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Optics and Spectroscopy

A collective behavior method in simulation of many-body quantum dynamics

Yu. I. Ozhigov, Al. Y. Ozhigov

Published Jul 1, 2007• 0 citations
Publisher

Abstract

With the help of a collective behavior method, quantum dynamics is represented as a result of mutual transformations of a swarm of classical samples of quantum particles. The method used is shown to generalize the Monte Carlo diffusion method to the case of many-body quantum dynamics. The method is illustrated by the example of the Schrödinger equation. It is shown that the diffusion representation of the Coulomb field linearly simulates a multiparticle system compared to the traditional method of quadratic complexity. A simple method of description of entangled states of any complexity with the help of association reactions of samples of quantum particles is given.

DOI
10.1134/s0030400x07070065

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With the help of a collective behavior method, quantum dynamics is represented as a result of mutual transformations of a swarm of classical samples of quantum particles. The method used is shown to generalize the Monte Carlo diffusion method to the case of many-body quantum dynamics. The method is illustrated by the example of the Schrödinger equation. It is shown that the diffusion representation of the Coulomb field linearly simulates a multiparticle system compared to the traditional method of quadratic complexity. A simple method of description of entangled states of any complexity with the help of association reactions of samples of quantum particles is given.
A straightforward algorithm is proposed for simulating and visualizing nonrelativistic quantum dynamics in terms of the collective behavior of classical particles. In this approach, a quantum particle is treated as a swarm (collection) of its classical samples interacting with one another by simple rules involving the emission and absorption of associated photons. The quantum dynamics is regarded as resulting from the collective behavior of the swarm, and the eigenstates are treated as equilibrium states of the process of photon emission and absorption. Entanglement is seen as classical correlation between samples from distinct swarms; the information on this correlation is stored in a spatiotemporal section of the model inaccessible to the user. Amplitudes are invariably treated as consisting of amplitude quanta. A Coulomb field experienced by quantum particles is represented in a similar manner to the free spreading of a wave packet, by point interaction between the particle samples and the samples of scalar photons propagating by diffusion. This provides a square-root gam in computational speed against the direct method involving item-by-item examination. The approach presented covers decoherence and allows natural generalization to multiparticle quantum electrodynamics, the amount of memory required growing linearly.
The method of collective behavior is based on the representation of real quantum particle by the swarm of classical particles which have all properties of the initial particle but have classical states like coordinates and impulse. Simulation with swarms can be more flexible and powerful than analytical methods because it preserves the methodology of classical description of dynamics. The method of collective behavior is illustrated on the diffusion Monte Carlo way of calculating stationary states of electrons.
The simple algorithm for the simulation and visualization of non relativistic quantum dynamics is proposed that is based on a collective behavior of classical particles. Any quantum particle is represented as the swarm of its classical samples which interact by simple rules including emission and absorption of samples of tied photons. The quantum dynamics results from the collective behavior of such a swarm where the eigenstates are treated as the equilibrium states relatively to emission-absorption of photons. The entanglement is treated as a correlation between samples of the different swarms that is stored in the space-time part of the model inaccessible for a user. The amplitude is always grained. The Coulomb field between quantum particles is simulated, analogously to free flow of quantum package, by the point wise interaction between its samples and scalar photon samples which propagate by diffusion. It gives square root speedup in comparison to each-with-each method. This method obviously includes decoherence and admits the natural generalization on the QED of many particles with the linear computational cost.
A model of entangled quantum states of many bodies using tuples consisting of samples of individual real particles is proposed. This approach generalizes Bohm’s method for complex systems. The dynamics can be described both in the form of quantum hydrodynamics and in the form of dynamic diffusion which is examined in detail in this study. The latter method fundamentally differs from the choice of the grain of spatial resolution and cannot be reduced to differential equations; therefore, it requires direct simulation. The limitation on the number of samples is the fundamental factor causing decoherence, a deviation of the swarm dynamics from the exact solution to the Schrödinger equation. The model complexity is linear with respect to the number of particles.
We develop the constructive viewpoint to quantum theory, which means the using of constructive mathematics as the basic formalism. It is shown how the heuristic of collective behavior leads to the description of complex quantum systems with the inbuilt decoherence on classical computers. Decoherence comes from the finite total number of samples for each quantum particles. When this number converges to infinity, its trajectory converges to the solution of Schrödinger equation. This model rests on the simple rule of the sort of momentum exchange and gives the linear growth of the complexity.
This paper presents a novel methodology for simulating the dynamics of many-body quantum entanglement using quantum dynamics simulation techniques. The core of the approach involves employing quantum Monte Carlo methods to propagate the time evolution of complex many-body quantum systems. Specifically, we calculate the strength and topology of multi-body entanglement during this dynamic process. The developed framework offers a significant advancement in understanding and controlling the intricate behavior of quantum many-body systems, providing a more precise and detailed simulation of entanglement compared to conventional methods. The simulation results are presented, illustrating the method's ability to capture the key features of entanglement dynamics in various quantum systems.