|mEIilIEM PI RI CAL
Empirical Economics (1993)18 : 707-727
IIEIII/ECONOMICS
The HUMP-Shaped Behavior of Macroeconomic
Fluctuations
PIERRE PERRON1
D6partement de Sciences Economiques et C.R.D.E. Universit+de Montr6aI C.P. 6128,
Succ. A Montreal, Qu6bec, Canada, H3C-3J7
Abstract: We analyze the nature of persistence in macroeconomic fluctuations. The current view
is that shocks to macroeconomic variables (in particular real GNP) have effects that endure over an
indefinite horizon. This conclusion is drawn from the presence of a unit root in the univariate time
series representation. Following Perron (1989), we challenge this assessment arguing that most
macroeconomic variables are better construed as stationary fluctuations around a breaking trend
function. The trend function is linear in time except for a sudden change in its intercept in 1929 (The
Great Crash) and a change in slope after 1973 (followingthe oil price shock). Using a measure of
persistence suggested by Cochrane (1988) we find that shocks have small permanent effects, if any,
To analyze the effects of shocks at finite horizon, we select a member of the ARMA(p, q) class
applied to the appropriately detrended series. For the majority of the variables analyzed the implied
weights of the moving-average representation have the once familiar humped shape.
Key Words: Measures of persistence, unit root, trend-stationarity, ARMA models, non-stationarity,
structural change.
JEL Classification System-Numbers: C22, E32
I
Introduction
The most widely used m o d e l i n g device in empirical economics characterizes
a time series variable b y some d y n a m i c structure subject to shocks that are
u n c o r r e l a t e d over time. There are m a n y ways to i n c o r p o r a t e this a p p r o a c h
in a particular analysis. The a p p r o a c h popularized by Box a n d Jenkins (1970)
analyzes the b e h a v i o r of a u n i v a r i a t e series by a n autoregressive m o v i n g average representation. Here, the d y n a m i c s of the system, or the p r o p a g a t i o n
m e c h a n i s m , is represented by the effect of past values of the variable a n d of the
u n d e r l y i n g shocks o n the present value of the variable. M o v e m e n t s of a given
variable are essentially driven by the present a n d past realizations of the shocks.
The n a t u r e of these shocks is generally left unspecified a n d can e n c o m p a s s
various factors such as m o n e t a r y policy surprises, technological shocks, changes
] I wish to thank Christian Dea and Serena Ng for research assistance as well as Charles Nelson
and John Campbell who kindly provided some of the data used in this study. Research support from
the Social Sciencesand Humanities Research Council of Canada and the Fonds pour la Formation
de Chercheurs et l'Aide/t la Recherche du Qu6bec is acknowledged.
0377- 7332/93/4/707 - 727 $2.50 9 1993 Physica-Verlag,Heidelberg
708
P. Perron
in foreign conditions, exogenous governmental policy variations, etc. In general,
the shocks may be viewed as a composite of factors.
A problem that has received considerable attention in the literature concerns
the effects of a shock on future values of the level of the variable. As an example
of such concern, consider the opening of Blanchard's article (1981, p. 150):
One of the few undisputed facts in maeroeconomics is that output is humped
shaped, or more precisely that the distribution of weights of the moving average
representation of the deviation of quarterly output from an exponential trend
has a hump shape.
Of course, this so-called 'undisputed fact' has been seriously challenged
recently, to the extent that it is now perceived as counterfactual. A composite
shock is now thought to have a lasting effect on the level of output and most
other macroeconomic variables. The latter view contrasts sharply with the 'humpshaped' description, which defines a case where the effects of a shock are negligible after some period of time.
The contrasting assessments result essentially from different methods of making a series stationary, i.e., different detrending procedures. According to the
earlier wisdom used by Blanchard to obtain the hump-shaped result, the trend
exhibited by many macroeconomic variables is essentially deterministic. The
trend can be succinctly represented by a linear first-order polynomial in time
applied (usually) to the logarithm of the series. This view has been challenged,
most notably by Nelson and Plosser (1982), who argue that the trend is primarily stochastic due to the presence of a unit root (with drift) in the univariate
representation of the series. The unit-root characterization implies that shocks
have a permanent effect on the level of the series.
Various studies have attempted to calculate the long-term percentage change
in the level of a variable following a one percent innovation. These include
Campbell and Mankiw (1987a, b, 1989), Cochrane (1988), Evans (1989), Clark
(1987), Watson (1986) and Blanchard and Quah (1989). While the authors may
disagree as to the precise long-term effect, and particularly whether it is greater
or less than one percent, the consensus appears to be that it most likely is
greater than zero. For example, Campbell and Mankiw (1987b, p. 1tl) argue
that "Much disagreement remains over exactly how persistent are shocks to
output. Nonetheless, among investigators using postwar quarterly data, there is
almost unanimity that there is a substantial permanent effect."
The purpose of the present study is to try to refloat the hypothesis that the
effects of shocks on most macroeconomic variables are short-lived and are, in
fact, hump-shaped. We extend a previous analysis (Perron (1989)), where we
argued that the statistical non-rejection of the unit-root hypothesis for macroeconomic data was essentially due to the presence of the 1929 Great Crash and
the post-1973 (post-oil-price shock) slowdown in growth. These extraordinary
events correspond to a shift in the intercept of the trend function in 1929 and a
sudden change in its slope in 1973. Regardless of whether these two events are
The HUMP-Shaped Behavior of Macroeconomic Fluctuations
709
seen as large outliers or as exogenous (i.e., not realizations of the underlying
probability structure of the shocks), the results in Perron (1989) suggest that the
non-rejection of a unit root is due in large part to the occurrence of these two
events. A way to isolate the events, i.e., to take them out of the noise function
characterizing the variables, is to allow for non-linear trends. More specifically,
if a sudden change in the intercept of the trend function in 1929 and a change
in its slope in 1973 are permitted, the evidence for a unit-root hypothesis is
considerably weakened. Here, shocks have no permanent effects except those
associated with the 1929 crash and the slowdown in growth after 1973.
The present paper deals with two issues. The first is a reassessment of the
findings described above, using the method following Cochrane (1988) and
Campbell and Mankiw (1987a), which calculates the long-term effect of shocks
by estimating the spectral density of the first-differences of the series at the zero
frequency. This approach is particularly useful since this measure of persistence
will be shown to be (asymptotically) unaffected by the presence of a 'crash' (i.e.,
a sudden change in the intercept of the trend function). We investigate various
series for real GNP, including a long span of annual data and a post-war quarterly series. We also analyze the series used in Nelson and Plosser (1982). Our
findings tend to confirm our earlier results. The effects of shocks vanish over
a long horizon. It must be noted, however, that the present analysis is not
intended to provide a formal statistical test to discriminate between the classes
of trend-stationary (possibly with breaks) and differenced-stationary processes.
Rather, our intention is to provide qualitative results that support our earlier
claim as well as offering a possible explanation of differing results found by
Cochrane and Campbell and Mankiw.
The second aim of the paper is to characterize the stochastic structure of the
'detrended' series using the non-linear trend described above. To this effect, we
use the Akaike and Schwartz criteria to select members within the class of
ARMA models. With very few exceptions, the appropriate stochastic structure
is an AR(2) or ARMA(1, 1) with very similar dynamic properties. In most cases,
the weights in the moving-average representation have a hump-shape.
The paper is organized as follows. Section 2 introduces the models considered
and discusses the non-parametric statistic used to measure the persistence effects.
Section 3 analyses the behavior of this statistic under the hypothesis that the
trend function contains a single break. Section 4 presents an empirical analysis
of the Nelson-Plosser data set, and Section 5 considers various real GNP
series. In each case, the impulse-response function corresponding to the selected
stochastic models are described. Finally, Section 6 presents some concluding
comments and a discussion of the implications of our results for macroeconomic
modeling, forecasting and the issue of detrending to achieve stationarity.
710
2
?. Perron
The Models and the Statistics
The *extraordinary' nature of the 1929 crash and the 1973 oil-price shock when
compared to the modern historical experience motivates the present analysis.
The 1929 crash witnessed a sudden and dramatic decline in aggregate economic
activity, while the 1973 oil-price shock is associated with the beginning of the
slowdown in growth experienced by most western industrialized countries.
There are several possible statistical modeling strategies to incorporate these
major events. On the one hand, one can view the 1929 crash as a realization of
a shock issued from the same probability distribution as any other shock. This
would imply a fat-tailed distribution, possibly one with infinite variance. The
problem with this approach is that most statistical techniques are valid for finite
variance distributions, and there is a clear possibility that such a single major
event biases the statistics in favor of the unit-root hypothesis. This was shown
formally in Perron (1989). Since the issue here is whether or not "regular"
shocks have permanent effects, one may wish to remove the influence of a big
outlier and see what the rest of the noise can tell us about the properties of the
system. On the other hand, one can view such a large event, not as a realization
issued from the same probability distribution as the other shocks, but as a quite
separate random event. The idea is that the economy is regularly subjected to
some shocks (call them "regular shocks," say) but that once in a while it is
disrupted by a major event. This modeling strategy would allow two types of
shocks issued from quite different probability distribution functions. For instance, one may wish to model the major events as realizations from a Poisson
process. To be more precise, consider the following specification for a given
variable y~:
yt -- ~lt + Z t ;
rh -- pt + ~tt
(1)
where A(L)Z~ = B(L)6; e~ ,~ i.i.d.(0, o=); #~ = #t-1 + V(L)vt and fl~ = ~-1 +
W(L)w~. Here, the Z[s are (not necessarily stationary) deviations from the trend
function ~/,. The intercept and the slope of the trend functions, #~ and ~, are
themselves random variables modeled as integrated processes with W(L), V(L)
stationary and invertible polynomials. However, the important distinction is
that the timing of the occurrence of the shocks v, and w~ are rare relative to
the sequence of innovations {6}; for example, Poisson processes with arriva!
rates specified such that their occurrences are rare relative to the frequency of
the realizations in the sequence {6}- The intuitive idea behind this type of
modeling is that the coefficients of the trend function are determined by longterm economic fundamentals (e.g., the structure of the economic organization,
population growth, etc.) and that these fundamentals are rarely changed. In our
examples, v~is non-zero in 1929 (the great depression) and w~is non-zero in 1973
(the oil-price shock).
In any event, since we are interested in the effects of "regular" shocks (the et
in the notation of (1)) through time on various aggregate variables, a useful way
The HUMP-Shaped Behaviorof MacroeconomieFluctuations
711
to approach the problem is to view these major events as part of the deterministic trend function. This follows the spirit of the Box-Tiao (1975) intervention
analysis where we take "outlier" or "aberrant" events out of the noise function
and analyze what the remaining noise can tell us about the properties of interest.
This is the route we follow.
Following Nelson and Plosser (1982), Campbell and Mankiw (1987a),
Cochrane (1988) and others, we parameterize a model which possibly exhibits
permanent effects of shocks by the imposition of an autoregressive unit root
with a possibly non-zero drift. However, the approach is generalized to allow a
one-time change in the structure occurring at a time T~ (I < Ts < T, where T is
the sample size). Three different models are considered under this hypothesis:
one that permits an exogenous change in the level of the series (a "crash"),
one that permits an exogenous change in the rate of growth and one that allows
both changes. The models are, under the null hypothesis of a unit root:
Model (A): Yt = ,u + yD(TB)t + Yt-1 + et
,
Model (B): Yt = I2 + ODUt + Yt-~ + et ,
Model (C): Y t
=
12 + 7D(TB), + ODU~ + Yt-~ + ez ,
where D ( T B ) , = 1 if t = Tn + 1, 0 otherwise, D U t = 1 if t > TB, 0 otherwise,
and A ( L ) e t = B(L)v,, v, ,,~ i.i.d.(0, o-2) with A ( L ) and B(L), pth and q,h order polynomials, respectively, in the lag operator L. More general conditions on the
errors {et} are possible but to ease the presentation we shall only consider these
simpler ones. 2
The cases where the shocks have no permanent effect on the level of the series
{y,} are represented by trend-stationary models parameterized as follows:
M o d e l ( A ) : y , = 1 2 + 7 DU t + flt + w~ ,
Model (B): y, = (12 - OTs) + fit + ODT~ + w, ,
Model (C): Yt = (12 - OTB) + yDUt + fit + ODT, + w~ ,
where D Tt = t, if t > TB, 0 otherwise, and F ( L ) w t = D(L)vt; vt ,,, i.i.d.(0, a2), with
F ( L ) and D(L) again finite order polynomials in L. Model (A) describes what we
refer to as the crash model. The parameter ~ represents the magnitude of the
change in the intercept of the trend function occurring at time T~. Model (B) is
referred to as the "changing growth" model and 0 represents the magnitude of
the change in the slope of the trend function. Model (C) allows for both effects
to take place simultaneously, i.e., a sudden change in the level of the series
followed by a different growth path.
2 Note also that we describe the models in terms of the "additive outlier version"as opposed to
the "innovational outlier version,"a distinction which is discussed in Perron (1989).This does not
affectany of the results that follow.
712
P. Perron
In our earlier study, we considered testing the null hypothesis of a unit root
in a variety of macroeconomic time series allowing for such changes in the trend
function. The statistics derived were in the spirit of the Dickey-Fuller (1979)
procedure and required the tabulation of a new set of critical values. An alternative is to consider the procedure suggested by Cochrane (1988) and Campbell
and Mankiw (1987a) to provide a measure of the persistence effect of shocks~ It
is based on the properties of the noise function of the first-differences of the data.
Unit-root and trend-stationary models can be nested as:
Model (A): Ay, = ~ + 7D(TB), + ur ,
(2)
Model (B): Ay~ = tr + ODUr + ut ,
(3)
(4)
Model (C): Ay t = ~c + 7D(TB)t + ODU, + u, .
Under the unit-root hypothesis, ~c = # (the drift) and u, = e, = A(L)-~B(L)vv
Under the hypothesis that the series is trend-stationary, ~c = fl (the initial slope
of the deterministic trend function) and u~ = (1 - L)w t = (1 - L)F(L)-~D(L)vr
Hence, when the models are parameterized in first-differences, the only difference between each hypothesis is with respect to the nature of the errors {ut}.
When the model is trend-stationary, there is a unit root in the moving-average
representation of the errors, denoted u, = O(L)v,. The long-horizon effect of a
i
unit shock in vt on the level of Yt is given by 0(1) = l i m i ~ ~j=o
0j, where %
are the coefficients in the polynomial 0(L). If the model is trend-stationary,
0(1) = 0 since ~b(L) = (1 - L)F(L)-~D(L)vr On the other hand, if the model
contains an autoregressive unit root 0(1) > 0.
Cochrane (1988) has proposed an alternative measure of persistence that can
be estimated non-parametrically. The measure is based on the autocovariance
function of the differenced process, which can be related to the moving average
polynomial ~,(z) as C(z)
@(z)0(z-1)o "2 where C(z) = ~ = _ ~ Cjz j, Cj is the jth
autocovariance of the first-differenced process, and a 2 is the variance of the
innovations {vt}. Denoting the variance of the first-differenced process as a2
( = Co), the measure of persistence is given by V = C(1)/a 2, and is related to ~p(1)
by V = (az~/a 2) [~,(1)] 2. The measure V is simply 2~ times the normalized spectral density of the process {u~} evaluated at frequency zero. V and 0(1) are not
equivalent except in some special cases, in particular when ~(1) = 0 when there
is no persistence. For us, this is the interesting case, and we shall work directly
with the measure V and show that for most series its estimate turns out to be
close to zero.
-Ay
t = Yt _ Y~-i _ ~ where fi = T - 1 '~'~T
z.x (ty ~ - Yt-~) = T - t ( Y T . Yo) is the
Let
estimate of the slope of the trend function. A general class of estimators of the
spectral density at the origin is given by:
=
k
~ k = 1 -t-2 Z w(k, j)[)j ,
j=l
where
(5)
The HUMP-Shaped Behavior of Macroeconomic Fluctuations
~j = ( T / ( T - j))
~
(Ay, Ay,_i)
(~,)2 ,
713
(6)
t=j+l
with k a truncation lag parameter and w(k, j) a lag w i n d o w ? M a n y possible
choices of lag windows are available, and for ease of c o m p a r i s o n of our results
with the previous literature, we choose the Bartlett triangular window defined
by w(k, j) = 1 - j/(k + 1). I~k is a consistent estimate of V if k ~ oe and k / T --. 0
as T - , oc. Its asymptotic standard error is given by (see, e.g., Priestley (1981,
p, 463)):
s.e. [I~k] = v k / [ ( 3 / 4 ) ( T / ( k + 1))] 1/2
(7)
As a measure of persistence, 17k has several advantages due mainly to the fact
that it is non-parametric. However, a problem in finite samples concerns the
appropriate choice of the truncation lag parameter k. Campbell and M a n k i w
(1987b) conducted a small M o n t e Carlo experiment with 130 observations with
a r a n d o m walk and a stationary AR(2) model. They found that a value k of at
least 30, and preferably 40 or 50 (i.e., more than 1/3 of the total sample size) is
needed to be able to distinguish the above-mentioned models. P e r r o n and N g
(1992) found that the exact mean-squared error of I7k is minimized using a large
value of k if V is small, and a small value of k if V is large (e.g., in the vicinity of
1). Given our earlier results (Perron (1989)) that most m a c r o e c o n o m i c time
series appear to be best construed as "trend-stationary" if allowance is m a d e for
a shift in the trend function, more weight should be given to estimates of 17k with
k quite large, say between 1/3 and 1/2 of total sample size. This a p p r o a c h is
taken in the empirical sections, t h o u g h we present estimates ~k for a wide range
of values for k. 4
It is by now u n d e r s t o o d that statistics such as the variance ratio or any
estimate of the spectral density at the origin have p o o r properties as formal tests
to distinguish trend-stationary versus difference-stationary processes (see, in
particular, Cecchetti and L a m (1991)). The basic problem is that the finite sample confidence intervals are very wide if the process has a unit root. We verified
3 1?k as defined by (5) and (6) does not necessarily lead to a non-negative estimate of V. It would
do so if the biased estimates ofpj were used, i.e., without the correction factor (T/(T - j)). We report
results using 17k,as defined in (5) and (6), to permit a comparison with previous studies, namely those
of Cochrane (1988) and Campbell and Mankiw (1987a). Estimates of V using a variety of windows
and truncation lags were also computed and are available upon request. The results are not very
sensitive to other choices of windows and lead to the same conclusions.
4 The use of data-dependent methods to select the truncation lag parameter k, as in Andrews
(1991) for example, is problematic in the present context. Such methods usually start with a preliminary estimation of a simple time series model, such as an AR(1). The optimal truncation lag is then
a function of the estimated value of this autoregressive parameter. The problem with applying such
a procedure is that, as shown in Perron (1989), the presence of a break in the trend function will bias
the estimated first-order autocorrelation coefficient towards 1. In this context, the chosen truncation
lag parameter may be inappropriate. We therefore prefer the presentation of a range of values to
assess the robustness of the results.
714
?. Perron
this by doing the following experiment. We first assumed no break in the data
and estimated, for each series, an AR process with a unit root. We then simulated the statistic 17k for various values of k. Except in some rare cases, the
confidence intervals were so wide that no discrimination was possible.
With this caveat in mind we nevertheless applied the following modification
of an asymptotic test suggested by Phillips and Ouliaris (1988). The test is based
on the fact that I~ is asymptotically normal with mean V and variance given by
the square of (7). Their procedure is a bounds test based on the asymptotic
distribution. Let H be the hypothesis that the process is trend-stationary. Atso
let z, be the e-percentage point of the normal distribution. We say that we
accept H if lTk + Z,{S.e.(l~k)} < C*, for some bound c*; correspondingly we say
that we reject H if 12k - z~{s.e.(l~k) } > c*. If none of the inequalities are satisfied
the test is viewed as inconclusive. Of course, the procedure is quite arbitrary in
the sense that a choice of c* must be made. Moreover, for any such choice of e*
the test will likely have some size distortions in finite sample for particular
classes of data-generating processes. In any event, it nevertheless provides an
asymptotically valid procedure and permits us to infer, in some sense, the most
likely hypothesis (see the discussion in Phillips and Ouliaris (1988)). The particular choice of c* is discussed in the empirical sections, s
3
Properties of pk with a Breaking Trend Function
To understand the empirical results described in the next sections, it is instructive to analyze the asymptotic behavior of the usual sample autocorrelations
(with only a constant mean subtracted) when the trend function contains a
break. We wish to derive the limit of ~j when in fact the true process is either
given by equation (2) (a change in the intercept of the trend function) or equation (3) (a change in the slope of the trend function). As will be apparent from
the results below, the behavior of kj when the true model is equation (4) (both
changes allowed) is equivalent to that under equation (3).
To perform the asymptotic analysis, we require Tn to increase at the same rate
as T. For simplicity, we let TB/T = 2 for all values of T. We denote by pj the true
autocorrelation coefficient at lag j of the process {ut} and C(j) the true autocovariance at lag j of the same process. We collect our results in the following
Theorem, whose proof can be obtained by slight modifications of the proof of
Theorem 1 in Perron (1990).
s
We view the bounds test of Phillips and Ouliaris (1988) not as a formal test per se bm rather as
providing indirect evidence. We discuss in more detail, in the empirical sections, the strategy used to
select the bound and how such a choice can help us draw some inference of interest.
The HUMP-Shaped Behaviorof MacroeconomicFluctuations
715
Theorem I: Let ~j be defined by (6). Then as T ~ oo with T~/T = 2 for all T, we
have: a) if Ay~ is 9enerated accordin9 to (2): ~)j ~ pj; b) if Ay~ is 9enerated accordin9 to either (3) or (4), ~j ~ [2(1 - 2)0 2 + C(j)]/[),(1 - ).)0 z + C(O)~.
This Theorem shows that the standard sample autocorrelations are consistent estimates of their population values only for Model (A) where a break is
present in the intercept of the trend function. This result is intuitively clear, since
the mean of the first-differenced series is constant except for a single period. The
effect of neglecting this change vanishes asymptotically. There may, however,
remain a bias in finite sample.
Things are different when there is a break in the slope of the trend function.
Here, the sample autocorrelations are inconsistent estimates of the population
autocorrelation coefficient. An interesting feature is that the limit is greater than
the population value at any lag. The asymptotic bias is positive for all autocorrelations. The bias is greater the larger the relative magnitude of 2(1 - 2)0 2
compared to C(j) and C(0). In particular, the larger the break the greater is the
bias. For a given value of 0, the bias is maximized when 2 --= 1/2, with a break at
mid-sample. A consequence of this result is that one can expect tTk to be an
inconsistent estimate of V if a break in the slope of the trend function is not
taken into account. More importantly, l~k (using the standard autocorrelations
~3j) will tend to overestimate V, thereby suggesting a much greater degree of
persistence than exists. In particular, l~k will suggest some persistence even if the
shocks have no long-term effects.
To obtain consistent estimators in the presence of a change in the slope of the
trend function we need alternative estimates of the autocorrelation function of
{u~}. To this effect, first denote by z137t the "demeaned" series Ay t where allowance is made for a possible change in mean at time TB. More specifically AYt is
defined as the residuals in the following regression estimated by ordinary leastsquares:
Ay, = ~ + ODu, + ~y,
(8)
with DUt = 1 if t > Tn (0 otherwise). 12k is computed using (5-6) with Ayt instead
of Ay r
4
Analysis of the Nelson-Piosser Series
We analyze the series considered by Nelson and Plosser (1982) for several reasons.
First, it is a rich data set with a wide range of annual series covering a long
historical period. More importantly, it allows us to make some interesting comparisons between the results in the original Nelson-Plosser study and Perron
716
P, Perron
(1989). An interesting feature is that all series end in 1970 and cover the period
of the 1929 crash. Hence, for each series only one break is likely to be present.
For reasons discussed in Perron (1989), we consider model (A) (only a change in
the intercept in 1929) for the series Real GNP, Nominal GNP, Real Per Capita
GNP, Industrial Production, Employment, GNP Deflator, Consumer Prices,
Nominal Wages, Money Stock, Velocity and Interest Rate. We consider model
(C) (a change in both the intercept and the slope in 1929) for Real Wages and
Common Stock Prices. We do not consider any change in the trend function for
the unemployment series since there is agreement that it is stationary for the
period under consideration. 6
For most of the series considered there is only a change in the intercept of the
trend function. On the basis of Theorem 1, I~k is not influenced, asymptotically,
by the presence of such a change. However, as discussed in Perron (1989), stano
dard Dickey-Fuller tests for a unit root are biased toward non-rejection of the
unit-root hypothesis even asymptotically. Hence, it can be viewed as an alternative to standard tests for a unit root which is robust to a sudden change in the
intercept of the trend function and should, in principle, yield results similar to
those obtained in our earlier study.
The estimated measures of persistence (without any corrections for changes in
the trend function) are presented in Table 1. We tabulate results for the following values of the truncation lag parameter k: 8, 16, 20, 30, 40 and 50. The results
are quite striking. The estimates show very little evidence of persistence for alt
series, with the exception of Consumer Prices, Velocity and Interest Rate, precisely those series for which the unit root could not be rejected in Perron (1989).
The results are sometimes quite extreme. For example, consider the Industrial
Production index, where l~k is 0.07 with k = 50 (less than half of total sample
size). This result is quite contrary to the unit-root hypothesis found in NelsonPlosser but is in accord with our earlier results. The results are not so dramatic
for all series but are indeed suggestive that most of them exhibit little persistence, if at all. Apart from the above-mentioned three exceptions, all series
show an estimate less than 0.33 at k = 40 (except GNP Deflator with 0.50 and
Common Stock Prices with 0.49).
We also present in Table 1.a estimates for the Real Wages and Common
Stock Price series when allowance is made for a change in slope in 1929. Following the results of Zivot and Andrews (1992) and Perron (1991) we also present
the estimates with a change in slope in 1939 for Real Wages and 1936 for
Common Stock Prices. These dates were selected as the outcome of tests for unit
roots allowing the break point to be unknown. As expected from the theoretical
result of Section 3, the estimates are noticeably smaller when allowance is made
for a change in slope, For the Common Stock Prices series the choice of t936 as
opposed to 1929 as the break date has a more significant impact.
6 Relatedresults, using the Nelson-Plosserdata set can be found in Zivot and Andrews (1992)
and Raj (1993).Evidenceof rejectionsof the unit root with historical data from many countries can
be found in Raj (1992),
The HUMP-Shaped Behavior of Macroeconomic Fluctuations
717
Table I. Non-parametric estimates of persistence (l?k); Nelson-Plosser data
Series
T
Real G N P
62
Nominal G N P
62
Real Per Capita G N P
62
industrial Production
111
Employment
81
Unemployment Rate
81
G N P Deflator
82
Consumer Prices
! 11
Nominal Wages
71
Real Wages
71
Money Stock
82
Velocity
Interest Rate
Common Stock Prices
!02
71
!00
k= 8
k = 16
k = 20
k = 30
k = 40
k = 50
1.01
(.45)
1.59 r'
(.71)
1.03
(.46)
.45
(.15)
1.07"
(.41)
,56
(.22)
2.16'
(.83)
2.39 r
(.79)
1.9W
(.79)
.82
(.34)
2.63 r
(1.01)
.76
(.26)
2.06 r
(.85)
.74
(.26)
.41
(.25)
1.01
(.62)
.43
(.26)
.17 a
(.08)
.55
(.29)
~20~"
(.11)
1.81
(.96)
2.23"
(i.01)
1.i5
(.65)
.49
(.28)
1.35
(.71)
.72
(.34)
2.95
(1.68)
.67
(,32)
.16"
(.11)
.69
(.47)
.45
(.30)
.214"
(.11)
.49
(.30)
.16"
(.09)
1.38
(.81)
2.00
(1.01)
.68
(.43)
.49
(.31)
.76
(.45)
.81
(.42)
3.03
(1.91)
.63
(.34)
.37
(.30)
.35
(.29)
.34
(.28)
.190"
(.12)
.29
(.21)
.12 ~
(.09)
.45
(.32)
1.65
(1.01)
.32
(.25)
.48
(.37)
.40
(.29)
.86
(.55)
2.82
(2.17)
.57
(.37)
.21
(.20)
.23
(.22)
.20
(.19)
.15 a
(.11)
.11"
(.09)
.01"
(.01)
.50
(.41)
1.49
(1.05)
.33
(.29)
.31
(.27)
.19
(.16)
.86
(.63)
1.73
(1.53)
.49
(.36)
.11"
(.12)
.06"
(.06)
.12"
(.13)
.07"
(.06)
.17
(.16)
.06"
(.06)
.68
(.62)
1.18
(.93)
.17
(.17)
.19
(.19)
.28
(.26)
.92
(.75)
.76
(.75)
.46
(.38)
Table 1.a: Non-parametric estimates of persistence
(~k) with break in trends at time Tb
Series
Tb
k= 8
k = 16
k = 20
k = 30
k = 40
k = 50
Real Wages
1929
.65
(.27)
.71
(.29)
.70
(.24)
.59
(.20)
.27
(.15)
.30
(.17)
.58
(.28)
,40
(. 19)
.24
(.15)
.29
(.18)
.52
(.28)
.31
(. 16)
.19
(.15)
.27
(.21)
.46
(.30)
.19"
(.08)
.09"
(.08)
.14~
(.12)
.44
(.33)
.12"
(.09)
.05"
(.05)
.08"
(.08)
.41
(,34)
.094
(.07)
1939
Common Stock Prices
1929
1936
Notes: i) Asymptotic standard errors computed according to (7) are in parentheses, ii)" and "denote
a rejection of the trend-stationarity hypothesis, at the 10~ and 5~o level respectively, using the
bounds test described in Section 2 with c* = 0.40. Similarly, " and " denote acceptance of this
hypothesis at the I 0 ~ and 5~o level, respectively.
718
P. Perron
Tables 1 and !.a also present the outcome of Phillips and Ouhmls (1988)
bounds test. As noted in Section 2, this test depends on the arbitrary choice of
the bound c*. We selected .40 as the value to be used in the test. The reason for
such a choice is that it allows accepting the trend-stationarity hypothesis for the
Unemployment series at the 5~ level for values of k greater than or equal to 20
and at the 10~ level for all values of k greater than or equal to 16. Since it is
generally agreed that over this sample period the Unemployment Rate series is
stationary, one would like the outcome of the test to reflect this feature, and this
particular choice achieves this goat. Nevertheless, the tests presented should be
viewed as rather suggestive and subject to the caveats discussed in Section 2.
In many instances the tests yield an inconclusive outcome 9For values of k
other than 8, only one series, the Consumer Price index, shows a test that
suggests rejection of the trend-stationarity hypothesis 0br k = t6 only). The
tests suggest accepting the trend-stationarity hypothesis with large values of k
for Real GNP, Nominal GNP, Real per Capita GNP, Industrial Production,
Employment as well as for Real Wages and Common Stock Price, when allowance is made for a change in slope in the latter two series.
These results are, in an important sense, complementary to those obtained in
Perron (1989). The issue is as follows. The measures presented in Table l suggest
the absence of tong-term persistence effects of shocks. However, standard unitroot testing procedures fail to reject the unit root hypothesis. Furthermore, as
argued by Nelson and Plosser (1982), univariate ARMA models of these series
suggest a process close to an IMA(1, 1) whose first-differences are positively
correlated. The latter would suggest a high degree of persistence. Hence, the two
approaches yield quite different implications. One way to reconcile these results
is by viewing the 1929 crash as a change in the intercept of the trend function.
As argued in Section 3, the presence of such a change will have no effect (in large
samples) on the non-parametric measure of persistenceu However, as argued in
Perron (1989), it will bias the unit-root tests towards non-rejection of the unitroot hypothesis suggesting that standard univariate ARMA modeling will show
a higher degree of persistence than is present. Given our earlier results of the
many rejections of the unit root when allowance is made for a change in the
intercept of the trend function in 1929, we incorporate such a change prior to
estimating the ARMA models for the noise function.
To analyze the effects of shocks at finite horizons we therefore adopt the
following strategy. We detrend the data by allowing a change in the intercept
between 1929 and 1930. The residuals, considered estimates of the noise of the
series, are analyzed within the class of ARMA(p, q) models. We estimated all
models with p and q less than or equal to 5. The optimal parameterization was
chosen using either the Schwartz (1978) or the Akaike (1974, 1976) criteria. The
Akaike criterion minimizes 2 In L + 2m where L is the likelihood and m = p + q
is the number of parameters. The Schwartz criterion minimizes 2 In L + m In T
where T is the total number of observations. For the sample sizes considered
here, the Schwartz criterion penalizes extra parameters more heavily. We carried
The H UM P-Shaped Behavior of Macroeconomic
Fluctuations
7t9
o
~oo~w167I ~ ~ ~ o ~ o ~
I
I
I
i
I
I
I
I
t
I
I
l
I
N.=
i
l
o
m
o
0
~~
z
9
.~
e-
~a
n~
9
~2
u~
720
P. Perron
out this procedure for all Series except Consumer Prices, Velocity and Interest
Rate, given that for these series the unit-root hypothesis is not rejected.
For the majority of the series, the first and second choices, according to both
criteria, are AR(2) and ARMA(1, 1), One notable exception is the Industrial
Production series, where the chosen model is ARMA(O, 4). Table 2 presents the
implied weights of the moving-average representation for each model selected.
Not only are the impulse responses similar across models for a given series, they
are also quite similar across series. The typical pattern is that of a hump-shape
with most of the effects vanishing within 4 to 8 years.
The evidence presented in this section appears inconsistent with the notion
that shocks have permanent effects on a wide variety of macroeconornic variables. The fluctuations around the trend function are transitory, and the weights
in the moving-average representation have the once-familiar humped-shape.
Given that more attention is given to results pertaining to real GNP in the
literature, the next section presents a more detailed analysis focusing on a number of available indices of Real GNP.
5 An Empirical Analysis of Real GNP
We analyze three GNP series that are commonly used in the literature. The first
one is Post-war Quarterly Real GNP 1947: 1-1985:4 (seasonally adjusted) from
the National Income and Product Accounts. This is the same series analyzed in
Campbell and Mankiw (1987a) except for some minor data revisions. In this
case, we allow for a change in the slope of the trend function after 1973:1
(designated as detrending method B). The second series is Annual Real GNP
1869-1983 taken from Balke and Gordon (1986). Here, we allow two breaks: a
change in the intercept after 1929 and a change in the slope after 1973 (detrending
method D). The third series is Annual Real Per Capita GNP 1869-1975 taken
from Friedman and Schwartz (1982). This series was analyzed by Perron and
Phillips (1987) and Stock and Watson (1986). Here, we allow only for a change
in the intercept after 1929 (detrending method A) since the bias due to the
change in the slope of the trend function is likely to be small with only two data
points after the change in slope in 1973.
The estimated measures of persistence are presented in Table 3. Consider first
the Post-war Quarterly Real GNP series. Row (1) reproduces the results of
Campbell and Mankiw (1987a). Row (2) gives the estimates allowing for a shift
in the slope of the trend function (Model B) after 1973: 1. It uses the residuals
from regression (8) with TR set at 1973:1. The results clearly show much weaker
evidence for persistence. For instance, at k = 50 (1/3 of total sample size), the
estimate is reduced from 0.68 to 0.13, allowing for the break; at k = 100, it is
reduced from 0.57 to 0.05. Furthermore, the outcome of Phillips and Ouliaris'
The HUMP-Shaped Behavior of Macroeconomic Fluctuations
721
C~
C~
il
II
~-~i
~I~
~'~
I~
C~
II
~
F~
_~
C~
II
. . . . . . . .
~
II
.~
"~.~'~.~
~..
..~ ~ , . . ~
. . . . .
~
9 ~.~_~
~
~
~..~ ~
~
~
~
~'~.'~.Q
~..--~. ~-~.-~. ~
~.;
.
.
.
.
.
.
.
.
.
.
.
.
~..~ ,_> ,._~ ,..; ..~ ~_~ ,..: ._>
.
.
.
.
.
.
.
.
.
.
.
.
0
0
te~
c~
. . . .
c~
Z
I
~.-.
.-7.
0
722
P. Perron
--
T T T
0
~
~
0
=~ .'~
~
~
~,~ " ~
~ o_-~,
T ~tl
.~ ~ ~ , ~
~
g
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~.
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. . . . . . .
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8
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..~ ~ ~: ~= "~
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-
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]i
%
The HUMP-Shaped Behaviorof MacroeconomicFluctuations
723
bounds test, with c * = .40 again, suggests accepting the trend-stationarity
hypothesis when allowance is made for this change in slope in 1973. Rows (3)
and (4) present results using split-sample estimates with" no correction for break,
i.e., pre- and post-1973: 1. At k = 30, the post-1973 sample yields an estimate
of - 0 . 0 6 while at k = 50, the pre-1973 sample estimate is 0.03] Hence, these
results are consistent with the fact that the high value of the measure of persistence using the full sample with no break correction is simply due to a change
in the slope of the trend function after 1973: 1.
Rows (5) through (10) present results using annual real G N P from 1869 to
1983. Rows (5) and (6) show the estimates without and with corrections for shifts
in the trend function respectively (the corrected estimates are constructed with
the residuals from (8) setting TB = 1973). Again, the estimates are lower with
corrections, though here, the differences are smaller. For both cases the outcome
of the bounds test suggests accepting the trend-stationarity hypothesis for large
values of k.
The result, that the differences in the estimates with and without corrections for breaks are small, is because the proportion of the total sample where
the change in the slope of the trend function occurs is much smaller with the
sample of annual data (2 = 105/115) than with the sample of quarterly data
()~ = 105/156). From Theorem 1 we can expect the bias to be smaller with the
former set of data if no correction is made.
Campbell and Mankiw (1987a) argued that the small measure of persistence
obtained by Cochrane (1988) was due partially to the presence of the pre-1929
data in the annual sample (compare rows (7) and (8)). However, if a correction
is made for the shift in the trend function in the post-1929 sample (again allowing
for a shift in the slope of the trend function in 1973), 1~k is smaller for the
post-1929 than for the pre-1929 period for any value of k greater than 10 (compare row (7) and row (9)). This conclusion is supported from results for the
period 1930-1972 without any corrections; for k greater than 10, the measure
of persistence is indeed small. Hence, the differences between Cochrane's and
Campbell and Mankiw's results appear not to be due to the inclusion or not of
the pre-1929 sample but to the importance of the post-1973 period relative to
the total sample.
Rows (11) through (14) present the results for Friedman and Schwartz's Annual Real Per Capita G N P series. Here no correction is made in constructing
the estimates l~k. Using either the full sample or any sub-samples, the estimates
suggest that the shocks have little permanent effects. For example, for 18691975, ITk = 0.02 at k = 60, for 1869-1929 it is 0.07 at k = 30, for 1930-1975 it is
7 As noted in footnote 2, pk does not yield a non-negative estimate by construction. When a
negative value is obtained, the asymptotic standard errors given by (7) are non-sensible,hence we
do not report them. We interpret negative values of 17k as suggestiveof a true value close to zero.
This interpretation is supported by other estimates of V (not reported) which use alternative lag
windows that yield non-negativeestimates by construction.
724
P. Perron
~o
,9~
e.
eq
Ne-~
r
a,
rr
t"q
,.A , . ~
~'-1
,,A
o
The HUMP-Shaped Behavior of Macroeconomic Fluctuations
725
0.20 at k = 20 and for 1909-1975 it is 0.21 at k = 30. In all cases, the bounds test
suggests accepting the trend-stationarity hypothesis.
To analyze the effects of shocks at finite horizons we adopted the following
strategy. Since the estimates 17~, when appropriately corrected for the 1973
shift in the slope of the trend function, show little evidence of persistence, we
detrended the data by allowing a change in the intercept after 1929 and a change
in the slope of the linear time trend after 1973. The residuals are then considered
as the noise of the series and are analyzed within the class of ARMA(p, q)
models. We estimated all models with p and q less than or equal to 5 and the
models were selected using either the Schwartz or Akaike criteria.
For the Post-war Quarterly Real GNP series, the Akaike criterion selects the
ARMA(1, 3) model, while the Schwartz criterion favors an AR(3) model. However, the AR(2) model is a close contender according to both criteria. Table 4
presents the estimated impulse response function for each model; i.e., the weights
in the moving-average representation. The results are very similar across the
three models and clearly show a hump-shaped pattern with a peak after 2
quarters. Almost all the effects vanish after 16 quarters.
The results for the Annual Real GNP series are similar. According to both
criteria the chosen model is an AR(2) with the ARMA(1, 1) a close second and
ARMA(1, 2) a close third. The estimated impulse-response functions in Table 4
show again the hump-shaped pattern with a peak in the first year consistent
with the evidence from the quarterly data. Most of the effects of the shocks
vanish sometime between the 4th and 6th years.
The evidence presented in this section is inconsistent with the notion that
shocks have a permanent effect on real GNP. As with the Nelson-Plosser data,
the fluctuations around the trend function are transitory and the weights in the
moving-average representation have the once popular humped-shape.
6
Conclusions
The present study has several implications for empirical macroeconomics. First,
it suggests an alternative procedure for detrending to achieve stationarity. Some
authors, using post-war quarterly data on economic aggregates, have detrended
using a break in trend following the 1973 oil-price shock (e.g., Blinder (1981,
1986) and Blinder and Holtz-Eakin (1986)). Our results provide a formal justification for such a procedure.
More interestingly, our results present an alternative picture of economic
fluctuations somewhere in-between the current view that fluctuations have permanent effects and the view that fluctuations are stationary around a deterministic (strictly) linear time trend. This alternative view suggests that, most of the
time, fluctuations have transitory effects and that the economy tends to revert
726
P. Perron
to a stable-trend growth path. However, occasionally the economy is disrupted
by a major event which has a lasting effect. The view suggested here is that such
permanent shocks have been quite rare but are very important in magnitude.
The non-rejection of tests of the unit root, when only a time invariant linear
trend function is allowed, can be explained within the present context by noting
that, even though the shocks which have permanent effects are rare, they are of
such magnitude as to account for a substantial portion of the total variability of
the series. Hence, it is not too surprising to find such wide evidence for unit
roots. However, this evidence tells us only that something significant and permanent occurred. We cannot infer that most shocks have permanent effects.
A third interesting issue concerns confidence intervals for long-range forecasts.
The view of stationary fluctuations around a strictly linear time trend implies an
accurate long-horizon forecast. This is thought to be quite implausible, thereby
making the unit-root characterization more plausible, since it implies ltbrecasts
with ever-increasing confidence intervals. The view suggested here implies that
forecasts constructed using the estimated trend-stationary model are adequate
for short-term forecasting, i.e., conditional on no major break in the trend function occurring in the near future. For long-horizon fbrecasting, it becomes
implausible to suggest that no shift in the trend function witl occur. Hence,
one would expect to have confidence intervals for a long-horizon forecast that
eventually increase. However, to make this statement precise, we must transform
the short-term conditional forecast into unconditional forecasts. This means
that the breaks in the trend function must be modeled statistically to produce
forecasts of the occurrence and nature of the future breaks. This is indeed an
interesting subject for future research.
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