Abstract

A field theoretical framework is developed for the Hawkes self-excited point process with arbitrary memory kernels by embedding the original non-Markovian one-dimensional dynamics onto a Markovian infinite-dimensional one. The corresponding Langevin dynamics of the field variables is given by stochastic partial differential equations that are Markovian. This is in contrast to the Hawkes process, which is non-Markovian (in general) by construction as a result of its (long) memory kernel. We derive the exact solutions of the Lagrange-Charpit equations for the hyperbolic master equations in the Laplace representation in the steady state, close to the critical point of the Hawkes process. The critical condition of the original Hawkes process is found to correspond to a transcritical bifurcation in the Lagrange-Charpit equations. We predict a power law scaling of the PDF of the intensities in an intermediate asymptotics regime, which crosses over to an asymptotic exponential function beyond a characteristic intensity that diverges as the critical condition is approached. We also discuss the formal relationship between quantum field theories and our formulation. Our field theoretical framework provides a way to tackle complex generalisation of the Hawkes process, such as nonlinear Hawkes processes previously proposed to describe the multifractal properties of earthquake seismicity and of financial volatility.

Highlights

  • The self-excited conditional Poisson process introduced by Hawkes [1,2,3] has progressively been adopted as a useful firstorder model of intermittent processes with time clustering, such as those occurring in seismicity and financial markets

  • We have presented an analytical framework of the Hawkes process for an arbitrary memory kernel, based on the master equation governing the behavior of auxiliary field variables

  • While the Hawkes point process is non-Markovian by construction, the introduction of auxiliary field variables provides a formulation in terms of linear stochastic partial differential equations that are Markovian

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Summary

INTRODUCTION

The self-excited conditional Poisson process introduced by Hawkes [1,2,3] has progressively been adopted as a useful firstorder model of intermittent processes with time (and space) clustering, such as those occurring in seismicity and financial markets. We propose a natural formulation of the Hawkes process in the form of a field theory of probability density functionals taking the form of a field master equation This formulation is found to be ideally suited to investigate the hitherto ignored properties of the distribution of Hawkes intensities, which we analyze in depth in a series of increasingly sophisticated forms of the memory kernel characterizing how past events influence the triggering of future events. These sections are complemented by seven Appendixes, in which the detailed analytical derivations are provided

Notation
Definition of the Hawkes conditional Poisson process
Generalized non-Markovian Langevin equation
Origin of the non-Markovian property and Markov embedding
Fokker-Planck descriptions of non-Markovian processes
Field description for an infinite number of auxiliary variables
Relation to the non-Markovian Hawkes processes
Introduction of auxiliary variables
Mapping to Markovian dynamics
Master equation
Discrete sum of exponential kernels
Laplace representation of the master equation
General kernels
Field master equation
General formulation
Main results
Single exponential kernel
Steady-state solution
Time-dependent solution
Another derivation of the power law exponent
Double exponential kernel
Discrete superposition of exponential kernels
General case
DISCUSSION
Schrödinger-like representation for the Fokker-Planck equation
Schrödinger-like representation for the field Fokker-Planck equation
Quantum-field-like representation for the Hawkes process
CONCLUSION
Introduction of a UV cutoff
Kramers-Moyal approach
Consistency check 2
Proof of that its eigenvalues are real
Determinant
Inverse matrix
Findings
Proof that the eigenvalues are real

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