Markov switching multifractal

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In financial econometrics (the application of statistical methods to economic data), the Markov-switching multifractal (MSM) is a model of asset returns developed by Laurent E. Calvet and Adlai J. Fisher that incorporates stochastic volatility components of heterogeneous durations. [1] [2] MSM captures the outliers, log-memory-like volatility persistence and power variation of financial returns. In currency and equity series, MSM compares favorably with standard volatility models such as GARCH(1,1) and FIGARCH both in- and out-of-sample. MSM is used by practitioners in the financial industry to forecast volatility, compute value-at-risk, and price derivatives.

Contents

MSM specification

The MSM model can be specified in both discrete time and continuous time.

Discrete time

Let denote the price of a financial asset, and let denote the return over two consecutive periods. In MSM, returns are specified as

where and are constants and {} are independent standard Gaussians. Volatility is driven by the first-order latent Markov state vector:

Given the volatility state , the next-period multiplier is drawn from a fixed distribution M with probability , and is otherwise left unchanged.

drawn from distribution Mwith probability
with probability

The transition probabilities are specified by

.

The sequence is approximately geometric at low frequency. The marginal distribution M has a unit mean, has a positive support, and is independent of k.

Binomial MSM

In empirical applications, the distribution M is often a discrete distribution that can take the values or with equal probability. The return process is then specified by the parameters . Note that the number of parameters is the same for all .

Continuous time

MSM is similarly defined in continuous time. The price process follows the diffusion:

where , is a standard Brownian motion, and and are constants. Each component follows the dynamics:

drawn from distribution Mwith probability
with probability

The intensities vary geometrically with k:

When the number of components goes to infinity, continuous-time MSM converges to a multifractal diffusion, whose sample paths take a continuum of local Hölder exponents on any finite time interval.

Inference and closed-form likelihood

When has a discrete distribution, the Markov state vector takes finitely many values . For instance, there are possible states in binomial MSM. The Markov dynamics are characterized by the transition matrix with components . Conditional on the volatility state, the return has Gaussian density

Conditional distribution

Closed-form Likelihood

The log likelihood function has the following analytical expression:

Maximum likelihood provides reasonably precise estimates in finite samples. [2]

Other estimation methods

When has a continuous distribution, estimation can proceed by simulated method of moments, [3] [4] or simulated likelihood via a particle filter. [5]

Forecasting

Given , the conditional distribution of the latent state vector at date is given by:

MSM often provides better volatility forecasts than some of the best traditional models both in and out of sample. Calvet and Fisher [2] report considerable gains in exchange rate volatility forecasts at horizons of 10 to 50 days as compared with GARCH(1,1), Markov-Switching GARCH, [6] [7] and Fractionally Integrated GARCH. [8] Lux [4] obtains similar results using linear predictions.

Applications

Multiple assets and value-at-risk

Extensions of MSM to multiple assets provide reliable estimates of the value-at-risk in a portfolio of securities. [5]

Asset pricing

In financial economics, MSM has been used to analyze the pricing implications of multifrequency risk. The models have had some success in explaining the excess volatility of stock returns compared to fundamentals and the negative skewness of equity returns. They have also been used to generate multifractal jump-diffusions. [9]

MSM is a stochastic volatility model [10] [11] with arbitrarily many frequencies. MSM builds on the convenience of regime-switching models, which were advanced in economics and finance by James D. Hamilton. [12] [13] MSM is closely related to the Multifractal Model of Asset Returns. [14] MSM improves on the MMAR's combinatorial construction by randomizing arrival times, guaranteeing a strictly stationary process. MSM provides a pure regime-switching formulation of multifractal measures, which were pioneered by Benoit Mandelbrot. [15] [16] [17]

See also

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References

  1. Calvet, L.; Fisher, A. (2001). "Forecasting multifractal volatility" (PDF). Journal of Econometrics. 105: 27–58. doi:10.1016/S0304-4076(01)00069-0. S2CID   119394176.
  2. 1 2 3 Calvet, L. E. (2004). "How to Forecast Long-Run Volatility: Regime Switching and the Estimation of Multifractal Processes". Journal of Financial Econometrics. 2: 49–83. CiteSeerX   10.1.1.536.8334 . doi:10.1093/jjfinec/nbh003.
  3. Calvet, Laurent; Fisher, Adlai (July 2003). "Regime-switching and the estimation of multifractal processes". NBER Working Paper No. 9839. doi: 10.3386/w9839 .
  4. 1 2 Lux, T. (2008). "The Markov-Switching Multifractal Model of Asset Returns". Journal of Business & Economic Statistics. 26 (2): 194–210. doi:10.1198/073500107000000403. S2CID   55648360.
  5. 1 2 Calvet, L. E.; Fisher, A. J.; Thompson, S. B. (2006). "Volatility comovement: A multifrequency approach". Journal of Econometrics. 131 (1–2): 179–215. CiteSeerX   10.1.1.331.152 . doi:10.1016/j.jeconom.2005.01.008.
  6. Gray, S. F. (1996). "Modeling the conditional distribution of interest rates as a regime-switching process". Journal of Financial Economics. 42: 27–77. doi:10.1016/0304-405X(96)00875-6.
  7. Klaassen, F. (2002). "Improving GARCH volatility forecasts with regime-switching GARCH" (PDF). Empirical Economics. 27 (2): 363–394. doi:10.1007/s001810100100. S2CID   29571612.
  8. Bollerslev, T.; Ole Mikkelsen, H. (1996). "Modeling and pricing long memory in stock market volatility". Journal of Econometrics. 73: 151–184. doi:10.1016/0304-4076(95)01736-4.
  9. Calvet, Laurent E.; Fisher, Adlai J. (2008). Multifractal volatility theory, forecasting, and pricing. Burlington, MA: Academic Press. ISBN   9780080559964.
  10. Taylor, Stephen J (2008). Modelling financial time series (2nd ed.). New Jersey: World Scientific. ISBN   9789812770844.
  11. Wiggins, J. B. (1987). "Option values under stochastic volatility: Theory and empirical estimates" (PDF). Journal of Financial Economics. 19 (2): 351–372. doi:10.1016/0304-405X(87)90009-2.
  12. Hamilton, J. D. (1989). "A New Approach to the Economic Analysis of Nonstationary Time Series and the Business Cycle". Econometrica. 57 (2): 357–384. CiteSeerX   10.1.1.397.3582 . doi:10.2307/1912559. JSTOR   1912559.
  13. Hamilton, James (2008). "Regime-Switching Models". New Palgrave Dictionary of Economics (2nd ed.). Palgrave Macmillan Ltd. ISBN   9780333786765.
  14. Mandelbrot, Benoit; Fisher, Adlai; Calvet, Laurent (September 1997). "A multifractal model of asset returns". Cowles Foundation Discussion Paper No. 1164. SSRN   78588.
  15. Mandelbrot, B. B. (2006). "Intermittent turbulence in self-similar cascades: Divergence of high moments and dimension of the carrier". Journal of Fluid Mechanics. 62 (2): 331–358. doi:10.1017/S0022112074000711. S2CID   222375985.
  16. Mandelbrot, Benoit B. (1983). The fractal geometry of nature (Updated and augm. ed.). New York: Freeman. ISBN   9780716711865.
  17. Mandelbrot, Benoit B.; J.M. Berger; et al. (1999). Multifractals and 1/f noise : wild self-affinity in physics (1963 - 1976) (Repr. ed.). New York, NY [u.a.]: Springer. ISBN   9780387985398.