• 検索結果がありません。

Steinsson 2003 JME Errata

N/A
N/A
Protected

Academic year: 2018

シェア "Steinsson 2003 JME Errata"

Copied!
8
0
0

読み込み中.... (全文を見る)

全文

(1)

Erratum to:

Optimal Monetary Policy in an Economy with Inflation

Persistence

J´on Steinsson Harvard University

This note discribes errors in my article, Steinsson (2003).

1 Optimal Price Setting by Forward-Looking Households

There are several typos in the published version of equation (17) and the equation before equation (17). The forward-looking households’ price setting problem should be as follows. The forward- looking households choose the price that solves:

maxp Et

X

T =t

αT −ttRt,T(1 − τT)¯πT −tpyT(p) − βT −tv(yT(p); ξT)}. (1)

The first order condition of this problem is

Et

X

T =t

(αβ)T −t

YT

¯ πT −tpft

PT

!θT

(1 − θT)

"

uC(YT; ξT)(1 − τT) ¯π

T −tpf t

PT

!

θT θT − 1vy

YT π¯

T −tpf t

PT

!θT

; ξT

= 0 (2)

I would like to thank Mesut Arslan, Matthias Paustian, Dario Pontiggia, Niels Rønholt and Carlo Rosa for pointing out these errors. Date of last revision: January 24, 2006. Contact information: Department of Economics, Harvard University, Littauer Center. E-mail: [email protected]; Homepage: http://www.fas.harvard.edu/˜ steinss.

1

(2)

2 Log-Linearization of the Supply Block

Equations (A.1) and (A.2.) contain some errors. These errors are actually unrelated to the typos in the published version of equation (17) discussed above. The correct versions of equations (A.1) and (A.2.) are

πt= 1 − α

α ((1 − ω)ˆp

f

t + ω ˆpbt), (3)

Et

X

T =t

(αβ)T −t



−1+ ψ−1)xT + ¯τ 1 − ¯ττˆT

1 θ¯− 1θˆT

−(1 + ψ−1θ)¯

 ˆ

pftαβ

1 − αβπT +1



= 0 (4)

This second log-linearization may seem somewhat puzzling. The key is that in the steady state with zero inflation and ¯τ = −(¯θ− 1)−1 all terms outside the square brackets in equation (2) drop out since uC( ¯Y; 0) = vy( ¯Y; 0). The inflation terms have also been rearranged in order to avoid having a double sum. These errors affect the rest of the derivation of the Phillips curve. Equation (A.5) becomes

ˆ

pft = αβEtft+1+ 1 − αβ 1 + ψ−1θ¯



−1+ ψ−1)xt+ τ¯ 1 − ¯ττˆt

1 θ¯− 1θˆt



+ αβEtπt+1. (5)

Equation (A.6) becomes



ω+ α 1 − α



πt= (1 − ω)ˆpft + ω

1 − απt−1+ δωxt−1. (6) And equation (A.8) becomes

ηt= − (1 − α)(1 − αβ)(1 − ω)

(ω(1 − α + αβ) + α)(1 + ψ−1θ)¯¯θτˆt

(1 − α)(1 − αβ)(1 − ω)

(ω(1 − α + αβ) + α)(1 + ψ−1θ)(¯¯ θ− 1)θˆt (7)

3 Optimal Policy

There are also typos in equations (29) and (31). These equations should be as follows:

E0

(

X

t=0

βt{Lt+ 2φtfβπt+1− πt+ χbπt−1+ κ1xt+ κ2xt−1+ ηt)} )

. (8)

1+ βλ3)xt+ βλ4

2 Etπt+1 βλ4

2 πt+ κ1φt+ βκ2Etφt+1= 0. (9)

2

(3)

4 Sign of λ

4

There is a sign errror in the reported value of λ4. The correct expression for λ4 is

λ4= −2(1 − α)ωδ α(1 − ω) .

5 How Do These Errors Affect the Results of the Paper?

New versions of figures 1-9 in the paper are presented below. Most of the main features of the results are unchanged. However, there are some differences. One difference is the behavior from the first to the second period. In the published version of the paper the maximal impact of the shock occurs in the period after the shock first hits the economy. In the new version, the maximal impact is in the initial period. This difference is simply due to the error in equation (A.8) in the paper.

A second difference is that for the theoretical loss function the impulse response of inflation and output decay much more quickly in the new version of the figures than in the published version. This is interesting since it contrasts with the very slow decay that the traditional loss function yields. A third difference is that the price level response for ω = 0.7 is quite a bit smaller than in the published results.

References

Steinsson, J. (2003): “Optimal Monetary Policy in an Economy with Inflation Persistence,” Journal of Monetary Economics, 50, 1425–1456.

3

(4)

0 2 4 6 8 10 12 14 16 18 20

-5

0

5

10

15

20 x 10

-4 Figure 1: Inflation when ω = 0.01

Inflation, Commit, theoretical L.F.

Inflation, Commit, traditional L.F.

Inflation, Discr, theoretical L.F.

Inflation, Discr, traditional L.F.

0 2 4 6 8 10 12 14 16 18 20

-0.01

-0.008

-0.006

-0.004

-0.002

0

Figure 2: Output when ω = 0.01

Output, Commit, theoretical L.F.

Output, Commit, traditional L.F.

Output, Discr, theoretical L.F.

Output, Discr, traditional L.F.

(5)

0 2 4 6 8 10 12 14 16 18 20

-5

0

5

10

15 x 10

-4 Figure 3: Inflation when ω = 0.2

0 2 4 6 8 10 12 14 16 18 20

-0.01

-0.008

-0.006

-0.004

-0.002

0

Figure 4: Output when ω = 0.2

Inflation, Commit, theoretical L.F.

Inflation, Commit, traditional L.F.

Inflation, Discr, theoretical L.F.

Inflation, Discr, traditional L.F.

Output, Commit, theoretical L.F.

Output, Commit, traditional L.F.

Output, Discr, theoretical L.F.

Output, Discr, traditional L.F.

(6)

0 2 4 6 8 10 12 14 16 18 20

-2

0

2

4

6 x 10

-4 Figure 5: Inflation when ω = 0.7

0 2 4 6 8 10 12 14 16 18 20

-6

-5

-4

-3

-2

-1

0

1 x 10

-3 Figure 6: Output when ω = 0.7

Inflation, Commit, theoretical L.F.

Inflation, Commit, traditional L.F.

Inflation, Discr, theoretical L.F.

Inflation, Discr, traditional L.F.

Output, Commit, theoretical L.F.

Output, Commit, traditional L.F.

Output, Discr, theoretical L.F.

Output, Discr, traditional L.F.

(7)

0 2 4 6 8 10 12 14 16 18 20

0

0.2

0.4

0.6

0.8

1

1.2

1.4 x 10

-5 Figure 7: Inflation when ω = 0.99

0 2 4 6 8 10 12 14 16 18 20

-3

-2.5

-2

-1.5

-1

-0.5

0 x 10

-4 Figure 8: Output when ω = 0.99

Inflation, Commit, theoretical L.F.

Inflation, Commit, traditional L.F.

Inflation, Discr, theoretical L.F.

Inflation, Discr, traditional L.F.

Output, Commit, theoretical L.F.

Output, Commit, traditional L.F.

Output, Discr, theoretical L.F.

Output, Discr, traditional L.F.

(8)

0 2 4 6 8 10 12 14 16 18 20

0

0.2

0.4

0.6

0.8

1

1.2

1.4 x 10

-3 Figure 9: Price level for different ω

w = 0.01

w = 0.2

w = 0.7

Figure 1: Inflation when  ω  = 0.01
Figure 3: Inflation when  ω  = 0.2
Figure 5: Inflation when  ω  = 0.7
Figure 7: Inflation when  ω  = 0.99
+2

参照

関連したドキュメント

Finally, we give an example to show how the generalized zeta function can be applied to graphs to distinguish non-isomorphic graphs with the same Ihara-Selberg zeta

It is suggested by our method that most of the quadratic algebras for all St¨ ackel equivalence classes of 3D second order quantum superintegrable systems on conformally flat

(4) The basin of attraction for each exponential attractor is the entire phase space, and in demonstrating this result we see that the semigroup of solution operators also admits

Kilbas; Conditions of the existence of a classical solution of a Cauchy type problem for the diffusion equation with the Riemann-Liouville partial derivative, Differential Equations,

In this work we give definitions of the notions of superior limit and inferior limit of a real distribution of n variables at a point of its domain and study some properties of

Then it follows immediately from a suitable version of “Hensel’s Lemma” [cf., e.g., the argument of [4], Lemma 2.1] that S may be obtained, as the notation suggests, as the m A

Definition An embeddable tiled surface is a tiled surface which is actually achieved as the graph of singular leaves of some embedded orientable surface with closed braid

Applying the representation theory of the supergroupGL(m | n) and the supergroup analogue of Schur-Weyl Duality it becomes straightforward to calculate the combinatorial effect