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The effects of monetary policy regime shifts on the term structure of interest rates

  • Azamat Abdymomunov EMAIL logo and Kyu Ho Kang

Abstract

We investigate how the entire term structure of interest rates is influenced by changes in monetary policy regimes. To do so, we develop and estimate an arbitrage-free dynamic term-structure model which accounts for regime shifts in monetary policy and price of risk. Our results for US data from 1985 through 2008 indicate that (i) the Federal Reserve’s reaction to inflation has changed over time, switching between “active” and “passive” monetary policy regimes; (ii) on average, the term spread in the “active” regime was wider than in the “passive” regime; and (iii) the yields in the “active” regime were considerably more volatile than in the “passive” regime. The wider term spread in the “active” regime reflects higher term premia associated with a more sensitive response of the short-term interest rate to inflation. Additionally, our analysis suggests that the model fit improves substantially when we account for regime switching in monetary policy and price of risk.

JEL: G12; C11; E43

Corresponding author: Azamat Abdymomunov, Federal Reserve Bank of Richmond, 530 East Trade Street, Charlotte, NC 28202, USA, e-mail:

Acknowledgments

The views expressed in this paper are those of the authors and do not necessarily reflect the position of the Federal Reserve Bank of Richmond or the Federal Reserve System. We would like to thank the Editor, Bruce Mizrach, and the Referee for helpful feedback. We are especially grateful to James Morley for his valuable discussions and suggestions. We would also like to thank Steve Fazzari, William Gavin, Werner Ploberger, Guofu Zhou, and participants at the 2011 ASSA meetings for their helpful comments. All remaining errors are our own.

Appendices

Appendix A. Bond pricing

We solve for Aτj and Bτj using the law of iterated expectations, method of undetermined coefficients, and log-linearization:

Pt,τst=E[exp(rtst12Λtst+1Λtst+1Λtst+1εt+1)Pτ1,t+1st+1|ft,st]

1=E[exp(rtj12Λtst+1Λtst+1Λtst+1εt+1)Pτ1,t+1st+1Pτ,tj|ft,st=j]

=k=1SpjkE[exp(rtj12ΛtkΛtkΛtkεt+1)Pτ1,t+1kPτ,tj|ft,st=j,st+1=k]

=k=1SpjkE[exp(rtj12ΛtkΛtkΛtkεt+1+Aτj+BτjftAτ1kBτ1kft+1)|ft,st=j,st+1=k]

(17)=k=1Spjk{exp(rtj12Λtk'Λtk+AτjAτ1k+BτjftBτ1kμtj,k)×E[exp((Λtk'+Bτ1k'Lk)εt+1)|ft,st=j,st+1=k]} (17)
(18)=k=1Spjk{exp(rtj12Λtk'Λtk+AτjAτ1k+Bτj'ftBτ1k'μtj,k+12(Λtk+Bτ1kLk)(Λtk+Bτ1kLk))} (18)
(19)=k=1Spjkexp(rtj+AτjAτ1k+BτjftBτ1kμtj,k+Bτ1kLkΛtk+12Bτ1kLkLkBτ1k) (19)
(20)k=1Spjk{δ0jδfjft+AτjAτ1k+BτjftBτ1kdkBτ1kG(ftdj)+Bτ1k'Lk(λ0k+λfft)+12Bτ1kLkLkBτ1k+1}. (20)

(17) is transformed into (18) by using the property of moment generating function for normally distributed εt+1:

φtjk(x)E[exp(xεt+1)|ft,st=j,st+1=k]=exp(xx2),x3

evaluated at x=(Λtk+Bτ1k'Lk). Following Bansal and Zhou (2002), (19) is transformed into (20) using log-approximation exp(y)≈y+1 for a sufficiently small y and substituting for rtj using equation (9).

Using the above result for the bond pricing equation and collecting terms for ft:

0=k=1S{pjkE[exp(rtj12Λtk'ΛtkΛtk'εt+1)Pt+1,kτ1Pt,jτ|ft,st=j,st+1=k]}1k=1Spjk(δ0jδfj'ft+AτjAτ1k+Bτj'ftBτ1k'dkBτ1k'G(ftdj)+Bτ1k'Lk(λ0k+λfft)+12Bτ1k'LkLk'Bτ1k)=k=1Spjk(δ0j+AτjAτ1kBτ1k'dk+Bτ1k'Gdj+Bτ1k'Lkλ0k+12Bτ1k'LkLk'Bτ1k)+k=1Spjk(δfj'+Bτj'Bτ1k'G+Bτ1k'Lkλf)ft.

The above identity has to be true for every value of ft, which will be the case if only the first and second terms are 0:

0=k=1Spjk(δ0j+AτjAτ1kBτ1k'dk+Bτ1k'Gdj+Bτ1k'Lkλ0k+12Bτ1k'LkLk'Bτ1k)

and

0=k=1Spjk(δfj'+Bτj'Bτ1k'(GLkλf)).

This leads to the solution for Aτj and Bτj in the form of recursive system:

Aτj=δ0j+k=1Spjk(Aτ1k+(dkGdjLkλ0k)Bτ1k12Bτ1k'LkLk'Bτ1k)Bτj=δfj+k=1Spjk(GLkλf)Bτ1k.

To derive the initial conditions for A0j and B0j, we let τ=0. Given Pτ,tj=exp(τrtj), we have P0,tj=exp(0×rtj)=1. From Pj,tτ=exp(AτjBτj'ft) for τ=0: 1=P0,tj=exp(A0jB0j'ft) has to be true for every ft, therefore A0j=0 and B0j=0, consequently A1j=δ0j and B1j=δfj.

Appendix B. Expected excess return

The one-period expected excess return on the n-period bond is given by

ERτ,tj=E[p¯τ1,t+1|ft,st=j]+p¯1,tjp¯τ,tj,

where p¯τ,tj and p¯1,tj are log prices of bonds derived in the following ways:

p¯τ,tj=logPτ,tj=logE[exp(rtj12Λtk'ΛtkΛtk'εt+1)Pτ1,t+1|ft,st=j]=rtj+log(k=1SpjkE[exp(12Λtk'ΛtkΛtk'εt+1)Pt+1,τ1k|ft,st=j,st+1=k])=rtj+log(k=1SpjkE[exp(12Λtk'ΛtkΛtk'εt+1Aτ1kBτ1kft+1)|ft,st=j,st+1=k])=rtj+log(k=1Spjkexp(12Λtk'ΛtkAτ1kBτ1k'μtj,k)×E[exp((Λtk'+Bτ1k'Lk)εt+1)|ft,st=j,st+1=k])=rtj+log(k=1Spjkexp(Aτ1kBτ1kμtj,k+Bτ1kLkΛtk+12Bτ1kLkLkBτ1k))

and

p¯t,1j=log(exp(rtj))=rtj.

Then the expected value of the log price is given by

E[p¯τ1,t+1|ft,st=j]=k=1SpjkE[p¯τ1,t+1k|ft,st=j,st+1=k]=k=1Spjk(Aτ1kBτ1kE[ft+1|ft,st=j,st+1=k])=k=1Spjk(Aτ1kBτ1kμtj,k).

Next, the expected excess return is derived in the following way:

E[p¯τ1,t+1|ft,st=j]+p¯1,tjp¯τ,tj=k=1Sptjk(Aτ1kBτ1kμtj,k)rtj{rtj+log(k=1Spjkexp(Aτ1kBτ1kμtj,k+Bτ1k'LkΛtk+12Bτ1k'LkLk'Bτ1k))}=k=1Sptjk(Aτ1kBτ1kμtj,k)log(k=1Spjkexp(Aτ1kBτ1kμtj,k+Bτ1kLkΛtk+12Bτ1kLkLk'Bτ1k))k=1Sptjk(Aτ1kBτ1kμtj,k)logk=1Spjk(Aτ1kBτ1kμtj,k+Bτ1kLkΛtk+12Bτ1kLkLk'Bτ1k+1)k=1Sptjk(Aτ1kBτ1k'μtj,k)k=1Spjk(Aτ1kBτ1kμtj,k+Bτ1k'LkΛtk+12Bτ1kLkLk'Bτ1k)=k=1Spjk(Bτ1kLkΛtk+12Bτ1kLkLk'Bτ1k).

To derive the above result, we applied log-linearization for exp(y) and log(x). The argument of the exponent is a return, which is a sufficiently small number. Therefore, it can be approximated as exp(y)≈y+1. k=1Spjk(y+1)x is a number sufficiently close to 1, and therefore can be approximated as log(x)≈x–1.

Appendix C. Details of estimation techniques

Appendix C.1 State Space Form

We begin by providing the details for the state space form, which comprises the transition and measurement equations and is the basis for model estimation. The transition equation of the state space form is given by equation (3). To derive the measurement equation, we follow Dai, Singleton, and Yang (2007) and assume that one yield, in particular the 12 quarter maturity yield (R12,t), is priced without error. This yield is entitled basis yield. We choose the 12 quarter maturity yield to be priced without error based on the finding in Chib and Kang (2013) that the yields in the middle of the yield curve have the lowest variance of the measurement errors. As a result, the pricing equation for this yield has the form:

(21)R12,t=a12st+b12stft=a12st+bu,12stut+bm¯,12stm¯t, (21)

where

b12st=(bu,12stbm¯,12st)

and m¯t denotes the vector of macro factors (πt, gt)′. This assumption allows the latent factor to be expressed in terms of observable yields and macro variables:

(22)ut=(bu,12st)1(R12ta12stbm¯,12stm¯t). (22)

Thus,

(23)ft=(utm¯t)=((bu,12st)1(R12ta12stbM¯,12stm¯t)m¯t). (23)

By denoting the vector of all yields other than R12t by Rt and yt(Rt, ft)′, the measurement equation can be expressed as

(24)yt=(a¯st0)A¯st+(b¯stI3)B¯stft+(I703×7)ε˜t,ε˜t~iidN(0,Σ), (24)

where Σ is the variance-covariance matrix for the measurement errors, which is assumed to be a diagonal and regime independent, and α¯st and b¯stdenote the vector and matrix of all stacked aτst and bτst excluding α12st and βu,12st.

Appendix C.2 Prior Distribution

We set the prior distributions of the model parameters based on the general observation that, on average, the yield curve is upward sloping. Following Chib and Ergashev (2009), we simulate parameters and model-implied yield curves from the prior distributions to ensure that our prior produces, on average, a reasonably shaped yield curve. At the same time, we set the variances of key parameter distributions to be relatively large so that the distributions cover economically reasonable values of parameters. The prior for the diagonal elements of G is based on the fact that interest rates, inflation, and the output gap are all persistent time series. Since λ0st and Ωst are key parameters determining the term premium, their means are set based on the simulation outcomes of the model-implied yield curve. To see the prior implied outcomes, we sample the parameters 25,000 times from the prior distributions and simulate factor dynamics and yield curves. This simulation exercise produces, on average, a slightly upward-sloping yield curves with substantial variation between –3% and 15%. Our specific prior distributions are as follows.

First, we describe the approach for estimating the transition probabilities. We estimate the transition probabilities separately for each regime process as functions of normally distributed parameters

(25)prgjk=11+exp(ηrgjk),jk, (25)

which truncates the transition probability values to be within 0 and 1 bounds.

We assume that all parameters, denoted as θ, are distributed independently from each other. Table 3 provides detail for the prior distributions of the parameters. We set the prior for all variances to be defuse to ensure that the prior implied yield curve and the factor processes have considerable variations. Parameters Ω1, Ω2, Σ are reparameterized using coefficients

Table 3

Prior distributions.

ParameterDensityMeanStd.
α1, α2Normal0.400.401.001.00
β1, β2Normal0.300.301.001.00
GNormal0.800.000.000.200.100.10
0.000.800.000.100.200.10
0.000.000.800.100.100.20
λ01Normal–0.10–0.10–0.100.300.300.30
λ02Normal–0.10–0.10–0.100.300.300.30
λfNormal1.001.001.002.002.002.00
ηm12,ηm21Normal3.483.480.500.50
ηλ12,ηλ21Normal3.483.480.500.50
dΩ×Ω1, dΩ×Ω2Defuse prior1.001.000.230.23
dΣ×ΣDefuse prior1.000.15

All elements of the reparameterized dΩ×Ω1, dΩ×Ω2, and dΣ×Σ matrices have the same prior means and standard deviations within each matrix stated in the Table, where dΩ and dΣ are defined by (26) and (27). The prior for ηrg12 and ηrg21 implies the prior for prg12 and prg21 with means and standard deviations equal to 0.03 and 0.02, respectively.

(26)dΩ=(5×1055×1057×104) (26)

and

(27)dΣ=(7×1054×1063×1076×107107107107). (27)

Appendix C.3 Posterior Distribution and MCMC Sampling

The posterior distributions of parameters are simulated by Markov Chain Monte Carlo (MCMC) methods. The joint posterior distribution to be simulated is described by

(28)π(θ,ST|y)f(y|θ,ST)f(ST|θ)π(θ), (28)

where f(yθ, ST) is the likelihood function for data, denoted by y comprising time series of all yields and macro factors, given all parameters of interest θ and time series of regimes ST={st}t=0,1,,T; f(STθ) is the density function for regime-indicators given the parameters; π(θ) is the prior density of the parameters.

The MCMC procedure is summarized as follows:

  • Step 1: Initialize (θ, uT, ST); where uT={ut}t=0T is the time series of the latent factor and ST={st}t=0T is the time series of regimes;

  • Step 2: Sample θ conditional on (ST, FT, RT), where FT={ft}t=0T is the time series of factors and RT={Rt}t=0T is the time series of yields;

  • Step 3: Sample ST conditional on (θ, FT, RT);

  • Step 4: Compute uT conditional on (θ,ST,m¯T,R12,T) using equation (22), where m¯T={m¯t}t=0...T is the time series of macro factors and R12,T={R12,t}t=0…T is the time series of basis yield;

  • Step 5: Repeat Steps 2–4 (n0+n) times, then disregard the first n0 iterations, which are burn-in iterations, and save n draws of the parameters.

The following provides details of the MCMC algorithm and the construction of the likelihood function.

Step 2: Samplingθ

Parameters θ conditional on (ST, FT, RT) are sampled using the Metropolis-Hastings (MH) algorithm. Because it is difficult to find an optimal parameter blocking scheme due to the high dimension of parameter space of the model, we use the tailored randomized block M-H (TaRB-MH) method developed by Chib and Ramamurthy (2010). The general idea of this method is in setting a number and composition of blocks randomly in each sampling iteration. We let the proposal density q(θiθi, y) for parameters θi in the ith block, conditional on the value of parameters in the remaining blocks θi to take the form of a multivariate student t distribution with 15 degrees of freedom

q(θi|θi,y)=St(θi|θ^i,Vθ^i,15),

where

θ^i=argmaxθiln{f(y|θi,θi,ST)π(θi)}andVθ^i=(2ln{f(y|θi,θi,ST)π(θi)θiθi)|θi=θ^i1.

Following Chib and Kang (2013) and Chib and Ergashev (2009), we solve numerical optimization problem using the simulated annealing algorithm, which has better performance in this problem than deterministic optimization routines due to high irregularity of the likelihood surface.

Next, we draw a proposal value θi from the multivariate student t distribution with 15 degrees of freedom, mean θ^i and variance Vθ^i. If the proposed value does not satisfy the model imposed constrains, then it is immediately rejected. The proposed value, satisfying the constraints, is accepted as the next value in the Markov chain with probability

α(θi(g1),θi|θi,y)=min{f(y|θi,θi,ST)π(θi)f(y|θi(g1),θi,ST)π(θi(g1))St(θi(g1)|θ^i,Vθ^i,15)St(θi|θ^i,Vθ^i,15),1},

where g is an index for the current iteration. The completed simulation of θ in the gth iteration with hg blocks produces sequentially updated parameters in all blocks:

π(θ1|θ1,y,ST),π(θ2|θ2,y,ST),,π(θhg|θhg,y,ST).

Now we derive the log-likelihood function conditional on θ and ST, which has the form:

logf(y|θ,ST)=t=1Tlogf(yt|It1,θ,ST),

where It1={yn}n=0t1 denotes the information set available for the econometricians at time t–1. Given the model specification, yt conditional on st–1=j, st=k, It–1, and θ is distributed normally with the mean and variance defined as

yt|t1jkE[yt|st1=j,st=k,It1,θ]=A¯k+B¯kμt1j,kVt|t1jkVar[yt|st1=j,st=k,It1,θ]=B¯kLkLkB¯k'+(Σ000)W¯.

Thus, the conditional density of yt becomes

(29)f(yt|st1=j,st=k,It1,θ)=1(2π)10/2|Vt|t1jk|1/2(12(ytyt|t1jk)[Vt|t1jk]1(ytyt|t1jk)). (29)

Step 3: Sampling regimesST

Regimes ST are sampled from f(STIT, θ) in a single block in backward order. First, the regime probabilities conditional on It and θ are obtained by applying the filtering procedure developed by Hamilton (1989) as follows:

  • Step 1: Probabilities of regime s0 conditional on available information at time t=0 and parameters are initialized at unconditional probabilities of regimes denoted by psteadystate:

    Pr(s0|I0,θ)=psteadystate.

  • Step 2: The joint density of st–1 and st conditional on information at time t–1 and parameters is given by

    (30)Pr(st1=j,st=k|It1,θ)=pjkPr(st1=j|It1,θ). (30)
  • Step 3: Then, the density of yt conditional on information at time t–1 and parameters is given by

    (31)f(yt|It1,θ)=j,kf(yt|st1=j,st=k,It1,θ)Pr(st1=j,st=k|It1,θ), (31)

    where the first and second terms are given by equations (29) and (30), respectively.

  • Step 4: The joint density of st–1 and st conditional on information at time t and parameters is obtained by using the Bayes rule:

    Pr(st1=j,st=k|It,θ)=f(yt,st1=j,st=k|It1,θ)f(yt|It1,θ)=f(yt|st1=j,st=k,It1,θ)Pr(st1=j,st=k|It1,θ)f(yt|It1,θ),

    where the first and second terms of the nominator are given by equations (29) and (30) and the denominator is given by equation (31).

  • Step 5: By integrating out regime st–1 we obtain the probabilities of regime st conditional of information at time t and parameters:

    Pr(st=k|It,θ)=jPr(st1=j,st=k|It,θ).

Next, the regimes are drawn backward based on regime probabilities. In particular, regime sT is sampled from Pr(sTIT, θ) and then for t from T–1 to 1 regimes are sampled from probabilities computed sequentially backward as

Pr(st=j|It,st+1=k,θ)=Pr(st+1=k|st=j)Pr(st=j|It,θ)j=1nPr(st+1=k|st=j)Pr(st=j|It,θ),

where n is the total number of regimes.

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The online version of this article (DOI: 10.1515/snde-2013-0031) offers supplementary material, available to authorized users.


Published Online: 2014-8-23
Published in Print: 2015-4-1

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