In this work, properties of 1-dimensional non-analytic potentials involving the absolute value of the coordinate are explored, In the framework of classical and quantum mechanics.
Quantum entanglement, a cornerstone of quantum mechanics, presents a unique challenge to traditional geometric analysis. This paper explores the potential of a non-Planck geometry to provide a deeper understanding of entanglement's non-classical properties, specifically focusing on its geometric implications. We propose a framework built upon quantum entanglement, aiming to reveal previously unacknowledged geometric features. This work seeks to address limitations of existing approaches by incorporating the fundamental entanglement properties directly into the geometric analysis. The core mechanism involves establishing a new geometric tool to analyze entanglement's non-classical behavior. The resulting analysis will pave the way for novel quantum algorithm design and a more complete understanding of entanglement's geometric landscape.
In non-relativistic quantum mechanics, the absolute square of Schrödinger's wave function for a particle in a potential determines the probability of finding it either at a position or momentum at a given time. In classical mechanics the corresponding problem is determined by the solution of Liouville's equation for the probability density of finding the joint position and momentum of the particle at a given time. Integrating this classical solution over either one of these two variables can then be compared with the probability in quantum mechanics. For the special case that the force is a constant, it is shown analytically that for an initial Gaussian probability distribution, the solution of Liouville's integrated over momentum is equal to Schrödinger's probability function in coordinate space, provided the coordinate and momentum initial widths of this classical solution satisfy the minimal Heisenberg uncertainty relation. Likewise, integrating Lioville's solution over position is equal to Schrödinger's probability function in momentum space. Quanta 2017; 6: 53–56.