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Inverse Limits and Models with Backward Dynamics (PDF) Working Paper Series* Department of Economics Alfred Lerner College of Business & Economics University of Delaware Working Paper No. 2006-12 Inverse Limits and Models with Backward Dynamics… Judy Kennedy David R. Stockman James A. Yorke 2006 ____________________________ *http://lerner.udel.edu/economics/workingpaper.htm …© 2006 by author(s). All rights reserved. Inverse Limits and Models with Backward Dynamics∗ Judy Kennedy,† David R. Stockman‡and James A. Yorke§ First Draft: March 2006 This Draft: November 2006 Abstract Some economic models like the cash-in-advance model of money have the property that the dynamical system characterizing equilibria is multi-valued going forward in time, but single-valued going backward in time, i.e., the model has backward dynamics. In this paper, we apply the theory of inverse limits to characterize topologically the set of equilibria in a dynamic economic model with this property. We show that such techniques are particularly well-suited for analyzing the dynamics going forward in time even though the dynamics are multi-valued in this direction. In particular, we analyze the inverse limit of the cash-in-advance model of money and illustrate how information about the inverse limit is useful for detecting or ruling out complicated dynamics. Keywords: backward dynamics, chaos, inverse limits, continuum theory, cash-in-advance. JEL: C6, E3, and E4. ∗We would like to thank two anonymous referees for helpful comments and suggestions. Stockman would like to thank the Lerner College of Business and Economics for its generous summer research support. †Department of Mathematical Sciences, University of Delaware, Newark, DE 19716. ‡Department of Economics, University of Delaware, Newark, DE 19716. §Institute for Physical Science and Technology, University of Maryland, College Park, MD 20742. 1 1 Introduction An equilibrium of a dynamic economic model can often be characterized as a solution to a dynamical system. Many nonlinear dynamical systems are single-valued moving forward, but multi-valued going backward. However, in economics we sometimes have just the opposite, namely dynamics that are multi-valued going forward, but are single-valued going backward. In such instances, we say the model (or dynamical system) has backward dynamics. Two economic models that may have backward dynamics include the overlapping generations (OLG) model and the cash-in-advance (CIA) model.1 Typically, the problem of backward dynamics is either ignored by using a local analysis or avoided by analyzing the model with the single-valued backward map as in Grandmont (1985) and Michener and Ravikumar (1998).2 However, using a local analysis ignores some potentially interesting equilibria. And as Medio (1992, pp. 222–23) notes, the backward map solution is unsatisfactory because the backward map gives orbits that go backward into the infinite past, whereas economists are interested in orbits that lead off into the infinite future. In this paper we apply the theory of inverse limits to characterize topologically equilibria in an economic model with backward dynamics and use the inverse limit space to establish or rule out complicated dynamics. Heuristically, the inverse limit of a dynamical system is a subset of an infinite dimensional space (e.g. the Hilbert cube) where each point in the inverse limit corresponds to a backward solution (backward orbit) of the dynamical system. Using the backward map from say the CIA model as our dynamical system, a point in the inverse limit, being a backward orbit of the backward map, corresponds to a forward orbit in the model. Since equilibria in the model correspond to backward orbits of the backward map, we see that the set of equilibria in the model is an inverse limit space. So we see that inverse limits are the right framework for analyzing models with backward dynamics. The question of how complicated is the set of equilibria in a model with backward dynamics is really a question of how complicated is the inverse limit space. There is a well-established literature in topology that addresses this question. For one-dimensional dynamical systems on an interval, the inverse limit has several important properties. First, the inverse limit is a continuum so the tools from topology that deal with continuum theory can be applied. Second, it is chainable and therefore can be topologically identified with an image in the plane. Inverse limits is a relatively new approach to analyzing models with backward dynamics. Medio and Raines (2006, 2005) use inverse limits to analyze the long-run behavior of an OLG model. Even though the the forward dynamics are multi-valued, they show that long-run behavior of equilibria in the model corresponds to an “attractor” of the shift map on the inverse limit space. Kennedy and Stockman (2006) use the inverse limit space to show that 1See Grandmont (1985) for the OLG model and Michener and Ravikumar (1998) for the CIA model. 2Grandmont (1985) also utilizes a “belief function” describing how agents form their beliefs about the future to the remedy problem of multi-valued forward dynamics. 2 a model with backward dynamics is chaotic going forward in time if and only if it is chaotic going backward in time. Our goal in this paper is to illustrate how inverse limit theory can be used to establish or rule out complicated/complex equilibria. When considering the inverse limit space of a model with backward dynamics, two ques- tions naturally arise: (1) what does the structure of the inverse limit tell us about the un- derlying dynamics, and (2) what does the underlying dynamics imply for the inverse limit? Ingram and Mahavier (2004) explore the connections between these two aspects of dynamical systems for maps on the unit interval. Working within a family of one-dimensional maps, they illustrate that restrictions on parameters that lead to simple/complicated dynamics also lead to simple/complicated inverse limits. Barge and Martin (1985) show that if f : X → X is a piecewise monotone map with X being an interval, if lim(I, f) is indecomposable then ←− f has a periodic point of power not equal to a power of 2.3 Barge and Diamond (1994) extend this result for piecewise monotone map f on a finite graph X. In this case, they also show that the dynamical system will exhibit positive topological entropy if and only if the inverse limit contains an indecomposable continuum. Consequently, by analyzing the inverse limit one can detect chaotic/complicated dynamics or rule out chaotic/complicated behav- ior based on properties of the inverse limit. This offers an alternative method of detecting chaotic behavior that does not work directly with establishing a 3-cycle (or some other cycle and using Sarkovskii’s ordering on the integers) and ruling out chaotic behavior as well. The paper is organized as follows. In section 2 we briefly cover the cash-in-advance model focusing on some of the properties of the implicitly-defined difference equation from that model. Next, we provide the necessary background material from dynamical systems and inverse limits in section 3. Section 4 discusses why inverse limits are the right framework for analyzing models with backward dynamics and a useful tool for analyzing single-valued dynamical systems as well. In section 5, we illustrate how inverse limits can be applied to the CIA model of money. We conclude in section 6. 2 The Model In this section, we briefly describe the cash-in-advance model with particular emphasis on the problem of backward dynamics. The model is the standard endowment CIA model of Lucas and Stokey (1987). We closely follow the exposition of Michener and Ravikumar (1998), hereafter [MR]. It is an endowment economy with both cash and credit goods. There is a representative agent and a government. The government consumes nothing and sets monetary policy using a money growth rule. The household has preferences over sequences of the cash good (c1t) and credit good (c2t) 3These objects are defined and discussed in section 3. For now, we note that chainable indecomposable continua are topologically equivalent to certain fractal objects in the plane. 3 represented by a utility function of the form X∞ t β U(c1t, c2t), (1) t=0 with the discount factor 0 < β < 1. ∞ The household seeks to maximize (1) by choice of {c1t, c2t, mt+1}t=0 subject to the con- straints c1t, c2t, mt+1 ≥ 0, ptc1t ≤ mt, (2) mt+1 ≤ pty + (mt − ptc1t) + θMt − ptc2t, (3) ∞ taking as given m0, y, θ and {pt,Mt}t=0. θMt represents a lump-sum transfer of cash from the government. The money supply {Mt} is controlled by the government and follows a constant growth path Mt+1 = (1 + θ)Mt where θ is the growth rate and M0 > 0 given. [MR] make assumptions on the function U so that the solution to this problem will be interior and the solution to the first-order conditions and transversality condition will be necessary and sufficient. 2 2 Assumption 1. ([MR], p. 1120) The function U : R+ → R is C with U1 > 0,U2 > 0 and the Hessian matrix negative definite. Both c1t and c2t are assumed to be normal goods. Further, to guarantee interior solutions we will assume lim U1(c, y − c) = lim U2(c, y − c) = ∞, c→0 c→y and that U1(y, 0) < ∞ and U2(0, y) < ∞. The first-order conditions from this problem imply that U2(c1t, c2t)/pt = βU1(c1t+1, c2t+1)/pt+1. (4) This condition reflects that at the optimum, the household must be indifferent between spending a little more on the credit good (giving a marginal benefit U2(c1t, c2t)/pt) versus savings the money and purchasing the cash good in the next period (giving a marginal benefit βU2(c1t+1, c2t+1)/pt+1).
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