Chapter 9
Stochastic Correlation

Stochastic correlation models may provide a more realistic approach to the pricing and hedging of certain types of exotic derivatives, such as worst-of and best-of options and correlation swaps and correlation options. In this chapter, we review various types of stochastic correlation models and propose a framework for the pricing of realized correlation derivatives that is consistent with variance swap markets.

9.1 Stochastic Single Correlation

Consider the following general model framework for two assets S(1) and S(2):

equation

where μ's are instant drift coefficients, σ's are instant volatility coefficients, and ρ is the instant correlation coefficient between the driving Brownian motions W's. Here all the coefficients may be stochastic, and we focus on ρ.

There are some simple ways to make ρ stochastic and comprised between −1 and 1; for example, take c09-math-0002 where Z is an independent Brownian motion. The dynamics of t may then be found by means of the Ito-Doeblin theorem. One issue with this approach is that the parameters may not be very intuitive.

A better approach is to specify diffusion dynamics for ρ and examine the Feller conditions at bounds −1 and 1 (see Section 2.4.2.2). A popular process here is the affine Jacobi process, also known as a Fischer-Wright process, which is very similar to Heston's stochastic volatility process (see Section 2.4.2.2):

equation

where c09-math-0004 is the long-term mean, κ is the mean reversion speed, and α is the volatility of instant correlation. The Feller condition is then c09-math-0005. A technical analysis of this type of process can be found in van Emmerich (2006).

Figure 9.1 shows the path obtained for an affine Jacobi process with parameters c09-math-0006. Observe how all values are comprised between −1 and 1.

Stock price on this chart begins at 0.65, fluctuates and drops to −0.52 at day 220, fluctuates and recovers to −0.2 at day 250.

Figure 9.1 Sample path of an affine Jacobi process with parameters c09-math-0007.

9.2 Stochastic Average Correlation

We now shift our focus to average correlation measures c09-math-0008 as introduced in Section 6.3. Because the correlation matrix c09-math-0009 must be positive-definite at all times we cannot naively extend the single correlation case with, for instance, n(n − 1)/2 affine Jacobi processes and take their average. Note that as a consequence of positive-definiteness ρ(x) is actually comprised between 0 and 1 for large n.

Before we go into further detail we must distinguish between nontradable correlation, such as rolling historical or implied correlations, and tradable correlation, such as the historical correlation observed over a fixed time period [0, T]:

  • Nontradable average correlation can be modeled quite freely, using, for example, a standard Jacobi process between 0 and 1 or econometric processes such as Constant and Dynamic Conditional Correlation models (see, e.g., Engle (2009)).
  • Tradable average correlation requires special consideration to be consistent with other related securities such as variance swaps.

The rest of this section is devoted to the study of tradable average correlation.

9.2.1 Tradable Average Correlation

Consider c09-math-0010 which was introduced in Section 7-1.2 and is related to the proxy formula c09-math-0011 introduced in Section 6.3.1. Because c09-math-0012 is the ratio of two tradable assets—namely, basket variance and average constituent variance—we can derive its dynamics from those of the two tradable assets. For example, suppose we have:

equation

where Xt is the price of basket variance at time t, YtXt is the price of average constituent variance at time t, and the driving Brownian motions W, Z are taken under the forward-neutral measure.

Using the Ito-Doeblin theorem the resulting dynamics for c09-math-0014 are then:

where B is another standard Brownian motion constructed from W and Z.

Note that, as the ratio of two prices, c09-math-0016 is not the price of correlation at time t, which is why the drift coefficient in Equation (9.1) is nonzero under the forward-neutral measure:

equation

Because c09-math-0018 is invariant when multiplying X and Y by the same scalar λ, we may further focus on one-dimensional reductions of the model (see Section 7-2.3) and assume that f, g, h are functions of X/Y:

equation

In this case Equation (9.1) becomes one-dimensional; that is, the drift and volatility coefficients depend only on time and c09-math-0020. This makes the following Feller analysis considerably easier.

Omitting the time subscript for ease of exposure and using x to denote the state variable we may rewrite Equation (9.1) as:

The Feller conditions at bounds 0 and 1 are then:

equation

Dividing both the numerator and denominator by g2(u), the integrand in s(y) may be rewritten as c09-math-0023 with c09-math-0024. Furthermore,

  • As x → 0 a sufficient condition is that c09-math-0025 in which case we have c09-math-0026 for y0 and y close to 0, and thus c09-math-0027. A formal proof of sufficiency is proposed in Appendix 9.A.
  • As x → 1 a necessary condition is that s(y) → ∞, which in turn implies that c09-math-0028 diverges (see Appendix 9.B for a formal proof). An analysis of this quantity over the domain p ≥ 0 and | h | ≤ 1 reveals that the only singularity is at (1, 1). Thus, as a corollary we have the weak necessary condition c09-math-0029 and h(u) → 1 as u → 1. This configuration intuitively makes sense: if average correlation is close to 1, there is almost no diversification effect, and basket variance and average constituent variance become almost identical.

Additionally, we want fg because basket variance is more volatile than average constituent variance, which unfortunately makes the sufficient condition stated above ineffective, since p ≥ 1. We must keep all these properties in mind when researching suitable functions f, g, and h.

9.2.2 The B-O Model

The following model, which we call the B-O model (for beta-omega), is a further step towards a suitable stochastic average correlation model:

9.3 equation

where ω is the instant volatility of constituent volatility and β is the “additional” volatility of basket volatility.1 The corresponding dynamics for the average correlation c09-math-0035 are then given by Equation (9.2) using the functions:

equation

Unfortunately, both lower and upper bounds [0,1] turn out to be attracting in the B-O model, making it unsuitable for extreme starting values ρ0 and long-term horizons T. However, empirical simulations exhibit plausible paths. Further research is needed here.

Figure 9.2 shows 10 sample paths obtained with parameters ω = 70%, β = 40% and c09-math-0037. Remarkably enough, using Monte Carlo simulations the price of correlation c09-math-0038 in this model appears to be close to the initial value c09-math-0039, also known as variance-implied correlation. This suggests that the fair strike of a correlation swap on c09-math-0040 should be close to c09-math-0041, and by extension a similar result should apply to standard correlation swaps.

Ten sample paths spread between 0.1 and 0.8 till 0.35, and further spread between 0.1 and 0.95.

Figure 9.2 Ten sample paths using the B-O model with parameters ω = 70%, β = 40%, and c09-math-0042.

9.3 Stochastic Correlation Matrix

A yet more ambitious endeavor is to devise a model for the evolution of the entire correlation matrix c09-math-0043 through time. As pointed out earlier, the difficulty here is to ensure that Rt is positive-definite at all times.

It is worth emphasizing that, when correlations are tradable, we should also ensure that the induced dynamics of average correlation c09-math-0044 be consistent with variance swaps under the forward-neutral measure.

As already pointed out in Section 6.2, equity correlation matrices have structure—namely, there is typically one large eigenvalue dominating all others, and the associated eigenvector corresponds to an all-stock portfolio. As such an equity correlation matrix cannot be viewed as any kind of random matrix.

Here we need to be more specific about the meaning of a (symmetric) random matrix. This concept was first introduced by Wishart (1928) in the form M = XXT where X is an n × n matrix of independent and identically distributed random variables; the special case where X is Gaussian deserves particular attention since it tends to the identity matrix as n → ∞. Another approach is Wigner's, whereby c09-math-0045; a remarkable property is that the empirical distribution of ordered eigenvalues then follows the semi-circle law:

equation

9.3.1 Spectral Decomposition and the Common Factor Model

The empirical analysis of equity correlation matrices suggests that they may be viewed as the sum of a (truly) random matrix and an orthogonal projector onto the maximal eigenvector. Following the spectral theorem we may indeed write:

equation

where (v1,…, vn) is an orthonormal basis of eigenvectors with eigenvalues λ1 ≤ λn. The residual matrix c09-math-0048 may then be approximated by a Wishart-type matrix.

For large n we could ignore c09-math-0049 altogether and write:

equation

where a1,…, an are the entries of the maximal eigenvector vn and c09-math-0051. Note that c09-math-0052 has different eigenelements from R; however, λn is related to average correlation because c09-math-0053 as n → ∞.

This approach corroborates Boortz's Common Factor Model (2008) whereby:

equation

where (ξt,1,…, ξt,n) is a vector of correlated stochastic processes in (−1, 1), such as affine Jacobi processes. One issue with the Common Factor Model is that the (equally weighted) average realized correlation has a risk-neutral drift, which has no particular reason to fit in the framework of Section 9.2.1. In other words the Common Factor Model does not appear to be consistent with variance swap markets.

9.3.2 The c09-math-0055 Fischer-Wright Model

Recent work by Ahdida and Alfonsi (2012) alternatively proposes the following stochastic process for the correlation matrix Rt, which is a generalization of the Jacobi process:

equation

where the matrix c09-math-0057 is the long-term correlation mean, c09-math-0058 is a diagonal matrix of mean-reversion speeds, α = diag1,…, αn) is a diagonal matrix of volatility coefficients, c09-math-0059 is the diagonal matrix with coefficient 1 at position (i,i) and 0 elsewhere, c09-math-0060 denotes the unique square root of a positive-semidefinite matrix H, and (Wt) is an n × n matrix of independent standard Brownian motions.

Subject to the condition c09-math-0061 being positive-semidefinite, the Ahdida-Alfonsi process is guaranteed to remain a valid correlation matrix through time; however, a corrected Euler scheme is required for simulation.

Unfortunately, Ahdida and Alfonsi have not studied the eigenelements of their respective correlation matrix processes. and it is difficult to tell how realistic their model is within the realm of equity correlation matrices. In particular, there is no guarantee that the induced dynamics of average correlation can be made consistent with realistic dynamics of basket variance and average constituent variance in the fashion described early in the chapter. Further research is thus needed.

References

  1. Ahdida, Abdelkoddousse, and Aurélien Alfonsi. 2012. “A Mean-Reverting SDE on Correlation Matrices.” arXiv:1108.5264.
  2. Boortz, C. Kaya. 2008. “Modelling Correlation Risk.” Diplomarbeit preprint, Institut für Mathematik, Technische Universität Berlin & Quantitative Products Laboratory, Deutsche Bank AG.
  3. Engle, Robert. 2009. Anticipating Correlations: A New Paradigm for Risk Management. Princeton, NJ: Princeton University Press.
  4. van Emmerich, Cathrin. 2006. “Modelling Correlation as a Stochastic Process.” Bergische Universität Wuppertal. Preprint.
  5. Wishart, John. 1928. “The Generalised Product Moment Distribution in Samples from a Normal Multivariate Population.” Biometrika 20A (1–2): 32–52.

Problems

Consider a stock S, which does not pay dividends, with dollar price S$, and let X be the exchange rate of one dollar into euros. Assume that S$ and X both follow geometric Brownian motions under the dollar risk-neutral measure with joint dynamics:

equation

where r$ is the constant dollar interest rate, σ, ν and η are free constant parameters, and W, Z are standard Brownian motions with stochastic correlation c09-math-0063.

  1. Show that the forward price of S quanto euro for maturity T is c09-math-0064.
  2. Assume that S0$ = $100, r$ = 0, σ = 25%, η = 10%, c09-math-0065 with c09-math-0066. Compute the one-year forward price of S quanto euro using Monte Carlo simulations over 252 trading days. Answer: €100.60

Consider the model for stochastic average correlation:

equation
  1. Verify that the process remains within (0,1) and that the lower bound is non-attracting.
  2. Define c09-math-0068. Find f(x), g(x) such that c09-math-0069 satisfies Equation (9.2). Hint: Show that c09-math-0070 where p = f/g and solve for p.
  3. Do you think that this model is suitable?

Appendix 9.A: Sufficient Condition for Lower Bound Unattainability

Following the notations of Section 9.2.1, suppose that c09-math-0071. By the definition of a limit this means that for arbitrary ϵ > 0 there exists an α > 0 such that:

equation

Thus, for all 0 < u ≤ α, c09-math-0073. By integration over [y0, y] ⊂ [0, α] we get:

equation

Taking exponentials:

equation

and thus c09-math-0076 since c09-math-0077 diverges for any β ≥ 0.

Appendix 9.B: Necessary Condition for Upper Bound Unattainability

Suppose that c09-math-0078 converges to a finite limit . By the definition of a limit this means that for arbitrary ϵ > 0 there exists an α < 1 such that:

equation

Thus, for all α ≤ u ≤ 1, c09-math-0080. By integration over [y0, y] ⊂ [α, 1] we get:

equation

Taking exponentials:

equation

and thus c09-math-0083 is finite since c09-math-0084 converges for any β, thereby contradicting the requirement that c09-math-0085.

 

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