An exact mapping between the states of arbitrary N-level quantum systems and the positions of classical coupled oscillators

TL;DR

This paper establishes an exact classical analogy for N-level quantum systems using coupled oscillators, enabling visualization and analysis of quantum dynamics through classical mechanics.

Contribution

It generalizes the classical-quantum mapping to arbitrary N-level systems, reducing the number of oscillators needed and providing a direct method to derive classical couplings from quantum Hamiltonians.

Findings

Exact classical models for quantum states and dynamics.

Linear scaling of oscillators with N for Schrodinger states.

Classical systems can visualize and analyze quantum behavior.

Abstract

The dynamics of states representing arbitrary N-level quantum systems, including dissipative systems, can be modelled exactly by the dynamics of classical coupled oscillators. There is a direct one-to-one correspondence between the quantum states and the positions of the oscillators. Quantum coherence, expectation values, and measurement probabilities for system observables can therefore be realized from the corresponding classical states. The time evolution of an N-level system is represented as the rotation of a real state vector in hyperspace, as previously known for density matrix states but generalized here to Schrodinger states. A single rotor in n dimensions is then mapped directly to n oscillators in one physical dimension. The number of oscillators needed to represent N-level systems scales linearly with N for Schrodinger states, in contrast to N^2 for the density matrix formalism. Although the well-known equivalence (SU(2), SO(3) homomorphism) of 2-level quantum dynamics to a rotation in real, physical space cannot be generalized to arbitrary N-level systems, representing quantum dynamics by a system of coupled harmonic oscillators in one physical dimension is general for any N. Values for the classical coupling constants are readily obtained from the system Hamiltonian, allowing construction of classical mechanical systems that can provide visual insight into the dynamics of abstract quantum systems as well as a metric for characterizing the interface between quantum and classical mechanics.