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European Journal of Physics

Brownian representation of fractal quantum paths

Didier Sornette

Published Nov 1, 1990• 22 citations
Publisher

Abstract

The analogy between quantum 'paths' and random walks of a Brownian particle is extended to the relativistic regime. This yields a coherent picture of the fine structure of quantum paths: these can be viewed as analogies of the trajectory of a random walker. The fractal dimension of quantum paths is df=2 at scales large compared with the Compton wavelength Lambda but small compared with the de Broglie wavelength lambda and becomes df=1 at scales smaller than Lambda . The transition between the two regimes is exhibited explicitly and is analogous to the cross-over from ballistic to diffusive motion of Brownian particles. The analogue of the collisions in Brownian motion is electron-positron pair creations and annihilations, and the unit thermodynamic free energy kT corresponds to the rest mass mc2 of the particle.

DOI
10.1088/0143-0807/11/6/004

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The analogy between quantum 'paths' and random walks of a Brownian particle is extended to the relativistic regime. This yields a coherent picture of the fine structure of quantum paths: these can be viewed as analogies of the trajectory of a random walker. The fractal dimension of quantum paths is df=2 at scales large compared with the Compton wavelength Lambda but small compared with the de Broglie wavelength lambda and becomes df=1 at scales smaller than Lambda . The transition between the two regimes is exhibited explicitly and is analogous to the cross-over from ballistic to diffusive motion of Brownian particles. The analogue of the collisions in Brownian motion is electron-positron pair creations and annihilations, and the unit thermodynamic free energy kT corresponds to the rest mass mc2 of the particle.
The path integral formalism is used to describe the statistical properties of an ideal gas of spinless particles.It is shown that the quantum paths exhibit the same properties in non-relativistic and relativistic domains provided the creation of new particles is avoided.Some quantities associated with the paths are introduced, they have a simple meaning if the quantity β , where β is the reverse of the temperature, is considered as an ordinary time.The relation between the velocity on the path and the momentum is not the usual one, an extra term appears showing that the thermostat can not fix the average value of this velocity although all the thermodynamic quantities have their traditional values.The paths describe fluctuating trajectories on which the particles do not follow the equation of motion.For time intervals much shorter than β we recover the properties of the Brownian motion.The trajectories are located in space in a volume restricted by the Compton wavelength for the short distances and the thermal de Broglie wavelength for the largest ones.It is shown that the time-energy uncertainty is verified on the quantum paths.This suggests that the density matrix obtained by quantification of the classical canonical distribution function via the path integral formalism should not be totally identical to that obtained via the usual route.Strong arguments are given showing that β can be considered as an ordinary time and not as a formal quantity having the same dimension as time.This paper shows that for a time scale of 10 femtoseconds a totally new physics can be expected at room temperature.In addition it is suggested that the ratio /k B may play a decisive role in the foundation of a covariant statistical physics.
The path integral formalism is used to describe the statistical properties of \nan ideal gas of spinless particles. It is shown that the quantum paths exhibit \nthe same properties in non-relativistic and relativistic domains provided the \ncreation of new particles is avoided. Some quantities associated with the \npaths are introduced, they have a simple meaning if the quantity βh , where \nβ is the reverse of the temperature, is considered as an ordinary time. The \nrelation between the velocity on the path and the momentum is not the \nusual one, an extra term appears showing that the thermostat can not fix \nthe average value of this velocity although all the thermodynamic quantities \nhave their traditional values. The paths describe fluctuating trajectories on \nwhich the particles do not follow the equation of motion. For time intervals \nmuch shorter than βh we recover the properties of the Brownian motion. \nThe trajectories are located in space in a volume restricted by the Compton \nwavelength for the short distances and the thermal de Broglie wavelength \nfor the largest ones. It is shown that the time-energy uncertainty is verified \non the quantum paths. This suggests that the density matrix obtained by \nquantification of the classical canonical distribution function via the path integral formalism should not be totally identical to that obtained via the usual \nroute. Strong arguments are given showing that βh can be considered as \nan ordinary time and not as a formal quantity having the same dimension \nas time. This paper shows that for a time scale of 10 femtoseconds a totally new physics can be expected at room temperature. In addition it is \nsuggested that the ratio h/kB may play a decisive role in the foundation of \na covariant statistical physics.
The properties of an ideal gas of spinless particles are investigated by using the path integral formalism. It is shown that the quantum paths exhibit a fractal character which remains unchanged in the relativistic domain provided the creation of new particles is avoided, and the Brownian motion remains the stochastic process associated with the quantum paths. These results are obtained by using a special representation of the Klein-Gordon wave equation. On the quantum paths the relation between velocity and momentum is not the usual one. The mean square value of the velocity depends on the time needed to define the velocity and its value shows the interplay between pure quantum effects and thermodynamics. The fractal character is also investigated starting from wave equations by analyzing the evolution of a Gaussian wave packet via the Hausdorff dimension. Both approaches give the same fractal character in the same limit. It is shown that the time that appears in the path integral behaves like an ordinary time, and the key quantity is the time interval needed for the thermostat to give to the particles a thermal action equal to the quantum of action. Thus, the partition function calculated via the path integral formalism also describes the dynamics of the system for short time intervals. For low temperatures, it is shown that a time-energy uncertainty relation is verified at the end of the calculations. The energy involved in this relation has not a thermodynamic meaning but results from the fact that the particles do not follow the equations of motion along the paths. The results suggest that the density matrix obtained by quantification of the classical canonical distribution function via the path integral formalism should not be totally identical to that obtained via the usual route.
Using quantum parallelism on random walks as the original seed, we introduce new quantum stochastic processes, the open quantum Brownian motions. They describe the behaviors of quantum walkers—with internal degrees of freedom which serve as random gyroscopes—interacting with a series of probes which serve as quantum coins. These processes may also be viewed as the scaling limit of open quantum random walks and we develop this approach along three different lines: the quantum trajectory, the quantum dynamical map and the quantum stochastic differential equation. We also present a study of the simplest case, with a two level system as an internal gyroscope, illustrating the interplay between the ballistic and diffusive behaviors at work in these processes. Notation : orbital (walker) Hilbert space, in the discrete, in the continuum : internal spin (or gyroscope) Hilbert space : system Hilbert space : probe (or quantum coin) Hilbert space, : density matrix for the total system (walker + internal spin + quantum coins) : reduced density matrix on : : system density matrix in a quantum trajectory: . If diagonal and localized in position: ρ t : internal density matrix in a simple quantum trajectory X t : walker position in a simple quantum trajectory B t : normalized Brownian motion ξ t , : quantum noises
Though classical random walks have been studied for many years, research concerning their quantum analogues, quantum random walks, has only come about recently. Numerous simulations of both types of walks have been run and analyzed, and are generally well-understood. Research pertaining to one of the more important properties of classical random walks, namely, their ability to build fractal structures in diffusion-limited aggregation, has been particularly noteworthy. However, only now has research begun in this area in regards to quantum random motion. The study of random walks and the structures they build has various applications in materials science. Since all processes are quantum in nature, it is important to consider the quantum variant of diffusion-limited aggregation. Recognizing that Schrödinger equation and a classical random walk are both diffusion equations, it is possible to connect and compare them. Using similar parameters for both equations, we ran various simulations aggregating particles. Our results show that particles moving according to Schrödinger equation can create fractal structures, much like the classical random walk. Furthermore, the fractal dimensions of these quantum diffusion-limited aggregates vary between 1.43 and 2, depending on the size of the initial wave packet.