<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">OALibJ</journal-id><journal-title-group><journal-title>Open Access Library Journal</journal-title></journal-title-group><issn pub-type="epub">2333-9705</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/oalib.1103050</article-id><article-id pub-id-type="publisher-id">OALibJ-71416</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject><subject> Business&amp;Economics</subject><subject> Chemistry&amp;Materials Science</subject><subject> Computer Science&amp;Communications</subject><subject> Earth&amp;Environmental Sciences</subject><subject> Engineering</subject><subject> Medicine&amp;Healthcare</subject><subject> Physics&amp;Mathematics</subject><subject> Social Sciences&amp;Humanities</subject></subj-group></article-categories><title-group><article-title>
 
 
  Soft Vibrational Force on Stock Market Networks
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Mehmet</surname><given-names>Ali Balci</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ömer</surname><given-names>Akgüller</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Mathematics, Mugla Sitki Kocman University, Mugla, Turkey</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>mehmetalibalci@mu.edu.tr(MAB)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>18</day><month>10</month><year>2016</year></pub-date><volume>03</volume><issue>10</issue><fpage>1</fpage><lpage>13</lpage><history><date date-type="received"><day>September</day>	<month>13,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>October</month>	<year>13,</year>	</date><date date-type="accepted"><day>October</day>	<month>17,</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  Stock market networks commonly involve uncertainty, and the theory of soft sets emerges as a powerful tool to handle it. In this study, we present a soft analogue of the differential of a vibrational potential function acting on a stock market network as vibrational force. For this purpose, we first study the vibrational potential function operating on each vertex by using the Laplacian of the neighborhood graph, then applied the soft approximator for the soft sets where the data points are embedded to Euclidean 
  n
   space. We used the data of the globally operating leading stock markets of 17 countries and prese
  nted the results respect to them.
 
</p></abstract><kwd-group><kwd>Network Modelling</kwd><kwd> Multivariate Analysis</kwd><kwd> Soft Analysis</kwd><kwd> Stock Exchange Network</kwd><kwd> Soft Set Theory</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Mathematical analysis of complex networks has become accepted since the more methodologies started to be used. The pioneering study is proposed by Mantegna in [<xref ref-type="bibr" rid="scirp.71416-ref1">1</xref>] , and long has been attracted several researchers. Analyzing networks with statistically and mathematically methods lets us get the topological properties of a market and its core information. Given stock market model uncertainty; soft, fuzzy, and rough com- puting techniques are viable candidates to capture stock market nonlinear relations. Recently, artificial neural networks and support vector machines have been applied to solve the problems of predicting financial stock market prediction [<xref ref-type="bibr" rid="scirp.71416-ref2">2</xref>] - [<xref ref-type="bibr" rid="scirp.71416-ref4">4</xref>] . Besides, studies in combination of neural networks with rough sets are used to predict the behavior of such stock markets [<xref ref-type="bibr" rid="scirp.71416-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.71416-ref6">6</xref>] .</p><p>One of the strong mathematical tool to deal with uncertainty is Soft Set Theory which is introduced in [<xref ref-type="bibr" rid="scirp.71416-ref7">7</xref>] . By the arise of the theory its algebraic [<xref ref-type="bibr" rid="scirp.71416-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.71416-ref9">9</xref>] and topological [<xref ref-type="bibr" rid="scirp.71416-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.71416-ref11">11</xref>] properties, its relation with other theories [<xref ref-type="bibr" rid="scirp.71416-ref12">12</xref>] - [<xref ref-type="bibr" rid="scirp.71416-ref14">14</xref>] , and also implicational feature of the theory [<xref ref-type="bibr" rid="scirp.71416-ref15">15</xref>] - [<xref ref-type="bibr" rid="scirp.71416-ref18">18</xref>] have been studied intensively. We refer [<xref ref-type="bibr" rid="scirp.71416-ref19">19</xref>] to the interested readers for soft set theoretical analogues of the basic set operations.</p><p>In this study we first consider a financial network which is constructed from the correlation of daily logarithmic return of the closure price of globally leading 17 stock markets. As a common approach, this network is modelled as the tuple <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x2.png" xlink:type="simple"/></inline-formula> where the V is the set of vertices, that is the stock markets, and E is the set of edges or links in the network. G is considered as an undirected simple graph throughout the study. For basic operations and well-known concepts about the graph theory, we refer interested readers to [<xref ref-type="bibr" rid="scirp.71416-ref20">20</xref>] . It can also be seen that a soft set is not a set but set systems, hence there is a strong correspondence between the theories of Soft Sets and Hypergraphs. Henceforth, to apply soft set theoretical concepts to networks, we first obtain a hypergraph representation of the network by using k-neighborhood of a graph vertex. In Section 3, we explain this correspondence in details. Also, since each stock market is represented with time series we present a soft approximator in Section 3. This approximator can also be seen as the soft analogue of the subgradient. In Section 4, we present a new function called “vibrational potential energy” that operating on each vertex of the network. Any kind of local or global economic stress or crisis in a stock market directly affects its neighboring stock markets. Therefore, we defined our function respect to neighborhood graph Laplacian rather than the one that is introduced in [<xref ref-type="bibr" rid="scirp.71416-ref21">21</xref>] . Finally, in Section 5, we present the data and the algorithm to construct networks with respect to graph spectrum that is used to obtain results. In this section, the results can also be found in details.</p></sec><sec id="s2"><title>2. Preliminaries</title><p>The tuple <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x3.png" xlink:type="simple"/></inline-formula> is called an undirected graph for the the vertices or nodes set V and the edge or links set E. Each elements of E is an unordered pair of vertices that is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x4.png" xlink:type="simple"/></inline-formula>. For any vertices <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x5.png" xlink:type="simple"/></inline-formula> the graph G is called connected if there is a path , i.e. a sequence of edges, whose end points are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x6.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x7.png" xlink:type="simple"/></inline-formula>. The complete graph is an undirected graph with every pair of apart vertices is connected by an edge. In the case of real world data representation, each edge in E may be assigned by a non-- negative numerical value. This value is called as a weigh and for the mapping<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x8.png" xlink:type="simple"/></inline-formula>, the triple <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x9.png" xlink:type="simple"/></inline-formula> is called as a weighted graph.</p><p>A common way to represent a graph is using a binary matrix whose elements are</p><disp-formula id="scirp.71416-formula128"><graphic  xlink:href="http://html.scirp.org/file/71416x10.png"  xlink:type="simple"/></disp-formula><p>This matrix is called adjacency matrix and symmetric by the definition. This symmetry property concludes that the adjacency matrix has orthonormal basis of eigenvectors and the number of vertices many eigenvalues.</p><p>For a vertex v in an undirected graph G, the number of edges incident to that vertex is called degree and let us denote it by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x11.png" xlink:type="simple"/></inline-formula>. For the graph<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x12.png" xlink:type="simple"/></inline-formula>, the Laplacian Matrix of G is the matrix whose entries are</p><disp-formula id="scirp.71416-formula129"><graphic  xlink:href="http://html.scirp.org/file/71416x13.png"  xlink:type="simple"/></disp-formula><p>The graph Laplacian does not depend on an ordering of the vertices of G. Let us now denote the spectrum of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x14.png" xlink:type="simple"/></inline-formula> by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x15.png" xlink:type="simple"/></inline-formula> for the graph with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x16.png" xlink:type="simple"/></inline-formula>. The Laplacian is positive-semidefinite, i.e. all of its eigenvalues have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x17.png" xlink:type="simple"/></inline-formula> with the least one 0. For an undirected graph with nonnegative weights, the multiplicity k of the eigenvalue 0 of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x18.png" xlink:type="simple"/></inline-formula> equals the number of connected components <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x19.png" xlink:type="simple"/></inline-formula> in the graph [<xref ref-type="bibr" rid="scirp.71416-ref22">22</xref>] .</p><p>Consider a graph<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x20.png" xlink:type="simple"/></inline-formula>. Now if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x21.png" xlink:type="simple"/></inline-formula> and there are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x22.png" xlink:type="simple"/></inline-formula> edges such that some one point, v, is directly connected or adjacent to all of the others, G is a n-star. A neighborhood graph, then, is any graph of n points that contains a n-star. The neighborhood graph of a given graph from a vertex v can also be seen as the subgraph induced by the neighborhood of a graph from vertex v [<xref ref-type="bibr" rid="scirp.71416-ref23">23</xref>] .</p></sec><sec id="s3"><title>3. Soft Analysis</title><p>Classical analysis concepts may not be as powerful as the soft computing concepts to deal with real world data since the uncertainty. One of the powerful tool to deal with uncertainty is Soft Set Theory that is first introduced by Molodtsov in [<xref ref-type="bibr" rid="scirp.71416-ref7">7</xref>] . This theory differs from the theories of same kind like rough sets, vague sets, and fuzzy sets theories by the qualifying the parameters.</p><p>Definition 3.1. Let A be a subset of E. A pair <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x23.png" xlink:type="simple"/></inline-formula> is called a soft set over U where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x24.png" xlink:type="simple"/></inline-formula> is a set-valued function.</p><p>It is possible to conclude that a soft set over U is a parameterized family of subsets of the universe U. It is also common to consider a soft set as the approximate descriptions of an object [<xref ref-type="bibr" rid="scirp.71416-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.71416-ref19">19</xref>] . For a real valued function, the concept of soft approximation of a function is defined and studied deeply in [<xref ref-type="bibr" rid="scirp.71416-ref7">7</xref>] . However, we need an extended definition for the soft sets whose points are embedded in Euclidean n-dimensional space:</p><p>Definition 3.2. Let E be <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x25.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x26.png" xlink:type="simple"/></inline-formula> with an intrinsic metric. For every point<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x27.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x28.png" xlink:type="simple"/></inline-formula>is defined as an open ball centered to the point x with the radius<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x29.png" xlink:type="simple"/></inline-formula>. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x30.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x31.png" xlink:type="simple"/></inline-formula> be positive numbers. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x32.png" xlink:type="simple"/></inline-formula>the set</p><disp-formula id="scirp.71416-formula130"><graphic  xlink:href="http://html.scirp.org/file/71416x33.png"  xlink:type="simple"/></disp-formula><p>is called <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x34.png" xlink:type="simple"/></inline-formula>-approximator of function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x35.png" xlink:type="simple"/></inline-formula> at the point x, where “<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x36.png" xlink:type="simple"/></inline-formula>” is an inner product.</p><p>The approximator given in Definition 3.2 can be seen as the three parameter approximator that is dealt in Non-differentiable Optimization. For more see [<xref ref-type="bibr" rid="scirp.71416-ref24">24</xref>] . It is also straightforward to show the basic properties such as linearity and convexity of the soft approximator.</p><p>From the mathematical point of view, a soft set is a set-valued function that maps parameters to the subset a universe. Frankly, similar mathematical settings such as Formal Concept Analysis [<xref ref-type="bibr" rid="scirp.71416-ref25">25</xref>] , Spatial Analysis [<xref ref-type="bibr" rid="scirp.71416-ref26">26</xref>] , and Hypergraphs [<xref ref-type="bibr" rid="scirp.71416-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.71416-ref28">28</xref>] have been studied extensively. A striking example is the concept of Hypergraphs. Hypergra- phs are the generalization of simple graphs in such way that an edge may include more than two vertices. When a hypergraph occurs as a set system one may correspond it as a soft set.</p><p>For an illustrative example let us consider the hypergraph model given in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The hypergraph that is given as a tuple <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x37.png" xlink:type="simple"/></inline-formula> with the vertex set</p><disp-formula id="scirp.71416-formula131"><graphic  xlink:href="http://html.scirp.org/file/71416x38.png"  xlink:type="simple"/></disp-formula><p>and the hyperedge set</p><disp-formula id="scirp.71416-formula132"><graphic  xlink:href="http://html.scirp.org/file/71416x39.png"  xlink:type="simple"/></disp-formula><p>naturally revokes the soft set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x40.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.71416-formula133"><graphic  xlink:href="http://html.scirp.org/file/71416x41.png"  xlink:type="simple"/></disp-formula></sec><sec id="s4"><title>4. Vibrational Potential</title><p>Whenever a complex network is under consideration, some of the physical concepts can be helpful to analyze it. One of these concepts is called Vibrational Potential and can be interpreted by immersing the network into a thermal bath, then analyzing the displacement of a node from its equilibrium under the small perturbations in the network. The vibrational potential energy of the network can be given as</p><disp-formula id="scirp.71416-formula134"><graphic  xlink:href="http://html.scirp.org/file/71416x42.png"  xlink:type="simple"/></disp-formula><p>where k is the spring constant, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x43.png" xlink:type="simple"/></inline-formula>is the graph Laplacian, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x44.png" xlink:type="simple"/></inline-formula> is the vector whose i-th entry is the displacement<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x45.png" xlink:type="simple"/></inline-formula>. The vibrational potential of a network is studied deeply in [<xref ref-type="bibr" rid="scirp.71416-ref21">21</xref>] .</p><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> A hypergraph example.</title></caption><fig id ="fig1_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/71416x46.png"/></fig></fig-group><p>In this study we aim to investigate the change of the vibrational potentials under the soft approximators. Henceforth, the definition of a real valued function defined on the nodes of a network is needed. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x47.png" xlink:type="simple"/></inline-formula> be the simple undirected graph repre- sentation of a network under consideration with the node set V and the link set E. For a complex network such as stock market network, a thermal bath can be seen as the global economic crisis or local economic stress that effects the network. Henceforth, the assumption of the node in a financial network is mostly effected by its neighborhood markets do not contradict to the neoclassical theory of economics. By this assumption, we may express the vibrational potential energy of the node in the network as</p><disp-formula id="scirp.71416-formula135"><graphic  xlink:href="http://html.scirp.org/file/71416x48.png"  xlink:type="simple"/></disp-formula><p>where k is the spring constant, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x49.png" xlink:type="simple"/></inline-formula>is the Laplacian of the neighborhood graph <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x50.png" xlink:type="simple"/></inline-formula> of the node v in the network G, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x51.png" xlink:type="simple"/></inline-formula> is the vector whose i-th entry is the displacement <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x52.png" xlink:type="simple"/></inline-formula> in the neighborhood graph<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x53.png" xlink:type="simple"/></inline-formula>.</p><p>The mean displacement of a node <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x54.png" xlink:type="simple"/></inline-formula> in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x55.png" xlink:type="simple"/></inline-formula> can be expressed by</p><disp-formula id="scirp.71416-formula136"><graphic  xlink:href="http://html.scirp.org/file/71416x56.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x57.png" xlink:type="simple"/></inline-formula> is the probability distribution</p><disp-formula id="scirp.71416-formula137"><graphic  xlink:href="http://html.scirp.org/file/71416x58.png"  xlink:type="simple"/></disp-formula><p>with</p><disp-formula id="scirp.71416-formula138"><graphic  xlink:href="http://html.scirp.org/file/71416x59.png"  xlink:type="simple"/></disp-formula><p>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x60.png" xlink:type="simple"/></inline-formula> is the inverse temperature. The mean square of the displacement of the i-th node can be given as</p><disp-formula id="scirp.71416-formula139"><graphic  xlink:href="http://html.scirp.org/file/71416x61.png"  xlink:type="simple"/></disp-formula><p>Using the unification methods that presented in [<xref ref-type="bibr" rid="scirp.71416-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.71416-ref29">29</xref>] the mean square of the displacement can also be computed as</p><disp-formula id="scirp.71416-formula140"><graphic  xlink:href="http://html.scirp.org/file/71416x62.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x63.png" xlink:type="simple"/></inline-formula> is the Moore-Penrose generalised inverse of the neighborhood graph Laplacian<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x64.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s5"><title>5. Experimental Verification</title><p>As pointed out in Section 3, a hypergraph naturally yields a soft set. In this section we present a method to construct a soft set from a financial network and then consider the soft derivatives of the vibrational potentials acting on the nodes of the network that are globally operating stock markets and name after “soft vibrational force”. For a stock market network represented by a simple graph, k-neighborhood of vertices yields a cluster of vertex set. Henceforth, a hypergraph representation for stock market network can be obtained by k-neighborhoods. Since a crisis or stress mostly effect stock markets that are mostly correlated, we use 1-neighborhood to obtain a soft set representation of the stock market. After we introduced the real valued vibrational potential function that operates on vertices separately in Section 4, the soft vibrational force on stock markets can be computed as</p><disp-formula id="scirp.71416-formula141"><graphic  xlink:href="http://html.scirp.org/file/71416x65.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x66.png" xlink:type="simple"/></inline-formula> is the set of vertices in the 1-neighborhood of each stock market.</p><sec id="s5_1"><title>5.1. Data</title><p>The data we used in this study are obtained from the stock markets that operating in America, Europe, and Asia in the time scale from 02.01.2006 to 29.02.2016. Those stock markets are Holland (AEX), Austria (ATX), Turkey (BIST), France (CAC), Germany (DAX), USA (DOW, NASDAQ, SP500), European Union (EUSTOX), UK (FTSE), Mexica (IPC), South Korea (KOSPI), Argentina (MERVAL), Japan (NIKKEI), Switzerland (SMI), Israel (TELAVIV), and Taiwan (TSEC).</p><p>For the daily closure price <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x67.png" xlink:type="simple"/></inline-formula> of the i-th stock market, the daily logarithmic return is calculated as</p><disp-formula id="scirp.71416-formula142"><graphic  xlink:href="http://html.scirp.org/file/71416x68.png"  xlink:type="simple"/></disp-formula><p>To catch optimized many links between the stocks, we use the Pearson correlation of each stock as</p><disp-formula id="scirp.71416-formula143"><graphic  xlink:href="http://html.scirp.org/file/71416x69.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x70.png" xlink:type="simple"/></inline-formula> is a temporal average performed on all the trading days of the investigated time period, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x71.png" xlink:type="simple"/></inline-formula>are the numerical labels of stocks, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x72.png" xlink:type="simple"/></inline-formula>. By the introduction of the distance function respect to correlation coefficients as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x73.png" xlink:type="simple"/></inline-formula>. Since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x74.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x75.png" xlink:type="simple"/></inline-formula>for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x76.png" xlink:type="simple"/></inline-formula>. The matrix D whose <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x77.png" xlink:type="simple"/></inline-formula>-th entry is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x78.png" xlink:type="simple"/></inline-formula> is also called as correlation distance matrix of the network. The correlation distance matrix respect to aforementioned data set is given in <xref ref-type="fig" rid="fig2">Figure 2</xref>. As <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x79.png" xlink:type="simple"/></inline-formula> varies 0 to 1, the colour in the figure varies white to black, respectively.</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> The monochromatic representation of the correlation distance matrix D</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/71416x80.png"/></fig></sec><sec id="s5_2"><title>5.2. Network Construction</title><p>Respect to the correlation distance matrix, it is possible to construct the network as threshold distance sense. Since our analysis depends on connectedness of the network, we may use the spectrum of the simple graph representation to determine boundary to the threshold. The well-known theorem from spectral graph theory states that the multiplicity k of the eigenvalue 0 of the graph Laplacian equals the number of connected components in the graph. Our method to construct network first starts with n-complete graph; i.e., a graph with all vertices are adjacent. Then by subdividing <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x81.png" xlink:type="simple"/></inline-formula> interval with h step, we determine the boundary as the greatest value where the correlation distance between each vertex is less and equal to and the graph remains with one component. The algorithm is given in <xref ref-type="table" rid="table1">Table 1</xref> in pseudo-codes.</p></sec><sec id="s5_3"><title>5.3. Results</title><p>Let us label vertices as the rule given in <xref ref-type="table" rid="table2">Table 2</xref> throughout the study.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> An Algorithm to determine the boundary for threshold distance</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Input:</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x82.png" xlink:type="simple"/></inline-formula>: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x83.png" xlink:type="simple"/></inline-formula>type matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x84.png" xlink:type="simple"/></inline-formula>: fraction size</th></tr></thead><tr><td align="center" valign="middle" >Initial:</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x85.png" xlink:type="simple"/></inline-formula>: n-complete graph with the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x86.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x87.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >while Number of 0 eigenvalue of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x88.png" xlink:type="simple"/></inline-formula> do <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x89.png" xlink:type="simple"/></inline-formula>; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x90.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x91.png" xlink:type="simple"/></inline-formula> to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x92.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x93.png" xlink:type="simple"/></inline-formula> to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x94.png" xlink:type="simple"/></inline-formula> if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x95.png" xlink:type="simple"/></inline-formula> then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x96.png" xlink:type="simple"/></inline-formula> end if end for end for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x97.png" xlink:type="simple"/></inline-formula>&#172; Graph with the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x98.png" xlink:type="simple"/></inline-formula> Compute the Eigenvalues of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x99.png" xlink:type="simple"/></inline-formula> end while</td></tr><tr><td align="center" valign="middle" >Output:</td><td align="center" valign="middle" >Boundary for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x100.png" xlink:type="simple"/></inline-formula></td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Vertex labelling rule for the stock market network</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x101.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x102.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x103.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x104.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x105.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x106.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x107.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x108.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x109.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x110.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x111.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x112.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x113.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x114.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x115.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x116.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x117.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><p>For the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x118.png" xlink:type="simple"/></inline-formula> the boundary of the network to be connected is 0.86. The respected network is given in <xref ref-type="fig" rid="fig3">Figure 3</xref>. This network structure preserves really strong connections between the nodes. However, these kind of links do not accurately model the real world situation. For instance, in this network NASDAQ is only connected to TELAVIV. However, it is well known that USA stock markets are effective in stock market networks [<xref ref-type="bibr" rid="scirp.71416-ref30">30</xref>] - [<xref ref-type="bibr" rid="scirp.71416-ref32">32</xref>] . Hence, for our study we choose a more accurate network for the threshold distance 0.8 as in <xref ref-type="fig" rid="fig4">Figure 4</xref>.</p><p>The 1-neighborhood of each node yields the following soft set for this network:</p><disp-formula id="scirp.71416-formula144"><graphic  xlink:href="http://html.scirp.org/file/71416x119.png"  xlink:type="simple"/></disp-formula><p>The neighborhood graphs of each elements of the soft set can be obtained by considering the network. In <xref ref-type="fig" rid="fig5">Figure 5</xref> two of the examples of neighborhood graphs are presented. The left on is for BIST and the right one is for NASDAQ.</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> The network with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x121.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/71416x120.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> The network with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x123.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/71416x122.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> The neighborhood graphs of BIST and NASDAQ</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/71416x124.png"/></fig><p>Since our soft approximation definition relies on the intrinsic metric of the network and the nodes are the time series of the each stock markets daily logarithmic return, we compute the soft differential analogue of the vibrational potential function operating on each node as</p><disp-formula id="scirp.71416-formula145"><graphic  xlink:href="http://html.scirp.org/file/71416x125.png"  xlink:type="simple"/></disp-formula><p>where the inner product arise from the standard correlation distance.</p><p>For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x126.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x127.png" xlink:type="simple"/></inline-formula>, resulting soft vibrational force is:</p><disp-formula id="scirp.71416-formula146"><graphic  xlink:href="http://html.scirp.org/file/71416x128.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula147"><graphic  xlink:href="http://html.scirp.org/file/71416x129.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula148"><graphic  xlink:href="http://html.scirp.org/file/71416x130.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula149"><graphic  xlink:href="http://html.scirp.org/file/71416x131.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula150"><graphic  xlink:href="http://html.scirp.org/file/71416x132.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula151"><graphic  xlink:href="http://html.scirp.org/file/71416x133.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula152"><graphic  xlink:href="http://html.scirp.org/file/71416x134.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula153"><graphic  xlink:href="http://html.scirp.org/file/71416x135.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula154"><graphic  xlink:href="http://html.scirp.org/file/71416x136.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula155"><graphic  xlink:href="http://html.scirp.org/file/71416x137.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula156"><graphic  xlink:href="http://html.scirp.org/file/71416x138.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula157"><graphic  xlink:href="http://html.scirp.org/file/71416x139.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula158"><graphic  xlink:href="http://html.scirp.org/file/71416x140.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula159"><graphic  xlink:href="http://html.scirp.org/file/71416x141.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula160"><graphic  xlink:href="http://html.scirp.org/file/71416x142.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula161"><graphic  xlink:href="http://html.scirp.org/file/71416x143.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula162"><graphic  xlink:href="http://html.scirp.org/file/71416x144.png"  xlink:type="simple"/></disp-formula><p>and for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x145.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x146.png" xlink:type="simple"/></inline-formula>, resulting soft vibrational force is:</p><disp-formula id="scirp.71416-formula163"><graphic  xlink:href="http://html.scirp.org/file/71416x147.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula164"><graphic  xlink:href="http://html.scirp.org/file/71416x148.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula165"><graphic  xlink:href="http://html.scirp.org/file/71416x149.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula166"><graphic  xlink:href="http://html.scirp.org/file/71416x150.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula167"><graphic  xlink:href="http://html.scirp.org/file/71416x151.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula168"><graphic  xlink:href="http://html.scirp.org/file/71416x152.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula169"><graphic  xlink:href="http://html.scirp.org/file/71416x153.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula170"><graphic  xlink:href="http://html.scirp.org/file/71416x154.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula171"><graphic  xlink:href="http://html.scirp.org/file/71416x155.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula172"><graphic  xlink:href="http://html.scirp.org/file/71416x156.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula173"><graphic  xlink:href="http://html.scirp.org/file/71416x157.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula174"><graphic  xlink:href="http://html.scirp.org/file/71416x158.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula175"><graphic  xlink:href="http://html.scirp.org/file/71416x159.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula176"><graphic  xlink:href="http://html.scirp.org/file/71416x160.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula177"><graphic  xlink:href="http://html.scirp.org/file/71416x161.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula178"><graphic  xlink:href="http://html.scirp.org/file/71416x162.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.71416-formula179"><graphic  xlink:href="http://html.scirp.org/file/71416x163.png"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s6"><title>6. Conclusions</title><p>Certain kinds of real world problems are hard to model by using only classical ideas. Hence, theories involving uncertainty, vagueness, or parameters such as soft set theory may be helpful to analyze these kinds of models. In this paper, we give a new soft approximation idea where each elements are described as a time series; i.e., embedded in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x164.png" xlink:type="simple"/></inline-formula>. Networks are usually modelled by simple graphs and involve an instinct metric. Therefore by introducing the soft set representation which arise from the hypergraph of a simple network respect to k-neighborhood, it is possible to use this soft approxima- tion on networks. Especially, we consider stock market networks in this study but it is also possible to extend this approach to other complex networks such as social networks, computer networks, biological networks etc. [<xref ref-type="bibr" rid="scirp.71416-ref33">33</xref>] [<xref ref-type="bibr" rid="scirp.71416-ref34">34</xref>] . To analyze soft analo- gue of the differential of a function acting on a network, we introduced vibrational potential function that is defined by the neighborhood graph of 1-neighborhood the vertices of the network under consideration. This function differs from the one that is given in [<xref ref-type="bibr" rid="scirp.71416-ref21">21</xref>] by using the Moore-Penrose inverse of the neighborhood graph.</p><p>The network we use in this study is constructed from the stock market’s daily logarithmic return of the closure price by a predetermined threshold distance and the correlation distance between each data. The upper boundary for the distance is 0.86, hence we used 0.8 to obtain more accurate results. By introducing the vibrational potential function operating on vertices, we analyzed the soft approximation of the function and softly-computed the vibrational force acting on the network. For the parameters <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x165.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x166.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x167.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/71416x168.png" xlink:type="simple"/></inline-formula> it can be concluded that a global economic crisis is mostly affect the small European economies such as Holland (AEX), Austria (ATX), and Turkey (BIST). The European Union Stock Market (EUSTOX) and DOW of USA are affected mostly from the leading global economies.</p></sec><sec id="s7"><title>Cite this paper</title><p>Balcı, M.A. and Akg&#252;ller, &#214;. (2016) Soft Vibrational Force on Stock Market Networks. Open Access Library Journal, 3: e3050. http://dx.doi.org/10.4236/oalib.1103050</p></sec></body><back><ref-list><title>References</title><ref id="scirp.71416-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Mantegna, R.N. (1999) Hierarchical Structure in Financial Markets. The European Physical Journal B-Condensed Matter and Complex Systems, 11, 193-197. http://dx.doi.org/10.1007/s100510050929</mixed-citation></ref><ref id="scirp.71416-ref2"><label>2</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Avc</surname><given-names> E. </given-names></name>,<etal>et al</etal>. 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