The Peril of the Inflation Exit Condition

Transcription

1 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 1 / 24 The Peril of the Inflation Exit Condition Fumio Hayashi (GRIPS) JEA Presidential Address, 9 September 2018

2 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 2 / 24 Policy Rates and Reserves, Japan, Jan May 2018 net policy rate = policy rate - IOR.

3 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 3 / 24 Takeaways Two monetary policy regimes: P (where the net rate > 0 and excess reserves 0), Z (where the net rate 0). Three Z spells Spell 1: March 1999-July 2000 (17 months), exit in August 2000, Spell 2: March 2001-June 2006 (64 months), exit in July 2006, Spell 3: Dec onward. Not all Z spells are alike. Spell 1 and 2: IOR = 0 in both. Excess reserves 0 in Spell 1. Spell 2 and 3: excess reserve dynamics different.

4 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 4 / 24 Two Findings about Spell 2 (March June 2006) (the QE effect) Measures of excess reserves have positive effects on output and inflation (Honda et. al. (2007), Honda (2014), and others). (Policy-induced exits can be expansionary) Exiting from Spell 2 one month earlier, in June 2006, would have been expansionary (a regime-switching SVAR evidence in Hayashi and Koeda ( Exiting from QE, 2018)). references IR

5 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 5 / 24 Plan for the Rest of My Talk Executive summary of the regime-switching SVAR (4 slides). Evidence for expansionary exits (1 slide). Three examples of expansionary exits: 1) active monetary policy (6 slides), 2) active monetary policy with one-period information lag (1 slide), 3) passive monetary policy with predetermined inflation (3 slides).

6 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 6 / 24 Only One Type of Z Assume (a) Spell 1 was a historical aberration. (b) Otherwise all Z s are like Spell 2 (so no anticipation of QQE). (c) No IOR. No need to distinguish between the policy rate and the net policy rate. Taken together, if s t denotes the monetary policy regime, { rt > 0 and m t = 0 if s t = P, ( where r policy rate, m log r t = 0 and m t > 0 if s t = Z, actual reserves required reserves ).

7 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 7 / 24 Dynamics under P and Z Additional notation: p monthly inflation rate, x output gap. The SVAR is about (s t, p t, x t, r t, m t). Switches between (P, p t, x t, r t, 0) and (Z, p t, x t, 0, m t). (super-standard) Dynamics under s t = P is block-recursive: p = const., lagged p, lagged x, lagged r x = const., lagged p, lagged x, lagged r r = const., π, x + v r, }{{} Taylor Rate + error, + error, where π t 1 (pt + + pt 11) is the year-on-year inflation rate. 12 Dynamics under Z: Just replace r by m and v r by v s. The reduced-form coefficients in the p and x equations can differ across regimes.

8 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 8 / 24 What Triggers Regime Changes? The usual formulation: (ZLB) s t = { P if Taylor rate > 0, Z otherwise. Inappropriate for Japan thanks to BOJ s inflation commitment. (April 1999) (The Bank of Japan will) continue to supply ample funds until the deflationary concern is dispelled. (then BOJ governor Hayami) (October 2003) The Bank of Japan is currently committed to maintaining the quantitative easing policy until the CPI (excluding fresh food, on a nationwide basis) registers stably a zero percent or an increase year on year. (BOJ release) (December 2016) The Bank will continue with Quantitative and Qualitative Monetary Easing (QQE) with Yield Curve Control, aiming to achieve the price stability target of 2 percent, as long as it is necessary for maintaining that target in a stable manner. It will continue expanding the monetary base until the year-on-year rate of increase in the observed CPI (all items less fresh food) exceeds 2 percent and stays above the target in a stable manner.

9 Regime Evolution with the Exit Condition The inflation exit condition means s t evolves recursively. Replace the ZLB by { P if Taylor rate > 0, If s t 1 = P, s t = Z otherwise. P if Taylor rate > 0 and π t v t, }{{} If s t 1 = Z, s t = threshold inflation Z otherwise. The central bank: observes (p t, x t) and hence π t. draws three shocks (v rt, v st, v t). computes the Taylor rate and m t. picks s t by (1). Then (1) (r t, m t) = { (Taylor rate, 0) if st = P, (0, value given by m t equation) if s t = Z. toy model absorbing state Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 9 / 24

10 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 10 / 24 The Effect of Exiting from QE in June Monthly Inflation (p) 1.5 Output Gap (x) 1 1 % annual rate 0.5 % months months Note: From Figure 4c of Hayashi and Koeda (2018). The 68% probability bands in shades. two findings IR defined

11 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 11 / 24 Plan for the Rest of My Talk Executive summary of the Hayashi-Koeda regime-switching SVAR (4 slides). Evidence for expansionary exits (1 slide). Theoretical examples of expansionary exits: 1) active monetary policy (6 slides), 2) active monetary policy with one-period information lag (1 slide), 3) passive monetary policy with predetermined inflation (3 slides).

12 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 12 / 24 A Toy Model: Fisher and Taylor Consists of Fisher and Taylor. (Fisher) r t = ρ + E t(π t+1), (2) ρ + π + ϕ(π t π ) }{{} if s t = P, (Taylor) r t = Taylor rate (3) 0 if s t = Z, The evolution of s t is (1) with Taylor rate = ρ + π + ϕ(π t π ). The target inflation rate π vs. the threshold inflation rate v t. The endogenous variables are (s t, π t, r t). Threshold inflation v t is the only shock. regime evolution

13 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 13 / 24 Example 1: ϕ > 1 and (π, r) Simultaneously Determined The threshold inflation v t is a two-state Markov chain. v > π. v t 1 v t v (state 0) π (state 1) v (state 0) q 1 q π (state 1) 0 1 Look for Markov equilibria: { (s (0), π (0), r (0) ) (s t, π t, r t) = in state 0, i.e., if v t = v (> π ), (s (1), π (1), r (1) ) in state 1, i.e., if v t = π. An exit time path for a sample path of {v t}: t v t v (> π ) v (> π ) π π... s t Z Z Z P P... π t... (ρ+π ) q +π (< 0) (ρ+π ) q +π (< 0) π π... r t ρ + π ρ + π...

14 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 14 / 24 In the Absorbing State In state 1 (v t = π ), the Fisher equation becomes: (Fisher) r (1) = ρ + π (1). (4) Suppose s t 1 = P. t 4 in the above table. The Taylor rule becomes ρ + π + ϕ(π (1) π ) if Taylor rate > 0, }{{} (Taylor) r (1) = Taylor rate 0 otherwise. (5) regime evolution

15 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 15 / 24 The Peril of the Taylor Rule Two equilibria under active monetary policy (ϕ > 1) (Benhabib et. al. (2001)). Pick point A: (π (1), r (1) ) = (π, ρ + π ). The targted-inflation equilibrium. Given s t 1 = P, s t = P.

16 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 16 / 24 Check the Transition The Taylor rule becomes ρ + π + ϕ(π (1) π ) if Taylor rate > 0 and π (1) > π, }{{} (Taylor) r (1) = Taylor rate 0 otherwise. (6)

17 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 17 / 24 The Exit Condition Eliminates the Good Equilibrium State 0 (v t = v > π ). Suppose s t 1 = Z. (Fisher) r (0) = ρ + qπ (0) + (1 q)π. (7) (Taylor) ρ + π + ϕ(π (0) π ) if Taylor rate > 0 and π (0) v, r (0) }{{} = Taylor rate 0 otherwise. (8)

18 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 18 / 24 Example 2: ϕ > 1 and π is predetermined One-period information lag and predetermined inflation. t v t... v (> π ) v (> π ) π π... s t Z Z Z Z P... π t... (ρ+π ) q + π (ρ+π ) q + π (ρ+π ) q + π π... r t ρ + π... E t(π t+1 )... (ρ+π ) q + π (ρ+π ) q + π π π...

19 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 19 / 24 Example 3: 0 < ϕ < 1 and Predetermined Inflation Suggested by Stephanie Schmitt-Grohe. π is predetermined. (Fisher) r t = ρ + π t+1. The Taylor rule is the same as in Example 1. Taylor & Fisher provides a mapping from (s t 1, π t) to (s t, π t+1). Taylor: (s t 1, π t) (s t, r t), Fisher: r t π t+1. {v t} doesn t have to be a Markov chain with absorbing states. The exit path for a sample path of {v t}: t v t... π π v 3 ( ρ) v 4 v 5... s t Z Z Z P P P...

20 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 20 / 24 Without the Exit Condition... Only one steady state. It is the targeted-inflation equilibrium. It is stable.

21 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 21 / 24 The Exit Condition Introduces the Bad Equilibrium Taylor rate is positive. Nevertheless regime Z is chosen.

22 What Happens if Suspend the Exit Condition? Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 22 / 24

23 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 23 / 24 References Benhabib, Jess, Stephanie Schmitt-Grohe, and Martin Uribe (2001) The Perils of Taylor Rules, JET. Eggertsson, Gauti, and Michael Woodford (2003), The Zero Lower Bound on Interest Rates and Optimal Monetary Policy, BPEA. Hagedorn, Marcus (2017), A Demand Theory of the Price Level, mimeo., University of Oslo. Hayashi, F. and J. Koeda (2018), Exiting from QE, conditionally accept, QE. Honda, Yuzo, Yoshihiro Kuroki, and Minoru Tachibana (2007) An Injection of Base Money at Zero Interest Rates: Empirical Evidence from the Japanese Experience Osaka University, Discussion Papers in Economics and Bus iness Honda, Yuzo (2014), The Effectiveness of Nontraditional Monetary Policy: The Case of Japan. JER. Schmitt-Grohe, Stephanie, and M. Uribe (2014), Liquidity Traps: An Interest-Rate-Based Exit Strategy, Manchester School. two findings

24 Fumio Hayashi (GRIPS) The Peril of the Inflation Exit Condition 24 / 24 Appendix: (Nonlinear) IR Defined The IR to an exit in t: E ( y t+k s t = P, (p t, x t, 0, 0) }{{} (p, x, r, m) for date t,... } {{ } alternative history ) E ( yt+k s t = Z, (p t, x t, 0, m t) }{{} (p, x, r, m) for date t } {{ } baseline history ),..., (9) This can be decomposed into two: (9) = [E ( y t+k s t = P, (p t, x t, 0, 0),... ) E ( y t+k s t = Z, (p t, x t, 0, 0),... ) ] }{{} transitional effect of an exit from Z to P [E ( y t+k s t = Z, (p t, x t, 0, m t),... ) E ( y t+k s t = Z, (p t, x t, 0, 0),... ) ]. }{{} the QE effect (10) back to IR graph