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arXiv:1112.6026 · The European Physical Journal D

Quantum-mechanical effects in a linear time-dependent potential

S. V. Mousavi

Published Dec 22, 2009• 2 citations
arXivHTMLPDF
DOI
10.1140/epjd/e2009-00318-y

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We calculate the frame potential for Brownian clusters of NNN spins or fermions with time-dependent all-to-all interactions. In both cases the problem can be mapped to an effective statistical mechanics problem which we study using a path integral approach. We argue that the kkkth frame potential comes within εεε of the Haar value after a time of order t∼kN+klog⁡k+log⁡ε−1t \sim k N + k \log k + \log ε^{-1}t∼kN+klogk+logε−1. Using a bound on the diamond norm, this implies that such circuits are capable of coming very close to a unitary kkk-design after a time of order t∼kNt \sim k Nt∼kN. We also consider the same question for systems with a time-independent Hamiltonian and argue that a small amount of time-dependent randomness is sufficient to generate a kkk-design in linear time provided the underlying Hamiltonian is quantum chaotic. These models provide explicit examples of linear complexity growth that are also analytically tractable.
In this paper I have drawn out the steps to be followed in order to derive the exact Schr\"odinger wave function for a particle in a general one-dimensional time-dependent linear potential. To this end I have used the so-called Lewis and Riesenfeld invariant method, which is based on finding an exact quantum-mechanical invariant in whose eigenstates the exact quantum states are found. In particular, I have obtained the wave functions of a particle in the linear potential well, driven by a monochromatic electric field.