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Leverage, investment, and optimal monetary policy

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Published/Copyright: June 21, 2014

Abstract:

We study optimal monetary policy in an economy where firms’ debt overhangs lead to under-investment and under-production. The magnitude of this debt-induced distortion varies over the business cycle, rising significantly during recessions. When debt is contracted in nominal terms, this distortion gives rise to a balance sheet channel for monetary policy. In the presence of real and financial shocks, the monetary authority faces a trade-off between inflation and output gap stabilization. The optimal monetary policy rule prescribes that the anticipated component of inflation should be set equal to a target level, while the unanticipated component should rise in response to adverse shocks, smoothing the debt overhang distortion and the output gap.

JEL Classification:: E32; E52

Corresponding author: Filippo Occhino, Research Department, Federal Reserve Bank of Cleveland, 1455 East 6th Street, Cleveland, OH 44114, USA, e-mail:
aThe views expressed herein are those of the authors and do not necessarily reflect those of the Federal Reserve Bank of Cleveland or of the Board of Governors of the Federal Reserve System.bThe views expressed herein are those of the authors and should not be attributed to the IMF, its Executive Board, or its management.

Acknowledgments

We would like to thank the Editor, an anonymous reviewer, and seminar participants at the 2012 Central Bank Macroeconomic Modeling Workshop in Warsaw, the 2011 Joint Central Bank Conference in Zurich, and Texas A&M University.

Appendices

A Derivation of equations (5) and (6)

This appendix derives equations (5) and (6) from the system of equations (1) through (4), which describes the equilibrium of the model.

Using the definition yωθAkα, and the expressions for k and b from equations (1) and (3), equation (2) becomes:

ν=ln(E{ω}θAkα)ln(b)σ+12σν=1σ{ln(E{ω}θA)+αln(E{ω}θAαΦ(ν))1αln(b¯e(πE0π))}+12σν=1σ{ln(E{ω}θA)1α+αln(αΦ(ν))1αln(b¯)+(πE0π)}+12σ

which is equation (5).

Taking a first-order Taylor expansion of equation (5) with respect to ν, ln(θ), (πE0π) and σ, we obtain:

ν^=1σ¯{11αθ˜+α1αΦ(ν¯)Φ(ν¯)ν^+(πE0π)(ν¯σ¯)σ˜}ν^=11χ¯1σ¯{11αθ˜+(πE0π)(ν¯σ¯)σ^}

where χ¯1σ¯α1αΦ(ν¯)Φ(ν¯)(0,1); bars over variables denote steady state values derived in the absence of aggregate shocks; while hats and tildes over variables denote, respectively, deviations and log-deviations from steady state values.[11]

Finally, taking a first-order Taylor expansion of equation (4), and using the previous result, we obtain:

x^=α1αΦ(ν¯)Φ(ν¯)ν^x^=α1αΦ(ν¯)Φ(ν¯)11χ¯1σ¯{11αθ˜+(πE0π)(ν¯σ¯)σ^}x^=χ¯1χ¯{11αθ˜+(πE0π)(ν¯σ¯)σ^}

which is equation (6).

B Solution of the optimal policy problem (9)

This appendix solves the optimal monetary policy problem (9).

Notice that monetary policy rules that differ by a scale factor (P′≡κP, or equivalently π′≡ln(κ)+π) induce the same real allocation. If you double up the price level, the face value of debt doubles and there is no change in the real allocation. However, the second term in the objective function, equal to E0(ππ¯)2=E0(πE0π)2+(E0ππ¯)2, is minimized by the rule such that E0π=π¯. Then, without loss of generality, we can restrict attention to rules where the expected value of inflation is the target inflation rate, adding the constraint

(11)E0π=π¯ (11)

to the optimal problem (9). Other rules have the same output gap but a larger inflation gap, so they are not optimal.

The optimal problem (9), then, becomes:

minπ(s)(8)subjectto:(11),(4),and(5).

After substituting the expression E0π=π¯ in the constraint (5),

minπ(s)12E0{γx2+(1γ)(ππ¯)2}subjectto:E0π=π¯,x=α1αln(Φ(ν)),ν=1σ{ln(E{ω}θA)1α+αln(αΦ(ν))1αln(b¯)+(ππ¯)}+12σ.

Equivalently,

minπ(s)12E0{γx2+(1γ)(ππ¯)2}subjectto:E0π=π¯,where:xα1αln(Φ(ν)),ν1σ{ln(E{ω}θA)1α+αln(αΦ(ν))1αln(b¯)+(ππ¯)}+12σ.

After defining π^ππ¯,

minπ^(s)12E0{γx2+(1γ)π^2}subjectto:E0π^=0,where:xα1αln(Φ(ν)),ν1σ{ln(E{ω}θA)1α+αln(αΦ(ν))1αln(b¯)+π^}+12σ.

Letting q(s) be the probability of the aggregate state,

minπ^(s)12s{γx2+(1γ)π^2}q(s)subjectto:sπ^q(s)=0,where:xα1αln(Φ(ν)),ν1σ{ln(E{ω}θA)1α+αln(αΦ(ν))1αln(b¯)+π^}+12σ.

Letting λ be the Lagrange multiplier (constant across states), the Lagrangian is

=s{12γx2+12(1γ)π^2+λπ^}q(s)where:xα1αln(Φ(ν)),ν1σ{ln(E{ω}θA)1α+αln(αΦ(ν))1αln(b¯)+π^}+12σ.

Taking the first-order conditions with respect to π^(s), for all states s,

γxxπ^+(1γ)π^+λ=0where:xπ^=α1αΦ(ν)Φ(ν)νπ^,νπ^=1σ{α1αΦ(ν)Φ(ν)νπ^+1}.

Letting χ1σα1αΦ(ν)Φ(ν), we obtain

νπ^χνπ^+1σνπ^1σ11χ

and then

xπ^=α1αΦ(ν)Φ(ν)1σ11χxπ^=χ1χ

so the previous first-order conditions become:

γxχ1χ+(1γ)π^+λ=0.

To obtain an expression for λ, we take the expectation of both sides and use E0π^=0:

E0{γxχ1χ+(1γ)π^+λ}=0λ=γE0{xχ1χ}.

Substituting this expression for λ into the previous first-order conditions, and using π^ππ¯, we obtain

γ{xχ1χE0{xχ1χ}}+(1γ)(ππ¯)=0

where χ1σα1αΦ(ν)Φ(ν). This is solution (10).

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Published Online: 2014-6-21
Published in Print: 2014-1-1

©2014 by De Gruyter

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