<?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">TEL</journal-id><journal-title-group><journal-title>Theoretical Economics Letters</journal-title></journal-title-group><issn pub-type="epub">2162-2078</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/tel.2016.63056</article-id><article-id pub-id-type="publisher-id">TEL-67228</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Business&amp;Economics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Symmetric Stability in Symmetric Games
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Andreas</surname><given-names>Hefti</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>School of Management and Law, University of Zurich, Winterthur, Switzerland</addr-line></aff><author-notes><corresp id="cor1">* E-mail:</corresp></author-notes><pub-date pub-type="epub"><day>31</day><month>05</month><year>2016</year></pub-date><volume>06</volume><issue>03</issue><fpage>488</fpage><lpage>493</lpage><history><date date-type="received"><day>29</day>	<month>March</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>6</month>	<year>June</year>	</date><date date-type="accepted"><day>9</day>	<month>June</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>
 
 
  The idea of symmetric stability of symmetric equilibria is introduced which is relevant, e.g., for the comparative-statics of symmetric equilibria with symmetric shocks. I show that symmetric stability can be expressed in a two-player reduced-form version of the 
  N
  -player game, derive an elementary relation between symmetric stability and the existence of exactly one symmetric 
  equilibrium, and apply symmetric stability to a two-dimensional 
  N
  -player contest.
 
</p></abstract><kwd-group><kwd>Symmetric Games</kwd><kwd> Symmetric Equilibrium</kwd><kwd> Stability</kwd><kwd> Uniqueness</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In this note I develop the idea of symmetric stability of symmetric equilibria in symmetric N-player games. With symmetric equilibria it is reasonable to consider dynamics where the set of trajectories is restricted by symmetric initial conditions. This is particularly relevant when studying the comparative-statics of symmetric equilibria to a common shock, such as changing the prize in a contest or a tax parameter in the Cournot model, since this has symmetric effects on symmetric players both in terms of the initial displacement and the subsequent adjustment process. Symmetric stability conditions can be expressed in terms of a best-reply function obtained by fixing the strategies of all other players to the same action. Given a k-dimensional strategy space, this reduces the dimensionality of the stability problem from Nk to k, while retaining all relevant information about symmetric equilibria and their symmetric stability. By means of this reduced form I prove that the existence of a single symmetric equilibrium is the same formal property as global symmetric stability in regular one-dimensional games, independent of the number of players. Further, stability under symmetric adjustments implies the existence of only one symmetric equilibrium for any finite-dimensional strategy space, and symmetric stability provides a meaningful restriction for the possible comparative-static patterns of symmetric equilibria. All results are independent of the possible existence of asymmetric equilibria, and the practical usefulness of symmetric stability is briefly illustrated by means of a two-dimensional N-player contest.</p></sec><sec id="s2"><title>2. Symmetric Games</title><p>I consider games of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x6.png" xlink:type="simple"/></inline-formula> players. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x7.png" xlink:type="simple"/></inline-formula>is a strategy of player g, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x8.png" xlink:type="simple"/></inline-formula></p><p>with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x9.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x10.png" xlink:type="simple"/></inline-formula>, and interior<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x11.png" xlink:type="simple"/></inline-formula>. All players have identical strategy space. The payoff of g</p><p>is represented by a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x12.png" xlink:type="simple"/></inline-formula> function<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x13.png" xlink:type="simple"/></inline-formula>, which is strongly quasiconcave<sup>1</sup> in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x14.png" xlink:type="simple"/></inline-formula>. In a symmetric game all players have identical payoff function in the sense that</p><disp-formula id="scirp.67228-formula9"><graphic  xlink:href="http://html.scirp.org/file/16-1500875x15.png"  xlink:type="simple"/></disp-formula><p>for any permutation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x16.png" xlink:type="simple"/></inline-formula> of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x17.png" xlink:type="simple"/></inline-formula>. With the above assumptions, player g’s best-reply function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x18.png" xlink:type="simple"/></inline-formula> is continuous, and differentiable at interior points. Given the focus on symmetric equilibria one can restrict attention to a reduced-form problem by picking an indicative player (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x19.png" xlink:type="simple"/></inline-formula>), and requiring all</p><p>opponents to play the same strategies, i.e.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x20.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x21.png" xlink:type="simple"/></inline-formula>. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x22.png" xlink:type="simple"/></inline-formula> with correspond-</p><p>ing best-reply <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x23.png" xlink:type="simple"/></inline-formula> and derivative<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x24.png" xlink:type="simple"/></inline-formula>. Any symmetric equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x25.png" xlink:type="simple"/></inline-formula> is identifiable by its first projection<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x26.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x27.png" xlink:type="simple"/></inline-formula>is a symmetric equilibrium if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x28.png" xlink:type="simple"/></inline-formula>, a symmetric equilibrium always exists and the set of symmetric equilibria is compact [<xref ref-type="bibr" rid="scirp.67228-ref1">1</xref>] .</p><sec id="s2_1"><title>2.1. Symmetric Stability</title><p>I mostly restrict attention to the system of gradient dynamics<sup>2</sup></p><disp-formula id="scirp.67228-formula10"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-1500875x29.png"  xlink:type="simple"/></disp-formula><p>where S is a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x37.png" xlink:type="simple"/></inline-formula> positive-diagonal adjustment matrix, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x38.png" xlink:type="simple"/></inline-formula>. A solution to (1) has the</p><p>form<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x39.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x40.png" xlink:type="simple"/></inline-formula> is the trajectory of j. I consider a restricted version of this trajectory map, where initial values <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x41.png" xlink:type="simple"/></inline-formula> are symmetric, i.e.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x42.png" xlink:type="simple"/></inline-formula>. Then, by symmetry, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x43.png" xlink:type="simple"/></inline-formula>is the same for all players and solves</p><disp-formula id="scirp.67228-formula11"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-1500875x44.png"  xlink:type="simple"/></disp-formula><p>I say that an interior symmetric equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x45.png" xlink:type="simple"/></inline-formula> is symmetrically stable if the dynamics induced by (2) converge to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x46.png" xlink:type="simple"/></inline-formula> whenever <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x47.png" xlink:type="simple"/></inline-formula> is close to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x48.png" xlink:type="simple"/></inline-formula>.<sup>3</sup> Hence:</p><p>Definition 1 (Symmetric stability) The symmetric equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x49.png" xlink:type="simple"/></inline-formula> is symmetrically stable if all eigenvalues of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x50.png" xlink:type="simple"/></inline-formula>, the Jacobian corresponding to (2), have negative real parts.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x51.png" xlink:type="simple"/></inline-formula>is symmetrically unstable if at least one eigenvalue of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x52.png" xlink:type="simple"/></inline-formula> has positive real part. Stability of (1) implies symmetric stability, but not vice-versa (see <xref ref-type="fig" rid="fig1">Figure 1</xref>). Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x53.png" xlink:type="simple"/></inline-formula>, and note that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x54.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x55.png" xlink:type="simple"/></inline-formula>is a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x56.png" xlink:type="simple"/></inline-formula>-vector field with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x57.png" xlink:type="simple"/></inline-formula> Jacobian<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x58.png" xlink:type="simple"/></inline-formula>. A symmetric game is</p><p>(symmetrically) regular if i) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x59.png" xlink:type="simple"/></inline-formula>has only regular zeroes<sup>4</sup> and ii) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x60.png" xlink:type="simple"/></inline-formula>points inwards at the boundary of S. Any future reference to a regular game means “symmetrically” regular, which is a weaker condition than general regularity of a symmetric game (see [<xref ref-type="bibr" rid="scirp.67228-ref2">2</xref>] ). The first theorem below reveals the general connection between symmetric stability and the existence of a single symmetric equilibrium, depending on the dimensionality of the strategy space. Its proof exploits an essential relation between<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x61.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x62.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x63.png" xlink:type="simple"/></inline-formula>.</p><p>Lemma 1 For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x64.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.67228-formula12"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-1500875x65.png"  xlink:type="simple"/></disp-formula><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Stable (left) and only symmetrically stable (right)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/16-1500875x66.png"/></fig><p>Proof: The first equality is immediate. Next, decompose<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x67.png" xlink:type="simple"/></inline-formula>. By the Implicit Function Theorem (IFT) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x68.png" xlink:type="simple"/></inline-formula>which, together with the decomposition of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x69.png" xlink:type="simple"/></inline-formula> gives the second equality. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x70.png" xlink:type="simple"/></inline-formula></p><p>Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x71.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x72.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x73.png" xlink:type="simple"/></inline-formula> is the a-th projection of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x74.png" xlink:type="simple"/></inline-formula>.</p><p>Theorem 1 (i) If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x75.png" xlink:type="simple"/></inline-formula> then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x76.png" xlink:type="simple"/></inline-formula> is a symmetrically stable equilibrium if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x77.png" xlink:type="simple"/></inline-formula> or equivalently if</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x78.png" xlink:type="simple"/></inline-formula>.</p><p>(ii) For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x79.png" xlink:type="simple"/></inline-formula> a symmetric equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x80.png" xlink:type="simple"/></inline-formula> is symmetrically stable if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x81.png" xlink:type="simple"/></inline-formula> has only positive principal minors.</p><p>(iii) If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x82.png" xlink:type="simple"/></inline-formula> and a regular games has multiple symmetric equilibria, then there is at least one symmetrically unstable equilibrium.</p><p>Proof: (i) Follows from lemma 1. (ii) Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x90.png" xlink:type="simple"/></inline-formula> be the eigenvalues of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x91.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x92.png" xlink:type="simple"/></inline-formula> be the diagon-</p><p>al entries of S. Lemma 1 and the condition in (ii) imply <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x93.png" xlink:type="simple"/></inline-formula> and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x94.png" xlink:type="simple"/></inline-formula>. Hence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x95.png" xlink:type="simple"/></inline-formula> have negative real parts. (iii) Follows from applying the Index theorem to the symmetric gradient field<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x96.png" xlink:type="simple"/></inline-formula>.<sup>5</sup> The index of a zero of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x97.png" xlink:type="simple"/></inline-formula> is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x98.png" xlink:type="simple"/></inline-formula> if</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x99.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x100.png" xlink:type="simple"/></inline-formula> if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x101.png" xlink:type="simple"/></inline-formula>. With multiple symmetric equilibria a symmetric equilibrium</p><p>with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x102.png" xlink:type="simple"/></inline-formula> index exists, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x103.png" xlink:type="simple"/></inline-formula>. By lemma 1<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x104.png" xlink:type="simple"/></inline-formula>, hence</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x105.png" xlink:type="simple"/></inline-formula>, which implies existence of at least one eigenvalue with negative real part. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x106.png" xlink:type="simple"/></inline-formula></p><p>It follows from (iii) that if each <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x107.png" xlink:type="simple"/></inline-formula> verifies symmetric stability then exactly one symmetric equilibrium exists.<sup>6</sup> In the one-dimensional case an even stronger relation between symmetric stability and the number of symmetric equilibria applies:<sup>7</sup></p><p>Corollary 1 Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x108.png" xlink:type="simple"/></inline-formula> in a regular game. There exists an odd number of symmetrically stable equilibria. Moreover, a symmetric equilibrium is globally symmetrically stable if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x109.png" xlink:type="simple"/></inline-formula> is the only symmetric equilibrium.</p><p>Proof: Given regularity, a zero of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x110.png" xlink:type="simple"/></inline-formula> is symmetrically stable if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x111.png" xlink:type="simple"/></inline-formula>. Hence symmetrically sta-</p><p>ble equilibria have index <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x112.png" xlink:type="simple"/></inline-formula> and the first claim follows from the Index theorem. Necessity in the second claim is trivial. For sufficiency, note that uniqueness of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x113.png" xlink:type="simple"/></inline-formula> implies <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x114.png" xlink:type="simple"/></inline-formula> (the corresponding index is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x115.png" xlink:type="simple"/></inline-formula>). From (3) deduce that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x116.png" xlink:type="simple"/></inline-formula>. Hence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x117.png" xlink:type="simple"/></inline-formula> crosses the 45˚-line from above. Thus <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x118.png" xlink:type="simple"/></inline-formula> whenever</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x119.png" xlink:type="simple"/></inline-formula>. Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x120.png" xlink:type="simple"/></inline-formula>. Because <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x121.png" xlink:type="simple"/></inline-formula> it follows from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x122.png" xlink:type="simple"/></inline-formula> and strong quasicon-cavity that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x123.png" xlink:type="simple"/></inline-formula>. Hence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x124.png" xlink:type="simple"/></inline-formula> whenever <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x125.png" xlink:type="simple"/></inline-formula> (<xref ref-type="fig" rid="fig2">Figure 2</xref>). Similarly, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x126.png" xlink:type="simple"/></inline-formula>whenever<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x127.png" xlink:type="simple"/></inline-formula>. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x128.png" xlink:type="simple"/></inline-formula></p><p>It may be noted from the above proof (or <xref ref-type="fig" rid="fig2">Figure 2</xref>) that the second claim of corollary 1 remains valid if there is a single symmetric equilibrium which belongs to the boundary (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x129.png" xlink:type="simple"/></inline-formula>).</p><p>Best-reply dynamics. Another standard dynamics in the literature are dynamics defined directly over the best-reply functions.<sup>8</sup> These dynamics are of the form</p><disp-formula id="scirp.67228-formula13"><graphic  xlink:href="http://html.scirp.org/file/16-1500875x130.png"  xlink:type="simple"/></disp-formula><p>and the symmetric restriction analogously to (2) yields</p><disp-formula id="scirp.67228-formula14"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-1500875x131.png"  xlink:type="simple"/></disp-formula><p>A symmetric equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x132.png" xlink:type="simple"/></inline-formula> is symmetrically stable with respect to (4) if the Jacobian, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x133.png" xlink:type="simple"/></inline-formula></p><p>has only eigenvalues with negative real parts. It follows that corollary 1 and theorem 1 (i) and (iii) apply, without modification, to the dynamics (4). The latter follows from (3) and the proof of theorem 1, and the former can be deduced directly from (4) together with <xref ref-type="fig" rid="fig2">Figure 2</xref>.<sup>9</sup></p><p>Relation to comparative statics. Typically, the IFT is the main formal tool to (locally) sign the comparative- static effects.<sup>10</sup> Stability conditions allow to robustly sign comparative-static effects [<xref ref-type="bibr" rid="scirp.67228-ref3">3</xref>] and additionally assure local convergence after a small shock, which many deem a natural requirement of a comparative-static predict- tion. A symmetrically unstable equilibrium is not re-established after a symmetric shock. Moreover, symmetri-</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Corollary 1</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/16-1500875x135.png"/></fig><p>cally unstable equilibria may “pervert” the comparative-statics. To illustrate consider a regular game with three symmetric equilibria <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x136.png" xlink:type="simple"/></inline-formula> (see <xref ref-type="fig" rid="fig3">Figure 3</xref>) where c is an exogenous common parameter. A and B are symmetrically stable (index<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x137.png" xlink:type="simple"/></inline-formula>), but C is symmetrically unstable (index<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x138.png" xlink:type="simple"/></inline-formula>). Consider a symmetric parameter shift <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x139.png" xlink:type="simple"/></inline-formula> and assume that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x140.png" xlink:type="simple"/></inline-formula>. As is suggested by the figure (formally</p><p>apply the IFT) points A and B both increase to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x141.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x142.png" xlink:type="simple"/></inline-formula>. As both <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x143.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x144.png" xlink:type="simple"/></inline-formula> are symmetrically stable, the symmetric dynamics (2) converge from A to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x145.png" xlink:type="simple"/></inline-formula> or from B to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x146.png" xlink:type="simple"/></inline-formula>, consistent with the suggested shift of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x147.png" xlink:type="simple"/></inline-formula>. For the symmetrically unstable point C we see that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x148.png" xlink:type="simple"/></inline-formula> (a consequence of the negative index), contradict-</p><p>ing the direction suggested by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x149.png" xlink:type="simple"/></inline-formula>. As C lies in the basin of attraction of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x150.png" xlink:type="simple"/></inline-formula> the dynamics do</p><p>not move down to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x151.png" xlink:type="simple"/></inline-formula> but monotonically up to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x152.png" xlink:type="simple"/></inline-formula> (which is also inconsistent with “small” changes). Hence the comparative-statics suggested by the IFT and the dynamics disagree at the unstable equilibria, and the IFT- prediction <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x153.png" xlink:type="simple"/></inline-formula> could never be supported as a stable equilibrium.</p></sec><sec id="s2_2"><title>2.2. Application: Two-Dimensional Contest with Endogenous Price</title><p>To illustrate symmetric stability in an example consider a payoff of the form</p><disp-formula id="scirp.67228-formula15"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-1500875x154.png"  xlink:type="simple"/></disp-formula><p>The interpretation is that N contestants choose their strategies, the pairs<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x155.png" xlink:type="simple"/></inline-formula>, to obtain a prize worth<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x156.png" xlink:type="simple"/></inline-formula>, where the value of a prize is endogenously determined. A specific context is provided by [<xref ref-type="bibr" rid="scirp.67228-ref10">10</xref>] , where firms com-</p><p>pete in salience and prices for attention-constrained consumers.<sup>11</sup> Assume that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x157.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x158.png" xlink:type="simple"/></inline-formula> (everybody has a chance to seize a prize) for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x159.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x160.png" xlink:type="simple"/></inline-formula> (a prize is worthwhile seizing) for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x161.png" xlink:type="simple"/></inline-formula>. An interior symmetric equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x162.png" xlink:type="simple"/></inline-formula> solves</p><disp-formula id="scirp.67228-formula16"><graphic  xlink:href="http://html.scirp.org/file/16-1500875x163.png"  xlink:type="simple"/></disp-formula><p>with associated Jacobian</p><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Symmetric stability and comparative statics.</title></caption><fig id ="fig3_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/16-1500875x165.png"/></fig></fig-group><disp-formula id="scirp.67228-formula17"><graphic  xlink:href="http://html.scirp.org/file/16-1500875x166.png"  xlink:type="simple"/></disp-formula><p>It easily follows from theorem 1 (ii) that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x167.png" xlink:type="simple"/></inline-formula> is symmetrically stable if both<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x168.png" xlink:type="simple"/></inline-formula>. By contrast, with dynamics (1) we would need to evaluate the eigenvalues of a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x169.png" xlink:type="simple"/></inline-formula> matrix. The symmetric stability condition states that second-order direct effects of each own strategy <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x170.png" xlink:type="simple"/></inline-formula> (which must be negative by strong</p><p>quasiconcavity) are not reversed by the second-order effects of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x171.png" xlink:type="simple"/></inline-formula>, a property which is typically satisfied in standard functional examples (see [<xref ref-type="bibr" rid="scirp.67228-ref7">7</xref>] ). Moreover, it follows from theorem 1 (iii) that if any <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-1500875x172.png" xlink:type="simple"/></inline-formula> verifies this condition and the game is symmetrically regular, a single symmetric and symmetrically stable equilibrium exists.</p></sec></sec><sec id="s3"><title>Acknowledgements</title><p>I thank Diethard Klatte and participants at seminars at University of Zurich, Harvard University and at the UECE Lisbon Game Theory meeting for valuable comments, and Ines Brunner for ongoing support.</p></sec><sec id="s4"><title>Cite this paper</title><p>Andreas Hefti, (2016) Symmetric Stability in Symmetric Games. Theoretical Economics Letters,06,488-493. doi: 10.4236/tel.2016.63056</p></sec><sec id="s5"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.67228-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Avriel, M., Diewert, W.E. and Zang, I. (1981) Nine Kinds of Quasiconcavity and Concavity. Journal of Economic Theory, 25, 397-420. http://dx.doi.org/10.1016/0022-0531(81)90039-9</mixed-citation></ref><ref id="scirp.67228-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Hefti, A. (2014) Equilibria in Symmetric Games: Theory and Applications. ECON Working Paper.</mixed-citation></ref><ref id="scirp.67228-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Dixit, A. (1986) Comparative Statics for Oligopoly. International Economic Review, 27, 107-122.  
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