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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">SAJEMS</journal-id>
<journal-title-group>
<journal-title>South African Journal of Economic and Management Sciences</journal-title>
</journal-title-group>
<issn pub-type="ppub">1015-8812</issn>
<issn pub-type="epub">2222-3436</issn>
<publisher>
<publisher-name>AOSIS</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">SAJEMS-21-1689</article-id>
<article-id pub-id-type="doi">10.4102/sajems.v21i1.1689</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Original Research</subject>
</subj-group>
</article-categories>
<title-group>
<article-title>What do deviation cycles measure? An analysis of the informational content of filter-based business cycles</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<contrib-id contrib-id-type="orcid">http://orcid.org/0000-0003-1520-3997</contrib-id>
<name>
<surname>Boshoff</surname>
<given-names>Willem H.</given-names>
</name>
<xref ref-type="aff" rid="AF0001">1</xref>
</contrib>
<contrib contrib-type="author">
<contrib-id contrib-id-type="orcid">http://orcid.org/0000-0003-4866-8678</contrib-id>
<name>
<surname>McLean</surname>
<given-names>Lewis</given-names>
</name>
<xref ref-type="aff" rid="AF0001">1</xref>
</contrib>
<aff id="AF0001"><label>1</label>Department of Economics, Stellenbosch University, South Africa</aff>
</contrib-group>
<author-notes>
<corresp id="cor1"><bold>Corresponding author:</bold> Willem Boshoff, <email xlink:href="wimpie2@sun.ac.za">wimpie2@sun.ac.za</email></corresp>
</author-notes>
<pub-date pub-type="epub"><day>30</day><month>08</month><year>2018</year></pub-date>
<pub-date pub-type="collection"><year>2018</year></pub-date>
<volume>21</volume>
<issue>1</issue>
<elocation-id>1689</elocation-id>
<history>
<date date-type="received"><day>02</day><month>11</month><year>2016</year></date>
<date date-type="accepted"><day>25</day><month>05</month><year>2018</year></date>
</history>
<permissions>
<copyright-statement>&#x00A9; 2018. The Authors</copyright-statement>
<copyright-year>2018</copyright-year>
<license license-type="open-access" xlink:href="https://creativecommons.org/licenses/by/4.0/">
<license-p>Licensee: AOSIS. This work is licensed under the Creative Commons Attribution License.</license-p>
</license>
</permissions>
<abstract>
<sec id="st1">
<title>Background</title>
<p>Empirical business cycle research typically commences with the extraction of a so-called deviation cycle using a time-series smoothing filter. This methodology is appealing for its pragmatism; it is easy to implement, and the output it produces is conveniently interpreted as percentage deviations from the natural level of output. However, recent literature offers staunch criticism of deviation cycle analysis, especially with regards to the assumption implicitly underlying it &#x2013; that business cycle fluctuations are restricted to distinct intervals on the frequency domain.</p>
</sec>
<sec id="st2">
<title>Aim</title>
<p>Despite its lack of a basis in theory, the analysis of deviation cycles over particular frequency ranges may still yield useful stylised business cycle facts. This, however, hinges on whether the information that a frequency filter captures consistently aligns with relevant theory-based business cycle concepts. Whether this is the case is an empirical matter, and herein lies the rationale for our research.</p>
</sec>
<sec id="st3">
<title>Setting</title>
<p>We investigate the informational content of South Africa&#x2019;s output deviation cycles.</p>
</sec>
<sec id="st4">
<title>Methods</title>
<p>We extract deviation cycles at standard high- and medium-frequency ranges (denoted as short- and medium-term deviation cycles respectively) and analyse their informational overlap with the components of an alternative theory-based estimate of the business cycle, decomposed into demand, supply, domestic and foreign sources of business cycle dynamics.</p>
</sec>
<sec id="st5">
<title>Results</title>
<p>Our findings suggest that the contents of deviation cycles extracted over a high-frequency range do not neatly correspond to the transitory &#x2018;demand-driven&#x2019; business cycle, while cycles extracted over a medium-frequency range correspond closely to the combined path of permanent output shocks.</p>
</sec>
<sec id="st6">
<title>Conclusion</title>
<p>One should thus be cautious of drawing strong conclusions about the nature of business cycles from filter-based deviation cycle estimates, particularly if the objective of the study relies on assuming that high-frequency deviation cycles correspond to transitory demand shocks.</p>
</sec>
</abstract>
</article-meta>
</front>
<body>
<sec id="s0001">
<title>Introduction</title>
<p>Empirical business cycle research typically commences with the extraction of a so-called deviation cycle using a time-series smoothing filter. This methodology is appealing for its pragmatism; it is easy to implement, and the output it produces is conveniently interpreted as percentage deviations from the natural level of output. However, recent literature offers staunch criticism of deviation cycle analysis, especially with regard to the assumption implicitly underlying it: that business cycle fluctuations are restricted to distinct intervals on the frequency domain. If permanent shocks are a significant driver of the business cycle (as real business cycle theory suggests), business cycle dynamics may be inextricably linked to the low-frequency permanent component of output, presenting challenges for the core assumption underlying frequency-based business cycle analysis (Canova <xref ref-type="bibr" rid="CIT0008">1998</xref>; Harding &#x0026; Pagan <xref ref-type="bibr" rid="CIT0020">2002</xref>). In short, the core assumption underlying deviation cycle analysis of business cycles may be at odds with economic theory, causing us to doubt its usefulness as a means of studying business cycles.</p>
<p>Despite the lack of a neat alignment between method and theory, the analysis of deviation cycles over particular frequency ranges may still yield useful stylised business cycle facts. This however hinges on whether the information that a frequency filter captures, consistently aligns with relevant theory-based business cycle concepts. Whether this is the case is an empirical matter, and herein lies the rationale for our research. We investigate the informational content of South Africa&#x2019;s output deviation cycles extracted at standard high- and medium-frequency ranges (denoted as short- and medium-term deviation cycles respectively) by comparing them with the components of an alternative theory-based estimate of the business cycle, decomposed into demand, supply, domestic and foreign sources of business cycle dynamics.</p>
<p>Our theory-consistent estimate of the business cycle consists of structural shocks to real output, which we estimate via an open-economy structural vector autoregressive (SVAR) model and identify by imposing long-run restrictions in the style of Blanchard and Quah (<xref ref-type="bibr" rid="CIT0004">1989</xref>). In addition to its strong theoretical coherence, we selected the Blanchard-Quah identification strategy on account of its decomposability, which allows us to isolate the source of business cycle dynamics. Using one such decomposition allows us to differentiate permanent and transitory fluctuations in real output, what real business cycle theorists regard as demand and supply shocks (Plosser <xref ref-type="bibr" rid="CIT0036">1989</xref>). Isolating these sources of fluctuations in real output allows us to test whether short- and medium-term deviation cycles correspond neatly to transitory or permanent components of real output. Similarly, we also use the Blanchard-Quah identification strategy in conjunction with the open-economy specification of our SVAR to decompose real output into domestic and foreign shocks and assess whether either of these aligns more closely with deviation cycles extracted at different frequencies.</p>
<p>Subsequent to obtaining our estimates of the business cycle, the bulk of our analysis centres on simple Pearson correlations between our statistically identified components of the business cycle and our short- and medium-term deviation cycles estimates. While rudimentary, we deem this approach appropriate and sufficiently robust, given that we are comparing information extracted from the same time series. However, we supplement our analysis of the informational content of deviation cycles extracted over medium-range frequencies by testing for cointegration with the decompositions of our benchmark SVAR business cycle estimate. We thereby take advantage of the apparent nonstationarity of our medium-term deviation cycles estimate to determine what information is sufficient to render this time series stationary. Given that cointegration in a univariate setting implies that the two series contain the same underlying stochastic trend (Engle &#x0026; Granger <xref ref-type="bibr" rid="CIT0017">1987</xref>), we regard cointegration between these series as an indication of extensive informational overlap.</p>
</sec>
<sec id="s0002">
<title>Literature</title>
<p>Harding and Pagan (<xref ref-type="bibr" rid="CIT0021">2005</xref>) develop a taxonomy of business cycle concepts that are typical in the applied literature of business cycle analysis, distinguishing between classical, deviation and growth rate cycles. Classical cycles, the original business cycle concept used by Burns and Mitchell (<xref ref-type="bibr" rid="CIT0007">1946</xref>), as well as central banks and research institutes such as the NBER, refers to cycles in the level of the output series. Deviation cycle analysis involves identifying and removing a so-called &#x2018;permanent component&#x2019; from the output series; the remainder is then a set of serially correlated deviations called deviation cycles.<xref ref-type="fn" rid="FN0001"><sup>1</sup></xref> Growth rate cycles, that is, cycles in growth rates, capture periods of accelerating and decelerating growth. These are a special type of deviation cycle, wherein the previous value of output is regarded as the permanent component. Economies experiencing sustained growth do not often exhibit classical cycles (see Mintz <xref ref-type="bibr" rid="CIT0034">1969</xref>) and mainstream business cycle research consequently departs predominantly from the analysis of deviation cycles. For a more thorough discussion of different business cycle concepts see Harding and Pagan (<xref ref-type="bibr" rid="CIT0021">2005</xref>) or see Du Plessis (<xref ref-type="bibr" rid="CIT0013">2006</xref>) for a concise summary.</p>
<p>Deviation cycle analysis is based on the decomposition of a time series into a growth component and a cyclical component. When applying this decomposition to real output data, the cyclical component is regarded as a measurement of the business cycle, and the permanent component is often interpreted as a measure of Lucas&#x2019;s (<xref ref-type="bibr" rid="CIT0033">1977</xref>) concept of potential output. These applications are common in the literature of applied macroeconomics, forming the basis of numerous papers in the South African and international literature. For example, Boshoff and Fourie (<xref ref-type="bibr" rid="CIT0006">2010</xref>) incorporate an analysis of deviation cycles in South African real output as part of their assessment of the relationship between economic activity and trade in the early Cape colony, where they find evidence that deviation cycles in productivity and trade are positively related. Kabundi and Loots (<xref ref-type="bibr" rid="CIT0025">2007</xref>) depart from the extraction of deviation cycles and subsequent estimation of dynamic correlation coefficients in their analysis of co-movement between South African real output and those of the other 13 Southern African development community countries, and similar research has been conducted for South Africa and Germany (Kabundi &#x0026; Loots <xref ref-type="bibr" rid="CIT0026">2010</xref>) and South Africa and the United States of America (U)S (Kabundi <xref ref-type="bibr" rid="CIT0024">2009</xref>). In the international literature, deviation cycles have served as a point of departure for establishing stylised facts about business cycles in developed and developing countries.<xref ref-type="fn" rid="FN0002"><sup>2</sup></xref></p>
<p>The widespread usage of the deviation cycle method makes due consideration of its weaknesses a worthy concern. In this regard, Harding and Pagan (<xref ref-type="bibr" rid="CIT0020">2002</xref>) have raised staunch criticisms of filter-based business cycle analysis. Firstly, they argue that the practice of shifting all information beyond the short-term into a permanent component may be associated with significant loss of information relevant for business cycle research. Their position departs from real business cycle theory, which implies that business cycles should not necessarily be regarded as transitory disturbances to a smooth long-run growth path (Blanchard <xref ref-type="bibr" rid="CIT0003">1997</xref>; Krugman <xref ref-type="bibr" rid="CIT0031">1998</xref>; Sargent <xref ref-type="bibr" rid="CIT0038">1999</xref>; Solow <xref ref-type="bibr" rid="CIT0039">2000</xref>). From this theoretical point of departure, it is arguable that the removal of permanent shocks from real output is at odds with business cycle research, particularly if the aim of that research is to obtain a plausible overall representation of business cycles. However, Harding and Pagan (<xref ref-type="bibr" rid="CIT0020">2002</xref>) also note that removing a filter-estimated trend from real output data does not necessarily remove the permanent shocks to the time series. Thus, even if the researcher&#x2019;s aim is to isolate transitory shocks to real output, frequency filters do not necessarily deliver the desired result. In sum, it might be said that the core contention that underlies Harding and Pagan&#x2019;s (<xref ref-type="bibr" rid="CIT0020">2002</xref>) critique is that deviation cycle analysis unduly circumvents the statistical identification problem that is fundamental to business cycle research, providing convenient estimates of quantities that may not correspond to any theoretical notion of the business cycle.</p>
<p>Despite this identification deficit, deviation cycles may still yield useful stylised facts and insights into business cycle dynamics. Frequency filters are advantageously flexible, allowing researchers to check the robustness of their results by isolating and analysing cyclical variation in real output at various frequency ranges, and recent research based on deviation cycle analysis has used this flexibility to conduct business cycle research that investigates and accounts for the impact of frequency range choices on stylised business cycle facts. For example, Comin and Gertler (<xref ref-type="bibr" rid="CIT0011">2006</xref>) show that the high-frequency characterisation of business cycles provides limited insight into their nature given that economies also exhibit medium-term fluctuations. Comin et al. (<xref ref-type="bibr" rid="CIT0012">2012</xref>) use the same concepts to show that short-term business cycles tend to have large and persistent effects in developing countries, and thus propagate into medium-term fluctuations. This research seems to indicate that an analysis of medium-term deviation cycles may be an appropriate point of departure to understanding of business cycle dynamics and propagation. However, regardless of frequency range choices, research on the dynamics of deviation cycles still departs from an atheoretical basis and thus remains exposed to the Harding and Pagan (<xref ref-type="bibr" rid="CIT0020">2002</xref>) critique: given the purely statistical basis of this methodology, the researcher simply cannot know precisely what information is captured at any choice of frequency ranges.</p>
<p>It is on account of this problem that we provide this evaluation of the informational content of deviation cycles in South African real output. We extract deviation cycles over frequencies conventionally used to capture short- and medium-term business cycle movements and compare them with business cycle estimates obtained from a structural econometric model. As discussed below, our SVAR estimate of the business cycle can be decomposed into transitory and permanent shocks (loosely interpreted as demand and supply shocks) and into domestic and foreign shocks. Comparison with these decompositions of the business cycle allows us to observe the extent to which deviation cycles, extracted at different frequencies correspond to these sources of business cycle fluctuations in South African real output.</p>
</sec>
<sec id="s0003">
<title>Methodology</title>
<p>We use the Christiano and Fitzgerald (<xref ref-type="bibr" rid="CIT0009">2003</xref>) (CF) filter to extract deviation cycles for domestic output. Our choice of filters was informed by research that suggests that the CF filter outperforms others when considering longer-term fluctuations (Zarnowitz &#x0026; Ozyildirim <xref ref-type="bibr" rid="CIT0041">2006</xref>). We define the high-frequency (i.e. short-term) deviation cycle as the component of output corresponding to a frequency range of 6&#x2013;32 quarters. This is the business cycle frequency range used by King and Watson (<xref ref-type="bibr" rid="CIT0030">1995</xref>), King and Rebelo (<xref ref-type="bibr" rid="CIT0029">1999</xref>) and Guay and St-Amant (<xref ref-type="bibr" rid="CIT0019">2005</xref>). Medium-term deviation cycles are extracted for a frequency range of 6&#x2013;200 quarters. The medium-term deviation cycles thus contain both high- and medium-frequency components, where the medium-frequency component ranges from 32 to 200 quarters.</p>
<p>As noted previously, filters are statistical instruments with no basis in economic theory. However, an alternative approach to estimating business cycles that grapples directly with the identification problem is the SVAR identification strategy developed by Blanchard and Quah (<xref ref-type="bibr" rid="CIT0004">1989</xref>). In their influential paper, Blanchard and Quah (<xref ref-type="bibr" rid="CIT0004">1989</xref>) show that it is possible to recover permanent and transitory structural shocks to real output from a two-variable reduced-form VAR by restricting the long-run response of real output to transitory shocks to zero. Consistent with real business cycle theory, one can then represent the contribution of transitory shocks and permanent shocks to the evolution of real output.</p>
<p>Following this work, various authors investigate the sources of business cycles using VAR estimation and the Blanchard-Quah identification strategy, and some have subsequently extended the framework to a greater number of variables, thus increasing the number of distinct structural shocks that may be estimated. For instance, Karras (<xref ref-type="bibr" rid="CIT0027">1993</xref>) estimates such a model for the US, Ahmed and Park (<xref ref-type="bibr" rid="CIT0001">1994</xref>) for a sample of small open economies, Karras (<xref ref-type="bibr" rid="CIT0028">1994</xref>) for various European economies, West (<xref ref-type="bibr" rid="CIT0040">1992</xref>) for Japan and Du Plessis, Smit and Sturzenegger (<xref ref-type="bibr" rid="CIT0015">2008</xref>) for South Africa. In all instances, these authors use the Blanchard-Quah identification strategy to recover permanent and transitory shocks to real output, which they often interpret as aggregate demand shocks (transitory shocks to real output) and supply shocks (permanent shock to real output). They then cumulate the demand or supply shocks to derive a demand- or supply-based estimate of the business cycle. This is precisely the approach we take to obtain a structural estimate of the components driving fluctuations in real output for South Africa.</p>
<p>The study by Du Plessis et al. (<xref ref-type="bibr" rid="CIT0015">2008</xref>) provides the basis for our SVAR-based estimate of the factors underlying the South African business cycle. Their study departs from a three variable SVAR, wherein government expenditure as a percentage of GDP and the real interest rate are used to identify demand shocks to output. We extend the Du Plessis et al. (<xref ref-type="bibr" rid="CIT0015">2008</xref>) study along two dimensions. Firstly, we incorporate data following the sample period set out in their study (2007Q1 &#x2013; 2015Q3), which allows us to observe how output has evolved since the recent financial crisis and subsequent European debt crisis. Secondly, we add two variables to the model that allow us to explicitly model the evolution of South African output in response to global shocks. Given that the Blanchard-Quah decomposition is standard in the literature we provide a cursory description of the identification procedure. See Du Plessis et al. (<xref ref-type="bibr" rid="CIT0015">2008</xref>) or Clarida and Gali (<xref ref-type="bibr" rid="CIT0010">1994</xref>) for a more extensive overview of this procedure for VARs of three or more variables; also see Enders (<xref ref-type="bibr" rid="CIT0016">2010</xref>) for an introduction to VARs, SVARs and the Blanchard-Quah identification strategy for the case of a two-variable VAR.</p>
<p>Variable selection is the first step to achieving identification via the Blanchard-Quah methodology. Following Clarida and Gali (<xref ref-type="bibr" rid="CIT0010">1994</xref>) and Du Plessis et al. (<xref ref-type="bibr" rid="CIT0015">2008</xref>), the domestic components of our model consist of real GDP (<italic>y</italic><sub><italic>t</italic></sub>) along with two sources of demand shocks, namely government expenditure as a percentage of GDP (<italic>g</italic><sub><italic>t</italic></sub>) and the real interest rate (<italic>r</italic><sub><italic>t</italic></sub>). Tests for unit roots in these variables were performed and the results are excluded for brevity (results are available upon request). We find a unit root in all series except for the real interest rate.</p>
<p>The model estimated by Du Plessis et al. (<xref ref-type="bibr" rid="CIT0015">2008</xref>) does not explicitly account for the impact of global shocks and their dynamics in relation to the other (domestic) variables. Given South Africa&#x2019;s small open-economy status, taking into account the effect that global shocks have on the economy seems appropriate. To this end, we augment the model proposed by Du Plessis et al. (<xref ref-type="bibr" rid="CIT0015">2008</xref>). Following Balcilar and Tuna (<xref ref-type="bibr" rid="CIT0002">2009</xref>), we add two additional variables chosen to identify global shocks to the economy: a trade weighted proxy for world output <inline-formula id="ID1"><alternatives><mml:math display="inline" id="I1"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>y</mml:mi><mml:mi>t</mml:mi><mml:mi>f</mml:mi></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i001.tif"/></alternatives></inline-formula> and the rand-denominated real oil price <inline-formula id="ID2"><alternatives><mml:math display="inline" id="I2"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>p</mml:mi><mml:mi>t</mml:mi><mml:mi>f</mml:mi></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i002.tif"/></alternatives></inline-formula>. Augmented Dickey-Fuller (ADF) tests confirm that these variables are difference stationary.</p>
<p>Variable section is important for obtaining a well-specified VAR, but it should be noted that our interest lies in the evolution of the structural shocks underlying these variables and the extent to which they determine the evolution of real output in particular. We are not interested in the causal parameters of these variables as determinants of real output. Additional variables that may constitute further sources of transitory and permanent shocks abound, but we have chosen to limit our specification to these five variables on account of data availability, the precedent set by Du Plessis et al. (<xref ref-type="bibr" rid="CIT0015">2008</xref>), in the case of domestic variables, and that of Balcilar and Tuna (<xref ref-type="bibr" rid="CIT0002">2009</xref>), in the case of external variables.</p>
<p>The next step in following Blanchard and Quah (<xref ref-type="bibr" rid="CIT0004">1989</xref>) is to ensure that our data are stationary. Thus we first-difference <inline-formula id="ID3"><alternatives><mml:math display="inline" id="I3"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>y</mml:mi><mml:mi>t</mml:mi><mml:mi>f</mml:mi></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i003.tif"/></alternatives></inline-formula> and <inline-formula id="ID4"><alternatives><mml:math display="inline" id="I4"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>p</mml:mi><mml:mi>t</mml:mi><mml:mi>f</mml:mi></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i004.tif"/></alternatives></inline-formula>, and we find that they are difference stationary &#x2013; we denote these as <inline-formula id="ID5"><alternatives><mml:math display="inline" id="I5"><mml:mrow><mml:mi>&#x0394;</mml:mi><mml:msub><mml:mi>y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>&#x0394;</mml:mi><mml:msubsup><mml:mi>y</mml:mi><mml:mi>t</mml:mi><mml:mi>f</mml:mi></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i005.tif"/></alternatives></inline-formula> and <inline-formula id="ID6"><alternatives><mml:math display="inline" id="I6"><mml:mrow><mml:mi>&#x0394;</mml:mi><mml:msubsup><mml:mi>p</mml:mi><mml:mi>t</mml:mi><mml:mi>f</mml:mi></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i006.tif"/></alternatives></inline-formula>. While ADF tests indicates that <italic>g</italic><sub><italic>t</italic></sub> is difference stationary, we hold the argument maintained by Du Plessis et al. (<xref ref-type="bibr" rid="CIT0015">2008</xref>), that the ratio of government expenditure to GDP cannot possibly be the product of a unit root process.<xref ref-type="fn" rid="FN0003"><sup>3</sup></xref> Tests of the stability of the VAR did not indicate that including <italic>g</italic><sub><italic>t</italic></sub> in levels destabilises the system.</p>
<p>Our system of equations can be represented as a vector moving-average process of the form <italic>Y</italic><sub><italic>t</italic></sub> = <italic>C</italic>(<italic>L</italic>)<italic>&#x03B5;</italic><sub><italic>t</italic></sub>, where <inline-formula id="ID7"><alternatives><mml:math display="inline" id="I7"><mml:mrow><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msup><mml:mrow><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mi>&#x0394;</mml:mi><mml:msubsup><mml:mi>p</mml:mi><mml:mi>t</mml:mi><mml:mi>f</mml:mi></mml:msubsup><mml:mtext>&#x2003;</mml:mtext><mml:mi>&#x0394;</mml:mi><mml:msubsup><mml:mi>y</mml:mi><mml:mi>t</mml:mi><mml:mi>f</mml:mi></mml:msubsup><mml:mtext>&#x2003;</mml:mtext><mml:mi>&#x0394;</mml:mi><mml:msub><mml:mi>y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mtext>&#x2003;</mml:mtext><mml:msub><mml:mi>g</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mtext>&#x2003;</mml:mtext><mml:msub><mml:mi>r</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow><mml:mo>]</mml:mo></mml:mrow></mml:mrow><mml:mo>&#x2032;</mml:mo></mml:msup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i007.tif"/></alternatives></inline-formula> is our vector of dependent variables, <inline-formula id="ID8"><alternatives><mml:math display="inline" id="I8"><mml:mrow><mml:msub><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msup><mml:mrow><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msubsup><mml:mtext>&#x2003;</mml:mtext><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>y</mml:mi></mml:mrow></mml:msubsup><mml:mtext>&#x2003;</mml:mtext><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>y</mml:mi></mml:msubsup><mml:mtext>&#x2003;</mml:mtext><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>g</mml:mi></mml:msubsup><mml:mtext>&#x2003;</mml:mtext><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>r</mml:mi></mml:msubsup></mml:mrow><mml:mo>]</mml:mo></mml:mrow></mml:mrow><mml:mo>&#x2032;</mml:mo></mml:msup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i008.tif"/></alternatives></inline-formula> our vector of structural shocks.
<disp-formula id="FD1"><alternatives><mml:math display="block" id="M1"><mml:mrow><mml:mi>C</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mtable><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>11</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>12</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>13</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>14</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>15</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>21</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>22</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>23</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>24</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>25</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>31</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>32</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>33</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>34</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>35</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>41</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>42</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>43</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>44</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>45</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>51</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>52</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>53</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>54</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>55</mml:mn></mml:mrow></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>L</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mrow><mml:mo>]</mml:mo></mml:mrow></mml:mrow></mml:math><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-e001.tif"/></alternatives><label>[Eqn 1]</label></disp-formula></p>
<p><italic>C</italic>(<italic>L</italic>) is an infinite order lag polynomial matrix defined as <italic>C</italic>(<italic>L</italic>) = <italic>C</italic><sub>0</sub> + <italic>C</italic><sub>1</sub><italic>L</italic> + <italic>C</italic><sub>2</sub><italic>L</italic><sup>2</sup> + <italic>C</italic><sub>3</sub><italic>L</italic><sup>3</sup> &#x2026; in the lag operator <italic>L</italic>, where each <italic>C</italic><sub><italic>n</italic></sub> for <italic>n</italic> = 0,1,2, is a 5&#x00D7;5 matrix containing the contemporaneous impact of <italic>&#x03B5;</italic><sub><italic>t</italic></sub><sub>&#x2212;</sub><sub><italic>n</italic></sub> on <italic>Y</italic><sub><italic>t</italic></sub>. The matrix <italic>C</italic>(<italic>L</italic>) thus represents the cumulative impact of all preceding structural shocks on the system of variables <italic>Y</italic><sub><italic>t</italic></sub>.</p>
<p>Each of the five structural shocks contained in the vector <italic>&#x03B5;</italic><sub><italic>t</italic></sub> are assumed to be independently, identically distributed and serially uncorrelated. We will refer to these, from left to right, as the oil price shock <inline-formula id="ID9"><alternatives><mml:math display="inline" id="I9"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i009.tif"/></alternatives></inline-formula>, global output shock <inline-formula id="ID10"><alternatives><mml:math display="inline" id="I10"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>y</mml:mi></mml:mrow></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i010.tif"/></alternatives></inline-formula>, domestic output shock <inline-formula id="ID11"><alternatives><mml:math display="inline" id="I11"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>y</mml:mi></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i011.tif"/></alternatives></inline-formula>, government expenditure shock <inline-formula id="ID12"><alternatives><mml:math display="inline" id="I12"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>g</mml:mi></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i012.tif"/></alternatives></inline-formula> and real interest rate shock <inline-formula id="ID13"><alternatives><mml:math display="inline" id="I13"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>r</mml:mi></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i013.tif"/></alternatives></inline-formula>. Despite our naming convention, it is important to note that variation due to these five shocks do not correspond uniquely to any one of these five variables. As discussed in Enders (<xref ref-type="bibr" rid="CIT0016">2010</xref>), this representation assumes that the system of variables is endogenous to five distinct structural shocks. This is made clear by the unrestricted matrix <bold><italic>C</italic></bold>(<italic>L</italic>), which allows each shock contained in <italic>&#x03B5;</italic><sub><italic>t</italic></sub> to impact <italic>Y</italic><sub><italic>t</italic></sub> to an arbitrary extent. Consequently, given the current state of the matrix <italic>C</italic>(<italic>L</italic>) it is not possible to differentiate these shocks from one another, that is, the system <italic>Y</italic><sub><italic>t</italic></sub> = <italic>C</italic>(<italic>L</italic>)<italic>&#x03B5;</italic><sub><italic>t</italic></sub> is an unidentified VAR. However, we can identify the structural shocks in <italic>&#x03B5;</italic><sub><italic>t</italic></sub> by placing a sufficient number of restrictions on <italic>C</italic>(<italic>L</italic>), the required number of restrictions being 10 in this instance (see Enders <xref ref-type="bibr" rid="CIT0016">2010</xref>). This is precisely the crux of the Blanchard-Quah identification strategy, that we can recover structural shocks underlying the progression of a set of endogenous variables <italic>Y</italic><sub><italic>t</italic></sub> via imposing theory-based restrictions on the long-run impact of the shocks <italic>&#x03B5;</italic><sub><italic>t</italic></sub> on the variables <italic>Y</italic><sub><italic>t</italic></sub>.</p>
<p>In addition to standard normalisation assumptions on <italic>&#x03B5;</italic><sub><italic>t</italic></sub>, the remaining assumptions required to achieve identification are a set of restrictions on <italic>C</italic>(<italic>L</italic>) However, because we have assumed that the shocks in <italic>&#x03B5;</italic><sub><italic>t</italic></sub> are independent and serially uncorrelated, we can identify <italic>&#x03B5;</italic><sub><italic>t</italic></sub> by imposing restrictions on the matrix:
<disp-formula id="FD2"><alternatives><mml:math display="block" id="M2"><mml:mrow><mml:mi>C</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mtable><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>11</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>12</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>13</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>14</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>15</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>21</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>22</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>23</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>24</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>25</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>31</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>32</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>33</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>34</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>35</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>41</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>42</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>43</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>44</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>45</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>51</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>52</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>53</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>54</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>55</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mrow><mml:mo>]</mml:mo></mml:mrow></mml:mrow></mml:math><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-e002.tif"/></alternatives><label>[Eqn 2]</label></disp-formula></p>
<p>This we obtained by setting <italic>L</italic> = 1. The matrix <italic>C</italic>(1) represents the cumulative impulse response of the vector <italic>Y</italic><sub><italic>t</italic></sub> to a single pulse of all five elements of <italic>&#x03B5;</italic><sub><italic>t</italic></sub>. In its current state, the matrix <italic>C</italic>(1) would allow for any of our five structural shocks to have a permanent effect on any one of the five variables in our VAR. However, if we are willing to assume that our unobserved structural shocks do not permanently affect a sufficient number of variables in our model (i.e. if we assume that a sufficient number of elements in <italic>C</italic>[1] are in fact zero) then we can recover each of the distinct shocks in <italic>&#x03B5;</italic><sub><italic>t</italic></sub>.</p>
<p>Following Balcilar and Tuna (<xref ref-type="bibr" rid="CIT0002">2009</xref>), we thus achieve identification by imposing the following 10 restrictions on the matrix <italic>C</italic>(1). Firstly, we assume that permanent shocks to world output <inline-formula id="ID14"><alternatives><mml:math display="inline" id="I14"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>y</mml:mi></mml:mrow></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i014.tif"/></alternatives></inline-formula> do not affect the real price of oil in the long run. This implies that <italic>C</italic><sub>12</sub> = 0. Next, the assumption that South Africa is a small open-economy implies that domestic shocks to domestic variables have no long-run impact on foreign variables, and as such that <italic>C</italic><sub>13</sub> = <italic>C</italic><sub>14</sub> = <italic>C</italic><sub>15</sub> = <italic>C</italic><sub>23</sub> = <italic>C</italic><sub>24</sub> = <italic>C</italic><sub>25</sub> = 0. Lastly, we assume that monetary shocks <inline-formula id="ID15"><alternatives><mml:math display="inline" id="I15"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>r</mml:mi></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i015.tif"/></alternatives></inline-formula> do not have a long-run impact on government expenditure and domestic output, and that shocks to government expenditure <inline-formula id="ID16"><alternatives><mml:math display="inline" id="I16"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>g</mml:mi></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i016.tif"/></alternatives></inline-formula> do not have a long-run effect on domestic output, implying that <italic>C</italic><sub>34</sub> = <italic>C</italic><sub>35</sub> = <italic>C</italic><sub>45</sub> = 0. Incorporating the above on the matrix <italic>C</italic>(1) gives the identified long-run impact of the shocks on the endogenous variables:
<disp-formula id="FD3"><alternatives><mml:math display="block" id="M3"><mml:mrow><mml:mi>C</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mtable><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>11</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mn>0</mml:mn></mml:mtd><mml:mtd><mml:mn>0</mml:mn></mml:mtd><mml:mtd><mml:mn>0</mml:mn></mml:mtd><mml:mtd><mml:mn>0</mml:mn></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>21</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>22</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mn>0</mml:mn></mml:mtd><mml:mtd><mml:mn>0</mml:mn></mml:mtd><mml:mtd><mml:mn>0</mml:mn></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>31</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>32</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>33</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mn>0</mml:mn></mml:mtd><mml:mtd><mml:mn>0</mml:mn></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>41</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>42</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>43</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>44</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mn>0</mml:mn></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>51</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>52</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>53</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>54</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mn>55</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mrow><mml:mo>]</mml:mo></mml:mrow></mml:mrow></mml:math><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-e003.tif"/></alternatives><label>[Eqn 3]</label></disp-formula></p>
<p>From these assumptions we have a sufficient number of restrictions to estimate the matrix <italic>C</italic>(1) and hence to identify the shocks in <italic>&#x03B5;</italic><sub><italic>t</italic></sub>. For the sake of brevity, we do not discuss the process of obtaining <italic>&#x03B5;</italic><sub><italic>t</italic></sub> in detail here, as the process of moving from restrictions on <italic>C</italic>(1) to estimates of <italic>&#x03B5;</italic><sub><italic>t</italic></sub> is a matter of mere computation now that we have restricted <italic>C</italic>(1) to a lower-triangle matrix. (Clarida and Gali, <xref ref-type="bibr" rid="CIT0010">1994</xref>, provide a step-by-step guide to this process.) However, for completeness sake we note succinctly that as under our 10 identifying assumptions the matrix <bold><italic>C</italic></bold>(1) may be obtained as the lower-triangle Cholesky decomposition <italic>C</italic>(1) <italic>C</italic>(1)&#x2019; = <italic>R</italic>(1) <bold>&#x03A3;</bold><italic>R</italic>(1)&#x2019;, where <bold>&#x03A3;</bold> and <italic>R</italic>(1) are respectively the variance-covariance matrix and cumulative impulse response matrix of an unidentified VAR of the form <italic>Y</italic><sub><italic>t</italic></sub> = <italic>R</italic>(<italic>L</italic>)<italic>u</italic><sub><italic>t</italic></sub>, and where <italic>u</italic><sub><italic>t</italic></sub> is its vector of reduced-form disturbances. Once we have estimated <italic>Y</italic><sub><italic>t</italic></sub> = <italic>R</italic>(<italic>L</italic>)<italic>u</italic><sub><italic>t</italic></sub>, we can write <inline-formula id="ID17"><alternatives><mml:math display="inline" id="I17"><mml:mrow><mml:msub><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msup><mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>R</mml:mi><mml:msup><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msup><mml:mi>C</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msup><mml:msub><mml:mi>u</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i017.tif"/></alternatives></inline-formula>, thus identifying <italic>&#x03B5;</italic><sub><italic>t</italic></sub> (Clarida and Gali <xref ref-type="bibr" rid="CIT0010">1994</xref>).</p>
<p>With <italic>&#x03B5;</italic><sub><italic>t</italic></sub> identified we can assess the informational content of deviation cycles extracted at different frequency ranges. We compare the content of deviation cycles with a range of combinations of structural shocks, with particular emphasis on the path of transitory shocks, that is, the demand-based business cycle as defined in Du Plessis et al. (<xref ref-type="bibr" rid="CIT0015">2008</xref>) (<inline-formula id="ID18"><alternatives><mml:math display="inline" id="I18"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>g</mml:mi></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i018.tif"/></alternatives></inline-formula> and <inline-formula id="ID19"><alternatives><mml:math display="inline" id="I19"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>r</mml:mi></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i019.tif"/></alternatives></inline-formula>), the path of aggregate supply disturbances, which we define as the combination of all permanent shocks to <italic>y</italic><sub><italic>t</italic></sub> (<inline-formula id="ID20"><alternatives><mml:math display="inline" id="I20"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>y</mml:mi></mml:mrow></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i020.tif"/></alternatives></inline-formula> and <inline-formula id="ID21"><alternatives><mml:math display="inline" id="I21"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>y</mml:mi></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i021.tif"/></alternatives></inline-formula>), the combined path of domestic shocks, both transitory and permanent (<inline-formula id="ID22"><alternatives><mml:math display="inline" id="I22"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>y</mml:mi></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>g</mml:mi></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i022.tif"/></alternatives></inline-formula> and <inline-formula id="ID23"><alternatives><mml:math display="inline" id="I23"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>r</mml:mi></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i023.tif"/></alternatives></inline-formula>), and the path of global shocks to output <inline-formula id="ID24"><alternatives><mml:math display="inline" id="I24"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i024.tif"/></alternatives></inline-formula> and <inline-formula id="ID25"><alternatives><mml:math display="inline" id="I25"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>y</mml:mi></mml:mrow></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i025.tif"/></alternatives></inline-formula>.</p>
<p>As a final note on our methodology, we acknowledge that the results of our analysis rest on whether or not the Blanchard-Quah identifying assumptions hold for our five variable VAR. With respect to the assumptions of spherical and serially uncorrelated error terms, we can (and do) test this, but we unfortunately cannot test whether our restrictions on the long-run impact matrix are valid. Our analysis also relies on the general efficacy of the Blanchard-Quah identification strategy. Lippi and Reichlin (<xref ref-type="bibr" rid="CIT0032">1993</xref>) show, for instance, that several nonstandard moving-average representations produce results quite different from those obtained by Blanchard and Quah (<xref ref-type="bibr" rid="CIT0004">1989</xref>) in their original application of the strategy. Even so, it must be remembered that the business cycle is an unobserved theoretical construct, and hence quantifying it necessarily requires some assumptions about the process underlying it. In the case of frequency filters, the implicit identifying assumption seems to be that the business cycle is in all instances restricted to a subset of the frequency domain, and this is clearly far removed from explicit economic reasoning. In contrast, the Blanchard-Quah identification strategy provides a set of explicit and economically sensible assumptions that produce an estimate of the business cycle. Notwithstanding the inevitability that the Blanchard-Quah identifying assumptions may not hold, the business cycle estimates it produces follow from a sensible application of economic theory. Hence, we propose that in the absence of any objective alternative measure of the business cycle, our method of assessing the informational content of filter-based deviation cycles provides an important step in the direction of becoming critically aware of the limitations of deviation cycle analysis and filter-based business cycle estimation broadly.</p>
</sec>
<sec id="s0004">
<title>Data</title>
<p>We estimate deviation cycles and SVAR-based structural shocks to real output on a sample period from 1961Q2 until 2015Q3, chosen on the basis of data availability. We define real output, our variable of interest, as real GDP measured at a quarterly frequency. Quarterly data for South African real output and government expenditure and monthly data for the repo rate were obtained from the South African Reserve Bank (SARB <xref ref-type="bibr" rid="CIT0037">2016</xref>).</p>
<p>Quarterly real output for the US, the United Kingdom (UK), Australia and Japan (all obtained from the International Monetary Fund&#x2019;s International Financial Statistics Database, <xref ref-type="bibr" rid="CIT0022">2016</xref>) and Europe (obtained from the Organisation for Economic Co-operation and Development&#x2019;s OECD.stat database, <xref ref-type="bibr" rid="CIT0035">2016</xref>) were averaged to construct a proxy for global output. This selection was informed by the variables used by Boshoff (<xref ref-type="bibr" rid="CIT0005">2010</xref>), updated to include Japan on account of its importance as major trading partner to South Africa. Note that China was initially considered as an additional economy to be included in our measure of global output but was omitted due to the limited availability of data detailing real output in China prior to the mid-1970s.</p>
<p>Monthly and quarterly South African consumer price index (CPI) and the quarterly series of the West Texas Intermediate (WTI) spot oil price and the rand-dollar exchange rate (used to convert the spot oil price to rand) were obtained from Quantec&#x2019;s EasyData database. We calculate the quarterly real interest rate from monthly data using the &#x2018;within-quarter&#x2019; formula from Du Plessis, Smit and Sturzenegger (<xref ref-type="bibr" rid="CIT0014">2007</xref>). The WTI spot oil price was first converted to nominal rand, then to real rand using the quarterly CPI. All data are seasonally adjusted with 2010 as the base year.</p>
<p>In the final specification of our SVAR, the real rand-denominated oil price, our proxy for global output and domestic real output, are specified in log-differences; the ratio of government expenditure to GDP and the real interest rate are included in levels.</p>
</sec>
<sec id="s0005">
<title>Estimation and results</title>
<p>We apply the CF filter to the log of South African real GDP data. The results are reported in <xref ref-type="fig" rid="F0001">Figure 1</xref>, which shows both the high- and medium-frequency deviation cycles along with the medium-term component. Recall that our high-frequency deviation cycles are the variations in real output within the frequency range of 6&#x2013;32 quarters, and that the medium-term deviation cycle encompasses both the high-frequency and medium-frequency component, that is, it encompasses the frequency range of 6&#x2013;200 quarters. As such, the difference between the medium-term cycles and the medium-frequency component (i.e. the variation in real output in the frequency range from 32 to 200 quarters) gives the high-frequency deviation cycles. Values are expressed as a percentage of the low-frequency component. The shaded area indicates the period following the financial crisis.</p>
<fig id="F0001">
<label>FIGURE 1</label>
<caption><p>Short- and medium-term deviation cycles.</p></caption>
<graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-g001.tif"/>
</fig>
<p>Several features of <xref ref-type="fig" rid="F0001">Figure 1</xref> are worth noting. The medium-frequency component is clearly characterised by a larger amplitude across the entire sample period. Following Giannone and Reichlin (<xref ref-type="bibr" rid="CIT0018">2005</xref>), we interpret this as an indication that short- and medium-frequency components of South Africa&#x2019;s business cycle contain distinct information. Historically, the medium-term deviation cycle reaches a local minimum during the time that South Africa underwent its democratic transition and started to recover thereafter. This feature is consistent with Boshoff (<xref ref-type="bibr" rid="CIT0005">2010</xref>), who finds that the medium-term deviation cycle starts declining relative to the low-frequency component in the early 1980s and falls below the low-frequency component in the late 1980s. Boshoff (<xref ref-type="bibr" rid="CIT0005">2010</xref>) attributes this marked decline to the political unrest, economic sanctions and subsequent debt standstill that characterised South Africa in the 1980s. Note that the cycle only moved above its permanent component recently, since 2005. Similar to Boshoff (<xref ref-type="bibr" rid="CIT0005">2010</xref>), we find that since about 2002 the short-term deviation cycle is smaller in comparison with the medium-frequency component, a finding which he ascertains implies that &#x2018;strong output growth since 2003 could be ascribed to a longer-term momentum, rather than short-term spikes&#x2019;. However, since the onset of the crisis, the short-term deviation cycle again increases relative to the medium-frequency component, in line with the recent sluggish and volatile output growth discussed previously.</p>
<p>For our theoretical benchmark, we estimate the SVAR described above at six lags. We conducted standard specification tests for normality and autocorrelation on the unrestricted VAR (the results have been omitted for brevity and are available upon request). Tests for autocorrelation were deemed passable, but it should also be noted that the unrestricted VAR did not pass tests for the joint normality of the residuals. This result seemed to follow primarily from world output, whose residual series is platykurtic on account of the great recession. Adding additional lags did not correct this misspecification. We do not attempt to correct for this finding by including outlier dummy variables, as this would unduly reduce the information contained in the residual series (and hence in our estimates of the vector of structural shocks). Furthermore, we maintain that non-normality is not so problematic in this context. While the assumption that the residuals are uncorrelated is necessary for the structural decomposition of the estimated residuals into structural shocks (Clarida &#x0026; Gali <xref ref-type="bibr" rid="CIT0010">1994</xref>), the assumption of spherical residuals is only necessary for statistical inference with ordinary least squares. We thus proceed, noting that inference on the coefficients of our model is biased.</p>
<p><xref ref-type="table" rid="T0001">Table 1</xref> provides a first look at the extent of the informational overlap between combinations of structural shocks to output and deviation cycles at different frequency ranges. We also check for correlation between the medium-term deviation cycle and structural shocks in differences, on account of the apparent nonstationarity of these series. Of course, filtered data is mean-reverting by design, but we investigate the extent of the relationship between changes in these series so as to check the robustness of our result in levels. Correlation between cycles and structural shocks is positive for all but the shock to the real interest rate, <inline-formula id="ID26"><alternatives><mml:math display="inline" id="I26"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>r</mml:mi></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i026.tif"/></alternatives></inline-formula>. The positive contemporaneous correlation with the shock real price of crude oil, found for all three series, is a counterintuitive result. However, as was mentioned in our discussion of the Blanchard-Quah methodology, it must be remembered that <inline-formula id="ID27"><alternatives><mml:math display="inline" id="I27"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i027.tif"/></alternatives></inline-formula> cannot strictly be interpreted as oil price shocks; <inline-formula id="ID28"><alternatives><mml:math display="inline" id="I28"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i028.tif"/></alternatives></inline-formula> is the series of shocks that has a permanent effect on the price of oil after factoring out the systematic relationship between the oil price and the other variables included in our SVAR model. Presumably, this series will contain shocks underlying variations in commodity prices more generally, where we might anticipate that positive shocks to commodity prices will be positively related to domestic real output. All other positive correlations are consistent with our intuition.</p>
<table-wrap id="T0001">
<label>TABLE 1</label>
<caption><p>Pearson correlation coefficients for shocks and deviation cycles.</p></caption>
<table frame="hsides" rules="groups">
<thead valign="top">
<tr>
<th align="left" rowspan="2">Cumulative shocks</th>
<th align="center" colspan="3">Deviation cycles</th>
</tr>
<tr>
<th align="center">Short-term</th>
<th align="center">Medium-term</th>
<th align="center">Medium-term (first differences)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">Real interest rate shocks <inline-formula id="ID29"><alternatives><mml:math display="inline" id="I29"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mtext>t</mml:mtext><mml:mtext>r</mml:mtext></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i029.tif"/></alternatives></inline-formula></td>
<td align="left">&#x2212;0.1942<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="left">&#x2212;0.1091</td>
<td align="left">&#x2212;0.0311</td>
</tr>
<tr>
<td align="left">Government expenditure shocks <inline-formula id="ID30"><alternatives><mml:math display="inline" id="I30"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mtext>t</mml:mtext><mml:mtext>g</mml:mtext></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i030.tif"/></alternatives></inline-formula></td>
<td align="left">0.0616</td>
<td align="left">0.1848<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="left">0.1291<xref ref-type="table-fn" rid="TFN0001">&#x002A;</xref></td>
</tr>
<tr>
<td align="left">Domestic output shocks <inline-formula id="ID31"><alternatives><mml:math display="inline" id="I31"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mtext>t</mml:mtext><mml:mtext>y</mml:mtext></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i031.tif"/></alternatives></inline-formula></td>
<td align="left">0.1109</td>
<td align="left">0.6137<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="left">0.3166<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
</tr>
<tr>
<td align="left">Global output shocks <inline-formula id="ID32"><alternatives><mml:math display="inline" id="I32"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mtext>t</mml:mtext><mml:mrow><mml:mtext>fy</mml:mtext></mml:mrow></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i032.tif"/></alternatives></inline-formula></td>
<td align="left">0.0619</td>
<td align="left">0.1591<xref ref-type="table-fn" rid="TFN0002">&#x002A;&#x002A;</xref></td>
<td align="left">0.0842</td>
</tr>
<tr>
<td align="left">Oil price shocks <inline-formula id="ID33"><alternatives><mml:math display="inline" id="I33"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mtext>t</mml:mtext><mml:mrow><mml:mtext>fp</mml:mtext></mml:mrow></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i033.tif"/></alternatives></inline-formula></td>
<td align="left">0.214<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="left">0.3842<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="left">0.2751<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
</tr>
<tr>
<td align="left">Domestic shocks</td>
<td align="left">0.1167<xref ref-type="table-fn" rid="TFN0001">&#x002A;</xref></td>
<td align="left">0.6534<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="left">0.3349<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
</tr>
<tr>
<td align="left">External shocks</td>
<td align="left">0.222<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="left">0.4069<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="left">0.2845<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
</tr>
<tr>
<td align="left">Transitory shocks</td>
<td align="left">0.0196</td>
<td align="left">0.166<xref ref-type="table-fn" rid="TFN0002">&#x002A;&#x002A;</xref></td>
<td align="left">0.1174<xref ref-type="table-fn" rid="TFN0001">&#x002A;</xref></td>
</tr>
<tr>
<td align="left">Permanent shocks</td>
<td align="left">0.1998<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="left">0.7244<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="left">0.4251<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
</tr>
<tr>
<td align="left">All five pure shocks</td>
<td align="left">0.2086<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="left">0.7672<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="left">0.4385<xref ref-type="table-fn" rid="TFN0003">&#x002A;&#x002A;&#x002A;</xref></td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn><p>Note: This table contains estimates of Pearson correlation coefficients for the variables mentioned. All calculations were obtained using R.</p></fn>
<fn id="TFN0001"><label>&#x002A;</label><p>, Statistical significance at 10&#x0025;;</p></fn>
<fn id="TFN0002"><label>&#x002A;&#x002A;</label><p>, Statistical significance at 5&#x0025;;</p></fn>
<fn id="TFN0003"><label>&#x002A;&#x002A;&#x002A;</label><p>, Statistical significance at 1&#x0025;.</p></fn>
</table-wrap-foot>
</table-wrap>
<p>With reference to short-term deviation cycles, we find that there is substantial correlation with the negative demand shocks that correspond to the real interest rate <inline-formula id="ID34"><alternatives><mml:math display="inline" id="I34"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>r</mml:mi></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i034.tif"/></alternatives></inline-formula>. The pure demand shock underlying government expenditure <inline-formula id="ID35"><alternatives><mml:math display="inline" id="I35"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>g</mml:mi></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i035.tif"/></alternatives></inline-formula> exhibits a positive correlation with the short-term cycles but is the least correlated with short-term cycles of all of the pure shocks (the correlation coefficient is also statistically insignificant). Interestingly, the combined path of these transitory shocks produces the smallest correlation coefficient of all the combinations we consider, seemingly indicative of some degree of countercyclicality between these demand shocks. This result can also be observed in <xref ref-type="fig" rid="F0002">Figure 2a</xref>, which shows that the combined path of transitory shocks is characterised by low variance relative to that of the short-term deviation cycles.</p>
<fig id="F0002">
<label>FIGURE 2</label>
<caption><p>Structural shocks and short-term deviation cycles: (a) medium-term deviation cycles and transitory shocks; (b) medium-term deviation cycles and permanent shocks; (c) Medium-term deviation cycles and domestic shocks; (d) medium-term deviation cycles and external shocks.</p></caption>
<graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-g002.tif"/>
</fig>
<p>In contrast with these results, it is interesting to note the correlation coefficient corresponding to <inline-formula id="ID36"><alternatives><mml:math display="inline" id="I36"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i036.tif"/></alternatives></inline-formula>. While the other permanent shocks (<inline-formula id="ID37"><alternatives><mml:math display="inline" id="I37"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>y</mml:mi></mml:mrow></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i037.tif"/></alternatives></inline-formula> and <inline-formula id="ID38"><alternatives><mml:math display="inline" id="I38"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>y</mml:mi></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i038.tif"/></alternatives></inline-formula>) show no significant correlation with the short-term deviation cycle, the oil price shock <inline-formula id="ID39"><alternatives><mml:math display="inline" id="I39"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i039.tif"/></alternatives></inline-formula> is the pure shock with the single highest correlation with the series of short-term deviation cycles. The correlation coefficient on <inline-formula id="ID40"><alternatives><mml:math display="inline" id="I40"><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msubsup><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i040.tif"/></alternatives></inline-formula> of 0.214 even exceeds the correlation associated with the combination of all permanent shocks (<inline-formula id="ID41"><alternatives><mml:math display="inline" id="I41"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>y</mml:mi></mml:mrow></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i041.tif"/></alternatives></inline-formula> and <inline-formula id="ID42"><alternatives><mml:math display="inline" id="I42"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>y</mml:mi></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i042.tif"/></alternatives></inline-formula>) as well as the correlation with all five shocks. Only the correlation coefficient of 0.222 associated with the combination of external shocks (<inline-formula id="ID43"><alternatives><mml:math display="inline" id="I43"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i043.tif"/></alternatives></inline-formula> and <inline-formula id="ID44"><alternatives><mml:math display="inline" id="I44"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>y</mml:mi></mml:mrow></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i044.tif"/></alternatives></inline-formula>) exceeds the coefficient associated with <inline-formula id="ID45"><alternatives><mml:math display="inline" id="I45"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i045.tif"/></alternatives></inline-formula> (a result that in any case appears to be primarily driven by the correlation with <inline-formula id="ID46"><alternatives><mml:math display="inline" id="I46"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mi>f</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i046.tif"/></alternatives></inline-formula>). Observing the patterns in <xref ref-type="fig" rid="F0002">Figures 2b</xref> and <xref ref-type="fig" rid="F0002">2d</xref>, it is apparent that the series of permanent and external shocks appear to align closely with the short-term deviation cycle turning points. In contrast, the combined path of domestic shocks (<xref ref-type="fig" rid="F0002">Figure 2c</xref>) exhibits cycles that occur over longer periods than those of the short-term deviation cycles.</p>
<p>In sum, the two factors most strongly related to short-term deviation cycles are transitory shocks associated with the real interest rate and permanent shocks associated with real oil prices. Short-term deviation cycles, frequently interpreted as transitory demand shocks, do not appear to be strongly related with the combined path of (domestic) transitory shocks. We regard these findings as cursory evidence corroborating the critique of Harding and Pagan (<xref ref-type="bibr" rid="CIT0020">2002</xref>), illustrating that high-frequency deviation cycles in South African output do not neatly correspond to transitory shocks.</p>
<p>Turning now to observations regarding medium-term cycles, permanent shocks (with a correlation of 0.7244) account for a far greater proportion of deviation cycle variation at this frequency than do transitory shocks (0.166). The varying extents of overlap between medium-term cycles and transitory and permanent shocks is evident in <xref ref-type="fig" rid="F0003">Figures 3a</xref> and <xref ref-type="fig" rid="F0003">3b</xref>. Note that while the combined path of all five structural shocks exhibits the highest overall correlation (0.7672) with the medium-term cycles, it is only marginally more correlated than the combined path of all permanent structural shocks (which shows a correlation coefficient of 0.7244).</p>
<fig id="F0003">
<label>FIGURE 3</label>
<caption><p>Structural shocks and medium-term deviation cycles: (a) ; (b) ; (c) ; (d)</p></caption>
<graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-g003.tif"/>
</fig>
<p>It is particularly interesting to note that the combination of transitory shocks is more strongly correlated with medium-term cycles than with short-term cycles. In fact, barring the correlation reported for the real interest rate, it seems that the cycles and shocks are more strongly related in the medium term for all of the reported combinations of structural shocks &#x2013; this observation is robust, holding for the correlations reported for both the levels and differences of these series. Tentatively, we regard the finding that the combined path of transitory shocks is more strongly correlated with medium-term cycles than with short-term as a corroboration of the notion that medium-term deviation cycles are less prone to discarding relevant business cycle information.</p>
<p>Considered along the domestic-external dichotomy, we find that the combined path of domestic shocks to output has a reportedly higher correlation with medium-term cycles than do external shocks &#x2013; these series are depicted in <xref ref-type="fig" rid="F0003">Figures 3c</xref> and <xref ref-type="fig" rid="F0003">3d</xref>. Referring again to <xref ref-type="table" rid="T0001">Table 1</xref>, these findings contrasts with what we observe for short-term cycles, which are reportedly more strongly correlated with external shocks than with domestic shocks. This result appears to be primarily driven by correlation with the permanent domestic shock <inline-formula id="ID47"><alternatives><mml:math display="inline" id="I47"><mml:mrow><mml:msubsup><mml:mi>&#x03B5;</mml:mi><mml:mi>t</mml:mi><mml:mi>y</mml:mi></mml:msubsup></mml:mrow></mml:math><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="SAJEMS-21-1689-i047.tif"/></alternatives></inline-formula>. This is an intuitive result, indicating that what would often be interpreted as domestic supply (permanent) shocks account for the majority of the medium-term variation in domestic output.</p>
<p>In order to further investigate the overlap between medium-term cycles and different combinations of structural shocks, we test for cointegration between these series. We test the stationarity of the medium-term cycles and find them to be difference stationary. Thus, if a regression of these cycles on a series of structural shocks yields stationary residuals, this might be regarded as an indication that the cycles capture the same stochastic trend as the shocks. For these tests, we capture the medium-term component of the business cycle by simply removing the long-term component &#x2013; that is, we use the information captured in the frequency range 1&#x2013;200 quarters. This leads to better behaved specification tests than for results obtained using medium-term cycles as defined earlier but does not change the conclusions we draw from our tests for cointegration.</p>
<p><xref ref-type="table" rid="T0002">Table 2</xref> presents specification tests and tests for cointegration for the medium-term cycles and 10 different combinations of structural shocks to domestic output. Following the Johansen (<xref ref-type="bibr" rid="CIT0023">1988</xref>) procedure, we first test for stationarity among the combinations of structural shocks; we find that none of these series is stationary at any traditional level of significance. We then estimate an unrestricted VAR for the cycles and each one of the combinations of structural shocks in levels. Each VAR was run with a lag length selected by the Akaike information criterion (AIC). Specification tests reported in <xref ref-type="table" rid="T0002">Table 2</xref> indicate that the only VAR that passes the Jarque-Bera (J-B) test for joint normality at the 5&#x0025; level is the VAR containing the combined path of permanent shocks to real output. However, even the combined path of permanent shocks to output fails the joint test for normality with regard to kurtosis at the 5&#x0025; level. For completeness sake, in <xref ref-type="table" rid="T0002">Table 2</xref> we show that four of the VARs that fail the J-B test at the 1&#x0025; level yield Johansen test results indicative of cointegration at the 5&#x0025; level, and that the Johansen tests on the VARs estimated on the combined path of permanent shocks and on the combined path of all shocks indicate the presence of a cointegrating vector at the 1&#x0025; level of significance. However, the J-B test results cast doubt on one of the key assumptions necessary for the validity of the maximum-likelihood-based Johansen test.</p>
<table-wrap id="T0002">
<label>TABLE 2</label>
<caption><p>Pretests and test for cointegration.</p></caption>
<table frame="hsides" rules="groups">
<thead valign="top">
<tr>
<th align="left" rowspan="2">Cumulative shocks</th>
<th align="center" rowspan="2">ADF <italic>p</italic>-values: Shocks</th>
<th align="center" colspan="3">Joint normality tests (VAR in levels)</th>
<th align="center" colspan="2">Cointegrating vectors (<italic>r</italic>)</th>
<th align="center" colspan="2">ADF <italic>p</italic>-values: OLS residuals</th>
</tr>
<tr>
<th align="center">J-B test</th>
<th align="center">Skewness</th>
<th align="center">Kurtosis</th>
<th align="center"><italic>r</italic> = 0</th>
<th align="center"><italic>r</italic> &#x00C4; 1</th>
<th align="center">Shock</th>
<th align="center">Cycles</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">Real interest rate shocks ()</td>
<td align="left">0.379</td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center">-</td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
</tr>
<tr>
<td align="left">Government expenditure shocks ()</td>
<td align="left">0.411</td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
</tr>
<tr>
<td align="left">Domestic output shocks ()</td>
<td align="left">0.981</td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
</tr>
<tr>
<td align="left">Global output shocks ()</td>
<td align="left">0.615</td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center">-</td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
</tr>
<tr>
<td align="left">Oil price shocks ()</td>
<td align="left">0.391</td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
</tr>
<tr>
<td align="left">Domestic shocks</td>
<td align="left">0.95</td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
</tr>
<tr>
<td align="left">External shocks</td>
<td align="left">0.363</td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
</tr>
<tr>
<td align="left">Transitory shocks</td>
<td align="left">0.408</td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center"><xref ref-type="table-fn" rid="TFN0005">&#x002A;&#x002A;</xref></td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
</tr>
<tr>
<td align="left">Permanent shocks</td>
<td align="left">0.898</td>
<td align="center"><xref ref-type="table-fn" rid="TFN0004">&#x002A;</xref></td>
<td align="center">-</td>
<td align="center"><xref ref-type="table-fn" rid="TFN0005">&#x002A;&#x002A;</xref></td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
</tr>
<tr>
<td align="left">All five pure shocks</td>
<td align="left">0.831</td>
<td align="center"><xref ref-type="table-fn" rid="TFN0005">&#x002A;&#x002A;</xref></td>
<td align="center">-</td>
<td align="center"><xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
</tr>
<tr>
<td align="left">Real interest rate shocks ()</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="left">14.837</td>
<td align="left">6.885</td>
<td align="left">0.373</td>
<td align="left">0.667</td>
</tr>
<tr>
<td align="left">Government expenditure shocks ()</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="left">20.83<xref ref-type="table-fn" rid="TFN0005">&#x002A;&#x002A;</xref></td>
<td align="left">1.131</td>
<td align="left">0.601</td>
<td align="left">0.839</td>
</tr>
<tr>
<td align="left">Domestic output shocks ()</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="left">21.831<xref ref-type="table-fn" rid="TFN0005">&#x002A;&#x002A;</xref></td>
<td align="left">1.611</td>
<td align="left">0.81</td>
<td align="left">0.385</td>
</tr>
<tr>
<td align="left">Global output shocks ()</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="left">24.536<xref ref-type="table-fn" rid="TFN0005">&#x002A;&#x002A;</xref></td>
<td align="left">6.977</td>
<td align="left">0.609</td>
<td align="left">0.706</td>
</tr>
<tr>
<td align="left">Oil price shocks ()</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="left">22.109<xref ref-type="table-fn" rid="TFN0005">&#x002A;&#x002A;</xref></td>
<td align="left">5.026</td>
<td align="left">0.224</td>
<td align="left">0.466</td>
</tr>
<tr>
<td align="left">Domestic shocks</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="left">18.861<xref ref-type="table-fn" rid="TFN0004">&#x002A;</xref></td>
<td align="left">1.918</td>
<td align="left">0.678</td>
<td align="left">0.424</td>
</tr>
<tr>
<td align="left">External shocks</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="left">18.027<xref ref-type="table-fn" rid="TFN0004">&#x002A;</xref></td>
<td align="left">4.536</td>
<td align="left">0.165</td>
<td align="left">0.457</td>
</tr>
<tr>
<td align="left">Transitory shocks</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="left">21.553<xref ref-type="table-fn" rid="TFN0005">&#x002A;&#x002A;</xref></td>
<td align="left">1.234</td>
<td align="left">0.588</td>
<td align="left">0.83</td>
</tr>
<tr>
<td align="left">Permanent shocks</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="left">45.01<xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="left">3.36</td>
<td align="left">0.114</td>
<td align="left">0.035<xref ref-type="table-fn" rid="TFN0005">&#x002A;&#x002A;</xref></td>
</tr>
<tr>
<td align="left">All five pure shocks</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="center">-</td>
<td align="left">41.977<xref ref-type="table-fn" rid="TFN0006">&#x002A;&#x002A;&#x002A;</xref></td>
<td align="left">3.775</td>
<td align="left">0.086<xref ref-type="table-fn" rid="TFN0004">&#x002A;</xref></td>
<td align="left">0.027<xref ref-type="table-fn" rid="TFN0005">&#x002A;&#x002A;</xref></td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn><p>Note: In addition to <italic>p</italic>-values obtained from ADF tests on each variable, this table contains figures relevant to the Johansen (<xref ref-type="bibr" rid="CIT0023">1988</xref>) and Engle and Granger (<xref ref-type="bibr" rid="CIT0017">1987</xref>) tests for cointegration. As per the Johansen methodology, tests for joint normality were obtained from a VAR of the variation in real output that is less than the medium-frequency threshold of 200 quarters and the corresponding variable as indicated. A rejection of the null hypothesis indicates that the residuals are not joint-normal distributed. Tests for the number of cointegrating vectors (<italic>r</italic>) are reported with the trace test statistic (as per the Johansen methodology) and were found to produce results that did not differ from those obtained via the maximum eigenvalue test. Statistical significance indicates that the corresponding hypothesis (i.e. <italic>r</italic> = 0 or <italic>r</italic> &#x00A3; 1) may be rejected. ADF <italic>p</italic>-values are reported for the residual series obtained from single equation regressions. In each instance, the dependent variable (which is indicated above the relevant column) is either the corresponding shock (as listed) or variation in real output that is less than the medium-frequency threshold of 200 quarters. All calculations were obtained using <italic>R</italic>.</p></fn>
<fn id="TFN0004"><label>&#x002A;</label><p>, Statistical significance at 10&#x0025;;</p></fn>
<fn id="TFN0005"><label>&#x002A;&#x002A;</label><p>, Statistical significance at 5&#x0025;;</p></fn>
<fn id="TFN0006"><label>&#x002A;&#x002A;&#x002A;</label><p>, Statistical significance at 1&#x0025;.</p></fn>
<fn><p>ADF, Augmented Dickey-Fuller; VAR, vector autoregressive mode; OLS, ordinary least squares.</p></fn>
</table-wrap-foot>
</table-wrap>
<p>On account of the non-robustness of the Johansen procedure under non-normally distributed errors, we opt to test for cointegration via the Engle and Granger (<xref ref-type="bibr" rid="CIT0017">1987</xref>) procedure. The Engle-Granger test for cointegration does not require the strong assumption of normally distributed errors for validity, reducing our risk of a type one error. <xref ref-type="table" rid="T0002">Table 2</xref> reports ADF tests of the residuals obtained from OLS regressions of the cycles on each of the shocks and of the shocks on each of the cycles. We find that none of the residuals of the shocks regressed on the cycles test as stationary at the 5&#x0025; or even the 10&#x0025; level; it is worth noting, however, that the combined path of permanent shocks to output is associated with a <italic>p</italic>-value of 0.114, and that the combined path of all five shocks tests as stationary at the 10&#x0025; level of significance. Reversing our specification, ADF tests indicate that a regression of the cycles on either the combined path of permanent shocks or the combined path of all shocks produces residuals that test as stationary at the 5&#x0025; level. No other set of cycle residuals tests as stationary at any traditional level of significance.</p>
<p>In sum, our tests for cointegration yield an interesting refinement to the findings reported in <xref ref-type="table" rid="T0001">Table 1</xref>. As discussed above, the results reported in <xref ref-type="table" rid="T0001">Table 1</xref> indicate that all of the structural shocks (barring the real interest rate shock) are more strongly correlated with medium-term deviation cycles than with short-term deviation cycles. Here we find that the combined path of permanent shocks and the combined path of all five shocks &#x2013; the two series of structural shocks that were found to have the highest correlation with the medium-term deviation cycles &#x2013; also appear to be cointegrated with medium-term deviation cycles. Our Engle-Granger tests show that in addition to being highly correlated with medium-term deviation cycles, the combined path of permanent shocks and of all five shocks contain sufficient informational overlap with these cycles to render them stationary. Thus, interpreting our tests for cointegration as tests for a common underlying stochastic trend (Engle &#x0026; Granger <xref ref-type="bibr" rid="CIT0017">1987</xref>), these test results are indicative of a strong degree of informational overlap between these series.</p>
</sec>
<sec id="s0006">
<title>Conclusion</title>
<p>Our comparison of deviation cycles with business cycles identified by an open-economy SVAR model produced several tentative, but interesting, conclusions. We did not find evidence that the high-frequency deviation cycle neatly corresponds to the purely transitory demand-based business cycle as measured by the open-economy SVAR. Rather, permanent shocks to output (often interpreted as supply shocks) seem to constitute an important source of variation in the high-frequency deviation cycle. Medium-term cycles were more strongly related with all shocks and combinations thereof, except shocks to the real interest rate. However, it seems that medium-term deviation cycles primarily capture business cycle information driven by permanent shocks to output, as suggested by our tests for cointegration.</p>
<p>Our findings suggest that deviation cycle analysis should be interpreted with caution. The medium-term deviation cycle seems to provide a good approximation of the South African business cycle, if one is interested in studying cycles derived from both transitory and permanent shocks, that is, demand- and supply-side variation in output. However, we did not find that short-term deviation cycles capture distinctly transitory, demand-driven information, as has been assumed in some applications. One should thus be cautious of drawing strong conclusions about the nature of business cycles from filter-based deviation cycle estimates, particularly if the objective of the study relies on assuming that high-frequency deviation cycles correspond to transitory demand shocks.</p>
</sec>
</body>
<back>
<ack>
<title>Acknowledgements</title>
<p>Willem Boshoff would like to acknowledge financial support from Economic Research Southern Africa (ERSA) for an earlier version of the paper, which appeared as a working paper: ERSA Working Paper 200. Willem Boshoff would like to thank Laurie Binge for research assistance on an earlier revision and would like to thank Adrian Pagan for enlightening discussions on an early version of this article, which led to the current version</p>
<sec id="s20007" sec-type="COI-statement">
<title>Competing interests</title>
<p>The authors declare that they have no financial or personal relationships that may have inappropriately influenced them in writing this article.</p>
</sec>
<sec id="s20008">
<title>Authors contributions</title>
<p>W.H.B. was responsible for the concept and earlier econometrics. L.M. dealt with the econometrics.</p>
</sec>
</ack>
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<fn-group>
<fn><p><bold>How to cite this article:</bold> Boshoff, W.H. &#x0026; McLean, L., 2018, &#x2018;What do deviation cycles measure? An analysis of the informational content of filter-based business cycles&#x2019;, <italic>South African Journal of Economic and Management Sciences</italic> 21(1), a1689. <ext-link ext-link-type="uri" xlink:href="https://doi.org/10.4102/sajems.v21i1.1689">https://doi.org/10.4102/sajems.v21i1.1689</ext-link></p></fn>
<fn id="FN0001"><label>1</label><p>Deviation cycles are also sometimes referred to as growth cycles; see Canova (<xref ref-type="bibr" rid="CIT0008">1998</xref>) for a critical summary.</p></fn>
<fn id="FN0002"><label>2</label><p>See for instance Ag&#x00E9;nor, McDermott and Prasad (2000) or Rand and Tarp (2002).</p></fn>
<fn id="FN0003"><label>3</label><p>See Du Plessis et al. (<xref ref-type="bibr" rid="CIT0015">2008</xref>) for an extended discussion.</p></fn>
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