Download PDF by Ángel S. Sanz: A Trajectory Description of Quantum Processes. I.

By Ángel S. Sanz

ISBN-10: 3642180914

ISBN-13: 9783642180910

ISBN-10: 3642180922

ISBN-13: 9783642180927

Trajectory-based formalisms are an intuitively attractive manner of describing quantum tactics simply because they enable using "classical" ideas. starting at an introductory point compatible for college kids, this two-volume monograph provides (1) the basics and (2) the purposes of the trajectory description of simple quantum strategies. this primary quantity is focussed at the classical and quantum historical past essential to comprehend the basics of Bohmian mechanics, which might be thought of the most subject of this paintings. Extensions of the formalism to the fields of open quantum structures and to optics also are proposed and discussed.

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Extra info for A Trajectory Description of Quantum Processes. I. Fundamentals: A Bohmian Perspective

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3 From Regular to Chaotic Dynamics 21 process can be no longer exponential. More formally, these resonances are defined as the poles of spectral functions and characterize transient behaviors in the time evolution. In nonlinear dynamics, these classical resonances are called Pollicott–Ruelle resoances [51]. 2 Random Walks and Lévy Flights Chaotic dynamics induce some intrinsic randomness in the system. This randomness is generated by the deterministic equation of motion, with no need to introduce any external fluctuation.

Physically, this means that it is not necessary to describe in a very detailed way the deterministic evolution of the adsorbates, but the effect induced by the surface on their positions (or velocities) allows us to accounted for them as Gaussian stochastic variables (see Appendix B). As a consequence, particles exhibit a Brownian motion. 51)—processes where particles do not undergo a Brownian motion—are generically called anomalous diffusion processes. 51) is replaced by |x(t) − x(0)|2 ∼ Dα t α .

These particles are also coupled through another linear force with constant κ12 . 101b) respectively. 102) with eigenfrequencies given by ω− = κ , ω+ = m κ + 2κ12 . 103) 36 1 From Trajectories to Ensembles in Classical Mechanics The displacements x1 and x2 can be therefore expressed as a linear combination of two motions, with frequencies ω− and ω+ . The motion with frequency ω− is called the symmetric mode, η− = x1 + x2 , because both particles oscillate in the same direction (in phase). On the other hand, ω+ gives rise to the so-called antisymmetric mode, η+ = x1 −x2 , because of their oscillation in opposite directions (out of phase).

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A Trajectory Description of Quantum Processes. I. Fundamentals: A Bohmian Perspective by Ángel S. Sanz


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