Abstract
Multiplicative random cascade model naturally reproduces the intermittency or multifractality, which is frequently shown among hierarchical complex systems such as turbulence and financial markets. As described herein, we investigate the validity of a multiplicative hierarchical random cascade model through an empirical study using financial data. Although the intermittency and multifractality of the time series are verified, random multiplicative factors linking successive hierarchical layers show a strongly negative correlation. We extend the multiplicative model to incorporate an additional stochastic term. Results show that the proposed model is consistent with all the empirical results presented here.
Similar content being viewed by others
References
Arneodo A, Bacry E, Muzy JF (1998b) Random cascades on wavelet dyadic trees. J Math Phys 39:4142–4164
Arneodo A, Muzy JF, Sornette D (1998a) “Direct” causal cascade in the stock market. Eur Phys J B 2:277–282
Bacry E, Delour J, Muzy JF (2001) Multifractal random walk. Phys Rev E 64:026103
Bacry E, Muzy JF, Arneodo A (1993) Singularity spectrum of fractal signals from wavelet analysis: exact results. J Stat Phys 70:635–674
Cont R (2001) Empirical properties of asset returns: stylized facts and statistical issues. Quant Finan 1:223–236
Daubechies I (1992) Ten lectures on wavelets, the Society for Industrial and Applied Mathematics. Philadelphia
Frisch U (1995) Turbulence: the legacy of A.N. Kolmogorov. Cambridge University Press
Ghashghaie S, Breymann W, Peinke J, Talkner P, Dodge Y (1996) Turbulent cascade in foreign exchange markets. Nature 381:767–770
Jiménez J (2000) Intermittency and cascades. J Fluid Mech 409:99–120
Jiménez J (2007) Intermittency in turbulence. Proc. In: 15th ’Aha Huliko’ a Winter Workshop
Kolmogorov AN (1941) The local structure of turbulence in incompressible viscous fluids for very large Reynolds numbers. Dokl Nauk SSSR 30:301–305
Kolmogorov AN (1962) A refinement of previous hypotheses related to the local structure of turbulence in a viscous incompressible fluid at high Reynolds number. J Fluid Mech 13:82–85
Lynch PE, Zumbach GO (2003) Market heterogeneities and the causal structure of volatility. Quant Finan 3:320–331
Mandelbrot BB (1963) The variation of certain speculative prices. J Business 36:394–419
Mandelbrot BB (1974) Intermittent turbulence in self-similar cascades: divergence of high moments and dimension of the carrier. J Fluid Mech 62:331–358
Müller UA, Dacrogna MM, Davé RD, Olsen RB, Pictet OV, von Weizsäcker JE (1997) Volatilities of different time resolutions—analyzing the dynamics of market components. J Empirical Finance 4:213–239
Muzy JF, Bacry E, Arneodo A (1993) Multifractal formalism for fractal signals: the structure-function approach versus the wavelet-transform modulus-maxima method. Phys Rev E 47:875–884
Richardson LF (1922) Weather Prediction by Numerical Process, p. 66. Cambridge University Press, reprinted by Dover
Schmitt F, Schertzer D, Lovejoy S (1999) Multifractal analysis of Foreign exchange data. Appl Stochastic Models Data Anal 15:29–53
Acknowledgements
This research was partially supported by a Grant-in-Aid for Scientific Research (C) No. 16K01259.
Author information
Authors and Affiliations
Corresponding author
Ethics declarations
Conflict of interest
On behalf of all authors, the corresponding author states that the authors have no conflict of interest, financial or otherwise, in relation to this study.
Appendix: WTMM method
Appendix: WTMM method
This appendix briefly describes the WTMM method based on the continuous wavelet transform proposed earlier in the literature (Bacry et al. 1993; Muzy et al. 1993). The continuous wavelet transformation of the function f using the analyzing wavelet \(\psi\) is defined as
where parameters s and x respectively represent the dilation and the translation of the function \(\psi\). The analyzing wavelet \(\psi\) has been assumed to have \(N_{\psi }>0\) vanishing moments. The successive derivative of the Gaussian function
has \(N_{\psi }>0\) vanishing moments. Here we specify \(N_{\psi }=2\) and use the second derivative of the Gaussian function as the analyzing wavelet. The WTMM method builds a partition function from the modulus maxima of the wavelet transform defined at each scale s as the local maxima of \(|W_{\psi }[f](x,s)|\) regarded as a function of x. Those maxima mutually connect across scales and form ridge lines designated as maxima lines. The set \(\mathcal {L}(s_0)\) is the set of all the maxima lines l that satisfy
The partition function is defined by the maxima lined as
Assuming the power-law behavior of the partition function
one can define the exponents \(\tau (q)\). The singular spectrum \(D(\alpha )\) can be computed using the Legendre transform of \(\tau (q)\):
About this article
Cite this article
Maskawa, Ji., Kuroda, K. & Murai, J. Multiplicative random cascades with additional stochastic process in financial markets. Evolut Inst Econ Rev 15, 515–529 (2018). https://doi.org/10.1007/s40844-018-0112-y
Published:
Issue Date:
DOI: https://doi.org/10.1007/s40844-018-0112-y