Contrary to common beliefs, financial correlations display statistically significant and expected properties.
Correlation levels as well as correlation volatility are generally higher in economic crises, which should be taken into consideration by traders and risk managers.
Strong mean reversion can be found in correlations and the distribution of correlations is typically not normal or lognormal.
THE STUDY –
The input data of the distribution tests were daily correlation values between all 30 Dow stocks from 1972 to 2012. This resulted in 426,300 correlation values. The distribution is shown in this figure. It can be observed that correlations between the stocks in the Dow are mostly positive . In fact, 77.23% of all 426,300 correlation values were positive.
The versatile Johnson SB distribution with four parameters, 𝛾 and 𝛿 for the shape, μ for location, and 𝜎 for scale, provided the best fit.
Standard distributions such as normal distribution, lognormal distribution, or beta distribution provided a poor fit.
Correlation Type | Average Correlation | Correlation Volatility | Reversion Rate | Best Fit Distribution |
---|---|---|---|---|
Equity | 34.83% | 79.73% | 77.51% | Johnson SB |
Bond | 41.67% | 63.74% | 25.79% | Generalized Extreme Value |
Default Probability | 30.43% | 87.74% | 29.97% | Johnson SB |
THE RESULT –
THE RESULT –
Correlation Level | Correlation Volatility | |
---|---|---|
Expansionary period | 27.46% | 71.17% |
Normal economic period | 32.73% | 83.40% |
Recession | 36.96% | 80.48% |
THE RESULT –
where
𝑆t: price at time t
𝑆t–1: price at the previous point in time 𝑡— 1
𝜕: partial derivative coefficient
The above equation tells us: If 𝑆t–1 increases by a very small amount, 𝑆t — 𝑆t–1, will decrease by a certain amount, and vice versa. This is intuitive: If 𝑆t–1 has decreased and is low at 𝑡 — 1 (compared to the mean of S, 𝜇S), then at the next point in time t, mean reversion will pull up 𝑆t–1 to 𝜇s and therefore increase 𝑆t — 𝑆t–1. If 𝑆t–1 has increased and is high in 𝑡 — 1 (compared to the mean of S,𝜇S), then at the next point in time t, mean reversion will pull down 𝑆t–1, to 𝜇s and therefore decrease 𝑆t — 𝑆t–1. The degree of the pull is the degree of the mean reversion, also called mean reversion rate, mean reversion speed, or gravity.
The degree of mean reversion can be calculated by starting with the discrete Vasicek process,
where
𝑆t : price at time t
𝑆t–1: price at the previous point in time 𝑡 — 1
𝑎: degree of mean reversion, also called mean reversion rate or gravity, 0 ≤ 𝑎 ≤ 1
𝜇s: long-term mean of 𝑆
𝜎s: volatility of 𝑆
𝜀: random drawing from a standardized normal distribution at time 𝑡, ε(𝑡): 𝑛 ~ (0,1)
To deal with mean reversion, the stochasticity part in the above equation (i.e. 𝜎s𝜀 Δ𝑡) can be ignored. If Δ𝑡 = 1, then a mean reversion parameter of a = 1 will pull 𝑆t–1 to the long-term mean 𝜇s completely at every time step. For example, if is 80 and 𝜇s is 100, then a × (𝜇s — 𝑆t–1) = 1 × (100 — 80) = 20, so the 𝑆t–1 of 80 is mean reverted up to its long- term mean of 100. Naturally, a mean reversion parameter a of 0.5 will lead to a mean reversion of 50% at each time step, and a mean reversion parameter a of 0 will result in no mean reversion.To quantify mean reversion. Setting Δ𝑡 to 1, and ignoring stochasticity, we get
To find the mean reversion rate 𝑎, a standard regression analysis can be done of the form
𝑌 = 𝛼 + 𝛽𝑋
Hence, 𝑆t — 𝑆t–1 is being regressed with respect to 𝑆t–1:
To find the mean reversion rate 𝑎, a standard regression analysis can be done of the form
It can be observed that the regression coefficient 𝛽 is equal to the negative mean reversion parameter 𝑎.
After this the author runs a regression to find the empirical mean reversion of the earlier obtained correlation data. Hence 𝑆 represents the 30 × 30 Dow stock monthly average correlations from 1972 to 2012. The regression analysis is displayed in this figure.
where
𝐴𝐶: autocorrelation
𝜌t: correlation values for time period 𝑡
𝜌t–1: correlation values for time period 𝑡 — 1
𝐶𝑜𝑣: covariance;
This equation is algebraically identical with the Pearson correlation coefficient equation. The autocorrelation just uses the correlation values of time period 𝑡 and time period 𝑡 — 1 as inputs.
The input data of the distribution tests were daily correlation values between all 30 Dow stocks from 1972 to 2012. This resulted in 426,300 correlation values. The distribution is shown in this figure. It can be observed that correlations between the stocks in the Dow are mostly positive . In fact, 77.23% of all 426,300 correlation values were positive.
The versatile Johnson SB distribution with four parameters, 𝛾 and 𝛿 for the shape, μ for location, and 𝜎 for scale, provided the best fit.
Standard distributions such as normal distribution, lognormal distribution, or beta distribution provided a poor fit.
Correlation Type | Average Correlation | Correlation Volatility | Reversion Rate | Best Fit Distribution |
---|---|---|---|---|
Equity | 34.83% | 79.73% | 77.51% | Johnson SB |
Bond | 41.67% | 63.74% | 25.79% | Generalized Extreme Value |
Default Probability | 30.43% | 87.74% | 29.97% | Johnson SB |