these edge codes in \(S_{n}\), we find that \(|A_{i}|=n\) (\(1\leq i \leq 8\)) and the sum of all of these cardinalities is equal to \(|E(S_{n})|\) and which is \(8n\). Moreover, all of these sets are pairwise disjoint, and so we find that no pair of two distinct edges in \(S_{n}\) are having the same edge metric coordinates, which implies that \(dim_{E}(S_{n})\leq 4\) as well in this case.
Now, on assuming that \(dim_{E}(S_{n})=3\), there are the same possibilities as discussed in Case (slowromancapi@) and a contradiction can be deduced similarly. Therefore, we have \(dim_{E}(S_{n}) = 4\) as well in this case, which proofs the theorem. ◻
Corollary 1. The minimum independent edge resolving set for \(S_{n}\) has cardinality four, for every \(n \geq 6\).
Remark 1. \(dim(S_{n})<dim_{E}(S_{n})\), for every \(n\geq 6\).
In the next section, we consider second family of convex polytope graph \(T_{n}\) for which we have \(E(T_{n})=\{j_{\bar{q}}j_{\bar{q}+1}, j_{\bar{q}}k_{\bar{q}}, k_{\bar{q}}j_{\bar{q}+1}, k_{\bar{q}}l_{\bar{q}}, l_{\bar{q}}l_{\bar{q}+1}:1 \leq \bar{q} \leq n\}\) (see Figure 2). We denote the sets of edge metric co-ordinates for the edges of \(T_{n}\) by \(A_{1}\), \(A_{2}\), \(A_{3}\), \(A_{4}\), and \(A_{5}\), where \(A_{1}=\{\gamma_{E}(j_{\bar{q}}j_{\bar{q}+1}|R_{E}): 1 \leq \bar{q} \leq n\}\), \(A_{2}=\{\gamma_{E}(j_{\bar{q}}k_{\bar{q}}|R_{E}): 1 \leq \bar{q} \leq n\}\), \(A_{3}=\{\gamma_{E}(k_{\bar{q}}j_{\bar{q}+1}|R_{E}): 1 \leq \bar{q} \leq n\}\), \(A_{4}=\{\gamma_{E}(k_{\bar{q}}l_{\bar{q}}|R_{E}): 1 \leq \bar{q} \leq n\}\), and \(A_{5}=\{\gamma_{E}(l_{\bar{q}}l_{\bar{q}+1}|R_{E}): 1 \leq \bar{q} \leq n\}\).
In this section, we study some of the basic properties and the EMD of \(T_{n}\).
The convex polytope \(T_{n}\) [8] consists of \(3n\) and \(n\) number of vertices and edges respectively. It has \(n\) cycles with \(3\)-sides, \(n\) cycles with \(5\)-sides, and two cycles with \(n\)-sides (see Figure 2). The set of edges and vertices of \(T_{n}\) are denoted separately by \(E(T_{n})\) and \(V(T_{n})\), where \(E(T_{n})=\{j_{\bar{q}}j_{\bar{q}+1}, j_{\bar{q}}k_{\bar{q}}, k_{\bar{q}}j_{\bar{q}+1}, k_{\bar{q}}l_{\bar{q}}, l_{\bar{q}}l_{\bar{q}+1}: 1 \leq \bar{q} \leq n\}\) and \(V(T_{n})=\{j_{\bar{q}}, k_{\bar{q}}, l_{\bar{q}} :1 \leq \bar{q} \leq n\}\).
We name the vertices \(\{j_{\bar{q}}:1 \leq \bar{q} \leq n\}\) in the planar graph, \(T_{n}\) as the \(j\)-cycle vertices, the vertices \(\{k_{\bar{q}}:1 \leq \bar{q} \leq n\}\) in the planar graph, \(T_{n}\) as the \(k\)-vertices, and the vertices \(\{l_{\bar{q}} : 1 \leq \bar{q} \leq n\}\) in the planar graph, \(T_{n}\) as the \(l\)-cycle vertices. For our purpose, we can write \(j_{1}=j_{n+1}\), \(k_{1}=k_{n+1}\), and \(l_{1}=l_{n+1}\). In the present section, we consider a family of convex polytope graph \(T_{n}\) for which we have \(E(T_{n})=\{j_{\bar{q}}j_{\bar{q}+1}, j_{\bar{q}}k_{\bar{q}}, k_{\bar{q}}j_{\bar{q}+1}, k_{\bar{q}}l_{\bar{q}}, l_{\bar{q}}l_{\bar{q}+1}: 1 \leq \bar{q} \leq n\}\). We denote the sets of edge metric co-ordinates for the edges of \(T_{n}\) by \(\mathbb{A}\), \(\mathbb{B}\), and \(\mathbb{C}\), where \(\mathbb{A}=\{\gamma_{E}(j_{\bar{q}}j_{\bar{q}+1}|R_{E}), \gamma_{E}(j_{\bar{q}}k_{\bar{q}}|R_{E}): 1 \leq \bar{q} \leq n\}\), \(\mathbb{B}=\{\gamma_{E}(k_{\bar{q}}j_{\bar{q}+1}|R_{E}), \gamma_{E}(k_{\bar{q}}l_{\bar{q}}|R_{E}): 1 \leq \bar{q} \leq n\}\), and \(\mathbb{C}=\{\gamma_{E}(l_{\bar{q}}l_{\bar{q}+1}|R_{E}): 1 \leq \bar{q} \leq n\}\). In the following result, we investigate the EMD of \(T_{n}\).
Theorem 1. For \(n\geq6\), we have \[\begin{aligned} % \nonumber to remove numbering (before each equation) dim_{E}(T_{n}) = \begin{cases} 3, & if\ n=2h\ h\in\mathbb{N}; \\ 4, & if\ n=2h+1\ h\in\mathbb{N}. \end{cases} \end{aligned}\]
Proof. It is easy to check for \(6\leq n\leq 11\) that the EMD of \(T_{n}\) is 3 and 4, when the natural \(n\) is even and odd respectively. The position of the edge basis vertices (color in green) can be found in Figure 2, for all \(n\geq6\). Now, for \(n\geq 12\), we divide our proof into two cases i.e., when \(n\) is even (\(n \equiv 0\ (mod\ 2)\)) and when it is odd (\(n \equiv 1\ (mod\ 2)\)).
Then, for the natural \(n\), we have \(n = 2h\), where \(h \in \mathbb{N}\) and \(h \geq 6\). Suppose \(R_{E} = \{j_{1}, j_{h+1}, l_{2}\} \subset V(T_{n})\). Next, we give edge metric representation to every edge of \(T_{n}\) concerning the set \(R_{E}\). For the edges of \(j\)-cycle \(\{e_{\bar{q}}=j_{\bar{q}}j_{\bar{q}+1}| \bar{q}=1,2,3,…, n\}\), the edge codes are
\(\gamma_{E}(e_{\bar{q}} |R_{E})\) | \(R_{E} = \{j_{1}, j_{h+1}, l_{2}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(1 \leq \bar{q}\leq 2\)) | \((\bar{q}-1,h-\bar{q},2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(3 \leq \bar{q} \leq h\)) | \((\bar{q}-1,h-\bar{q},\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((2h-\bar{q},\bar{q}-h-1,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+2 \leq \bar{q} \leq 2h\)) | \((2h-\bar{q},\bar{q}-h-1,2h-\bar{q}+3)\) |
For the edges \(\{e_{\bar{q}}=j_{\bar{q}}k_{\bar{q}}, k_{\bar{q}}j_{\bar{q}+1}, k_{\bar{q}}l_{\bar{q}}| \bar{q}=1,2,3,…,n\}\), the edge codes are
\(\gamma_{E}(e_{\bar{q}}=j_{\bar{q}}k_{\bar{q}}|R_{E})\) | \(R_{E} = \{j_{1}, j_{h+1}, l_{2}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((\bar{q}-1,h-\bar{q}+1,2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(2 \leq \bar{q} \leq h+1\)) | \((\bar{q}-1,h-\bar{q}+1,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+2\)) | \((2h-\bar{q}+1,\bar{q}-h-1,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+3 \leq \bar{q} \leq 2h\)) | \((2h-\bar{q}+1,\bar{q}-h-1,2h-\bar{q}+3)\) |
\(\gamma_{E}(e_{\bar{q}}=k_{\bar{q}}j_{\bar{q}+1}|R_{E})\) | \(R_{E} = \{j_{1}, j_{h+1}, l_{2}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((\bar{q},h-\bar{q},2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(2 \leq \bar{q} \leq h\)) | \((\bar{q},h-\bar{q},\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((2h-\bar{q},\bar{q}-h,\bar{q}-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+2 \leq \bar{q} \leq 2h\)) | \((2h-\bar{q},\bar{q}-h,2h-\bar{q}+3)\) |
and
\(\gamma_{E}(e_{\bar{q}}=k_{\bar{q}}l_{\bar{q}}|R_{E})\) | \(R_{E} = \{j_{1}, j_{h+1}, l_{2}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((\bar{q},h-\bar{q}+1,1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(2 \leq \bar{q} \leq h\)) | \((\bar{q},h-\bar{q}+1,\bar{q}-2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((2h-\bar{q}+1,\bar{q}-h,\bar{q}-2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+2 \leq \bar{q} \leq 2h\)) | \((2h-\bar{q}+1,\bar{q}-h,2h-\bar{q}+2)\) |
Finally, for the edges of \(l\)-cycle \(\{e_{\bar{q}}=l_{\bar{q}}l_{\bar{q}+1}| \bar{q}=1,2,3,…,n\}\), the edge codes are
\(\gamma_{E}(e_{\bar{q}}=l_{\bar{q}}l_{\bar{q}+1}|R_{E})\) | \(R_{E} = \{j_{1}, j_{h+1}, l_{2}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((\bar{q}+1,h-\bar{q}+1,0)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(2 \leq \bar{q} \leq h-1\)) | \((\bar{q}+1,h-\bar{q}+1,\bar{q}-2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h\)) | \((\bar{q}+1,2,\bar{q}-2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((2h-\bar{q}+1,\bar{q}-h+1,\bar{q}-2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+2\leq \bar{q}\leq 2h-1\)) | \((2h-\bar{q}+1,\bar{q}-h+1,2h-\bar{q}+1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2h\)) | \((2,\bar{q}-h+1,2h-\bar{q}+1)\) |
From these edge codes in \(T_{n}\), we find that \(|A_{i}|=n\) (\(1\leq i \leq 5\)) and the sum of all of these cardinalities is equal to \(|E(T_{n})|\) and which is \(5n\). Moreover, all of these sets are pairwise disjoint, and so we find that no pair of two distinct edges in \(T_{n}\) are having the same edge metric coordinates, which implies that \(dim_{E}(T_{n})\leq 3\). Using proposition 3 we obtain \(dim_{E}(T_{n})= 3\), in this case.
From this, we have \(n = 2h+1\), where \(h \in \mathbb{N}\) and \(h \geq 6\). Suppose \(R_{E} = \{j_{1}, j_{h+1}, l_{2}, k_{h+2}\} \subset V(T_{n})\). Next, we give edge metric representation to every edge of \(T_{n}\) with respect to the set \(R_{E}\).
For the edges of \(j\)-cycle \(\{e_{\bar{q}}=j_{\bar{q}}j_{\bar{q}+1}| \bar{q}=1,2,3,…,n\}\), the edge codes are
\(\gamma_{E}(e_{\bar{q}} |R_{E})\) | \(R_{E} = \{j_{1}, j_{h+1}, l_{2}, k_{h+2}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((\bar{q}-1,h-\bar{q},2,h)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2\)) | \((\bar{q}-1,h-\bar{q},2,h-\bar{q}+2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(3 \leq \bar{q} \leq h\)) | \((\bar{q}-1,h-\bar{q},\bar{q}-1,h-\bar{q}+2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((\bar{q}-1,\bar{q}-h-1,\bar{q}-1,h-\bar{q}+2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+2\)) | \((2h-\bar{q}+1,\bar{q}-h-1,\bar{q}-1,1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+3 \leq \bar{q} \leq 2h+1\)) | \((2h-\bar{q}+1,\bar{q}-h-1,2h-\bar{q}+4,\bar{q}-h-2)\) |
For the edges \(\{e_{\bar{q}}=j_{\bar{q}}k_{\bar{q}}, k_{\bar{q}}j_{\bar{q}+1}, k_{\bar{q}}l_{\bar{q}}| \bar{q}=1,2,3,…,n\}\), the edge codes are
\(\gamma_{E}(e_{\bar{q}}=j_{\bar{q}}k_{\bar{q}}|R_{E})\) | \(R_{E} = \{j_{1}, j_{h+1}, l_{2}, k_{h+2}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((\bar{q}-1,h-\bar{q}+1,2,h)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(2 \leq \bar{q} \leq h+1\)) | \((\bar{q}-1,h-\bar{q}+1,\bar{q}-1,h-\bar{q}+3)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+2\)) | \((2h-\bar{q}+2,\bar{q}-h-1,\bar{q}-1,0)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+3 \leq \bar{q} \leq 2h+1\)) | \((2h-\bar{q}+2,\bar{q}-h-1,2h-\bar{q}+4,\bar{q}-h-2)\) |
\(\gamma_{E}(e_{\bar{q}}=k_{\bar{q}}j_{\bar{q}+1}|R_{E})\) | \(R_{E} = \{j_{1}, j_{h+1}, l_{2}, k_{h+2}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((\bar{q},h-\bar{q},2,h-\bar{q}+2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(2 \leq \bar{q} \leq h\)) | \((\bar{q},h-\bar{q},\bar{q}-1,h-\bar{q}+2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((2h-\bar{q}+1,\bar{q}-h,\bar{q}-1,h-\bar{q}+2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+2\)) | \((2h-\bar{q}+1,\bar{q}-h,\bar{q}-1,0)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+3 \leq \bar{q} \leq 2h\)) | \((2h-\bar{q}+1,\bar{q}-h,2h-\bar{q}+4,\bar{q}-h-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2h+1\)) | \((2h-\bar{q}+1,h,2h-\bar{q}+4,\bar{q}-h-1)\) |
and
\(\gamma_{E}(e_{\bar{q}}=k_{\bar{q}}l_{\bar{q}}|R_{E})\) | \(R_{E} = \{j_{1}, j_{h+1}, l_{2}, k_{h+2}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((\bar{q},h-\bar{q}+1,1,h+1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(2 \leq \bar{q} \leq h\)) | \((\bar{q},h-\bar{q}+1,\bar{q}-2,h-\bar{q}+3)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((\bar{q},\bar{q}-h,\bar{q}-2,h-\bar{q}+3)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+2\)) | \((2h-\bar{q}+2,\bar{q}-h,\bar{q}-2,0)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+3 \leq \bar{q} \leq 2h+1\)) | \((2h-\bar{q}+2,\bar{q}-h,2h-\bar{q}+3,\bar{q}-h-1)\) |
Finally, for the edges of \(l\)-cycle \(\{e_{\bar{q}}=l_{\bar{q}}l_{\bar{q}+1}| \bar{q}=1,2,3,…,n\}\), the edge codes are
\(\gamma_{E}(e_{\bar{q}}=l_{\bar{q}}l_{\bar{q}+1}|R_{E})\) | \(R_{E} = \{j_{1}, j_{h+1}, l_{2}, k_{h+2}\}\) |
---|---|
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=1\)) | \((\bar{q}+1,h-\bar{q}+1,0,h-\bar{q}+2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(2 \leq \bar{q} \leq h-1\)) | \((\bar{q}+1,h-\bar{q}+1,\bar{q}-2,h-\bar{q}+2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h\)) | \((\bar{q}+1,2,\bar{q}-2,h-\bar{q}+2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=h+1\)) | \((2h-\bar{q}+2,\bar{q}-h+1,\bar{q}-2,h-\bar{q}+2)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(h+2 \leq \bar{q} \leq 2h\)) | \((2h-\bar{q}+2,\bar{q}-h+1,2h-\bar{q}+2,\bar{q}-h-1)\) |
\(\gamma_{E}(e_{\bar{q}}|R_{E})\):(\(\bar{q}=2h+1\)) | \((2,h+1,2h-\bar{q}+2,\bar{q}-h-1)\) |
From these edge codes in \(T_{n}\), we find that \(|A_{i}|=n\) (\(1\leq i \leq 5\)) and the sum of all of these cardinalities is equal to \(|E(T_{n})|\) and which is \(5n\). Moreover, all of these sets are pairwise disjoint, and so we find that no pair of two distinct edges in \(T_{n}\) are having the same edge metric coordinates, which implies that \(dim_{E}(T_{n})\leq 4\). Now, to finish the proof for this case, we prove that \(dim_{E}(T_{n})\geq 4\) by proving that there is no set \(R_{E}\) with \(|R_{E}| = 3\), which can resolve every pair of distinct edges in \(T_{n}\). On the contrary, suppose \(dim_{E}(T_{n})=3\). Then, we have the following:
By symmetry of \(T_{n}\), other relations can be considered, and they will produce the same kind of contradictions. As a result, it can be found that \(dim_{E}(T_{n})=4\), when \(n\) is odd. ◻
Corollary 2. The minimum independent edge resolving set for \(T_{n}\) has cardinality three (for even \(n\)) and four (for odd \(n\)), for \(n \geq 6\).
Remark 2. For odd integer \(n\geq 7\), we have \(dim(T_{n})<dim_{E}(T_{n})\).
In this article, the edge metric dimension of two graphs \(S_{n}\) and \(T_{n}\) have been studied. For these classes of convex polytopes, we proved that \(dim_{E}(S_{n})=4\) and \(dim_{E}(T_{n})=3\) or \(4\). We also found that \(dim_{E}(S_{n})>dim(S_{n})\) for all \(n\), \(dim(T_{n})<dim_{E}(T_{n})\) for odd \(n\), and \(dim(T_{n})=dim_{E}(T_{n})\) for even \(n\) (a partial response to the problem reported in [14]). We also determined that the minimum edge metric generators for all of these convex polytopes are independent. In the future, we shall try to find the values for some other metric dimension variants such as fault-tolerant edge and vertex metric dimension, mixed metric dimension, local metric dimension etc. for the convex polytope families of graphs \(S_{n}\) and \(T_{n}\) [26].
Data sharing is not applicable to this article as no data set were generated or analyzed during the current study.
The authors declare no conflict of interest.
All the authors have equally contributed to the final manuscript.