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Interest rate rules and equilibrium (in)determinacy in a small open economy: the role of internationally traded capital

  • Wen-ya Chang , Hsueh-fang Tsai , Juin-jen Chang EMAIL logo and Hsieh-yu Lin
Published/Copyright: March 21, 2018

Abstract

This study develops a small-open-economy version of Benhabib, J., S. Schmitt-Grohé, and M. Uribe. 2001. “Monetary Policy and Multiple Equilibria.” American Economic Review 91: 167–186. We systematically explore the role of international capital mobility and the portfolio balance channel in terms of macroeconomic (in)stability when the government follows a commonly-adopted interest-rate feedback rule. In a one-traded-good model, the steady-state equilibrium, in general, is locally determinate; international capital mobility stabilizes the economy against business cycle fluctuations under a simple interest-rate feedback rule. In a two-good (traded and non-traded goods) model, the relationship between equilibrium (in)determinacy and the aggressiveness of interest rate rules is not monotonic, and crucially depends on households’ portfolio preferences. These results suggest that a unified interest rate rule can end up with very different consequences of macroeconomic (in)stability in an open economy from those in a closed economy.

JEL Classification: F41; E52; E31

Acknowledgements

We thank two anonymous referees as well as Been-Lon Chen, Jang-Ting Guo, Ching-Chong Lai, and Ping Wang for their helpful suggestions and insightful comments on an earlier version of this paper, whose inputs have led to a much improved paper. The usual disclaimer applies. Financial support from the National Science Council is gratefully acknowledged.

Appendix

Appendix A

The proof of Propositions 1 and 2

The exact derivatives of (13) are given by:

cλ=1Δ{λt(1ψ)(umm+v11ψ(πt)ucm)+λtψ[v11v12+ucm(Rtf+πtψ(πt))]},ca=1Δ(λtucm)(v11ψv12),cbf=1Δ(λtucm)(v12v11+ψv21ψv22λtψRf),mλ=1Δ{λt(1ψ)(uccψ(πt)ucm)λtψucc[Rtf+πtψ(πt)]},ma=1Δλtucc(v11ψv12),mbf=1Δλtucc(v12v11+ψv21ψv22λtψRf),πλ=1Δ{(v11v12)(uccψ(πt)ucm)+(Rtf+πtψ(πt))[ucc(umm+v11)ucm2]},πa=1Δ(v11v12)(uccummucm2),πbf=1Δ{(v21v22v11+v12λtRf)[ucc(umm+v11)ucm2]+ucc(v11v12)2},

where Δ=λt(1ψ)[ucc(umm+v11)ucm2]+λtψ(v11v12)ucc. Apparently, this dynamic system should be complicated. Thus, we impose Assumption 2 in order to make our model analytically tractable.

Under Assumption 1 and Assumption 2, we can obtain the following Jacobian matrix of this dynamic system from (14)–(16):

(50)[λ˙tb˙tfa˙t]=[λ^(1ψ)πλ+ρ+π^R^λ^(1ψ)πbf0cλcbf+R^f(1η)0ΦλΦbfΦa][λtλ^btfb^fata^],

where Φλ=cλ+πλ[(ψ1)(a^b^f)ψm^]R^mλ,Φbf=cbf+R^f(1η)+πbf[(ψ1)(a^b^f)ψm^]R^mbf+π^R^, and Φa=(R^π^).

Let μ1, μ2, and μ3 be the eigenvalues of the dynamic system. From (50), it is easy to obtain:

(51)μ1+μ2=v2λ^+R^f(1η)cbf,
(52)μ1μ2=v2λ^[R^f(1η)cbf]+cλλ^(1ψ)πbf=ξv22+λ^Rfuccummucm2(ummψ(π^)ucm)+,
(53)μ3=R^π^>0,

where ξv2λ^R^f(1η)v1λ^cbf. As noted in the context, the steady-state equilibrium is locally determinate when there are two roots with positive real parts and one root with a negative real part. The equilibrium is locally indeterminate when the dynamic system has more than two roots with negative real parts. It is a source when there are three roots with positive real parts.

By focusing on Proposition 1, we first assume that v1 = v2 = 0, which rules out the portfolio balance channel. Under such a situation, ξ = 0 is true and hence μ1μ2 < 0. Thus, there are two roots with positive real parts and one root with a negative real part in the dynamic system. The equilibrium is then characterized by local determinacy.

We now turn to the analysis in which households exhibit a portfolio preference between domestic and foreign bonds. To focus on more meaningful cases, we abstract the source (three roots with positive real parts) from the analysis. Accordingly, it is easy to infer that if μ1 + μ2 > 0, we can rule out the possibility of indeterminacy, given that μ3 > 0. In what follows, we will prove that if μ1 + μ2 < 0, equilibrium determinacy can also be true. It is clear from (51) that R^f(1η)<cbf must hold under the case with μ1 + μ2 < 0. There are two scenarios: v1 > v2 and v2 > v1. In the scenario where v1 > v2, the condition R^f(1η)<cbf guarantees that ξ < 0 is true. From (52), we can refer to μ1μ2 < 0, given that ξ < 0. Accordingly, we have μ1 + μ2 < 0 and μ1μ2 < 0, implying that there is one negative eigenvalue and two positive eigenvalues in the dynamic system. Therefore, the equilibrium is locally determinate. In the scenario where v2 > ν1, we have R^π^>R^f, since the condition ρ=v1λ^+ψ(π^)π^=v2λ^+R^f is true in the steady state. Thus, we can further infer that under the condition ρ2>R^π^ the following inequality holds:

v1λ^>R^π^>R^f>R^f(1η).

Since v2λ^+R^f(1η)<cbf is true in the case where μ1 + μ2 < 0, we can further obtain:

ξ=v2λ^R^f(1η)v1λ^cbf<v2λ^R^f(1η)v1λ^[v2λ^+R^f(1η)]<0,

implying that μ1μ2 < 0. Therefore, the dynamic system has two roots with positive real parts and one root with a negative real part. The equilibrium is also locally determinate in the scenario where v2 > v1.

Appendix B

The characterization of the two-good model with flexible prices

First, we define:

ct=h(cT,t,cH,t)=cT,tαcH,t1α,and h1=αctcT,t>0,h2=(1α)ctcH,t>0,h12=α(1α)ctcT,tcH,t>0,h11=α(1α)ctcT,t2<0, and h22=α(1α)ctcH,t2<0.

Thus, by substituting (23) into (20)–(22), we can obtain the instantaneous relationships of the traded good consumption, real money balances, and inflation as follows:

cT,t=cT(et),mt=m(λt,et),πt=π(λt,et),

where

cT,e=h22h11h2h21h1, mλ=1h2ucm, me=(ucch1h2+u2h21)cT,eh2ucm, πe=cT,eλtψh2ucm[h1h2(ucm2uccumm)ummuch21], and πλ=1λtπ(ummh2ucmψ).

Given that v(bt,etbtf)=bt+A(etbtf)1ε1ε, (25)–(27) can be rewritten as:

λ˙t=λt[ρ+π(λt,et)ψ(π(λt,et))]1,b˙tf=[R¯f+Rf(btf)]btfcT(et),e˙t=et{A(e^b^f)ε1λt+[R¯f+Rf(btf)]+π(λt,et)ψ(π(λt,et))},

which implies that the dynamic system can be reduced to a 3×3 one in terms of λt, btf, and et. Therefore, the Jacobian matrix of this dynamic system is given by:

[λ˙tb˙tfe˙t]=[λ^(1ψ)πλ0λ^(1ψ)πe0R^f(1η)cT,ee^[A(e^b^f)ε1λ^2(1ψ)πλ]e^[e^Aε(e^b^f)ε1λ^+Rf]e^[b^fAε(e^b^f)ε1λ^+(1ψ)πe]][λtλ^btfb^fete^]

Appendix C

The characterization of the two-good model with price stickiness

Given that v(bt,etbtf)=bt+A(etbtf)1ε1ε, we can use (33)–(35) and (40) to obtain:

cT,t=cT(λt,et,πt),cH,t=cH(λt,et,πt),mt=m(λt,et,πt), and mp,t=mp(λt,et,πt),where cT,λ=1(etummψ(πt)ucmh1)(h12eth22),cT,e=h2[h1h2(uccummucm2)+uceth22umm],cT,π=λtψucmh1(h12eth22),cH,λ=1(h11eth21)(ψ(πt)ucmh1etumm),cH,e=h2[h12(uccummucm2)+uceth21umm],cH,π=λtψ(h11eth21)ucmh1,mλ=1(ψ(πt)ucch1etucm)h2(2h1h2h12h22h11h12h22),me=1λtumch1(h12eth22),mπ=λtψuccet(2h1h2h12h22h11h12h22),mp,λ=cH,λyH,mp,e=cH,eyH,mp,π=cH,πyH,and=et(uccummucm2)(2h1h2h12h22h11h12h22).

By substituting (45) into (46)–(49), we thus have a 4×4 dynamic system in terms of λt, et, πt, and btf and, accordingly, the corresponding Jacobian matrix is given by:

[λ˙te˙tπ˙tb˙tf]=[1λ^0λ^(1ψ)0e^[1A(e^b^f)ελ^2)e^[εA(e^b^f)ε1]b^fλ^e^(1ψ)e^[εA(e^b^f)ε1λ^e^Rf]ΩλΩeρΩπ0cT,λcT,ecT,πR^f(1η)][λtλ^ete^πtπ^btfb^f]

where Ωλ=[d(1)y^H/ς][1/(λ^y^H)+(y^H/y^H2)mp,λ(1+λ^ψ(π^))],Ωe=[d(1)y^H/ς](y^H/y^H2)mp,e(1+λ^ψ(π^)), and Ωπ=[d(1)y^H/ς][λ^ψ/y^H+(y^H/y^H2)mp,π(1+λ^ψ(π^))].

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Published Online: 2018-03-21

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