Classical stochastic approach to quantum mechanics and quantum thermodynamics
We derive the equations of quantum mechanics and quantum thermodynamics from the assumption that a quantum system can be described by an underlying classical system of particles. Each component $ϕ_j$ of the wave vector is understood as a stochastic complex variable whose real and imaginary parts are proportional to the coordinate and momentum associated to a degree of freedom of the underlying classical system. From the classical stochastic equations of motion, we derive a general equation for the covariance matrix of the wave vector which turns out to be of the Lindblad type. When the noise changes only the phase of $ϕ_j$, the Schrödinger and the quantum Liouville equation are obtained. The component $ψ_j$ of the wave vector obeying the Schrödinger equation is related to stochastic wave vector by $|ψ_j|^2=\langle|ϕ_j|^2\rangle$.