Dynamics of position-phase probability density in magnetic resonance

We consider the behaviour of precessional angle (phase) carried by molecules of a diffusing specimen under magnetic fields typical of magnetic resonance experiments. An evolution equation for the ensemble of particles is constructed, which treats the phase as well as the position of the molecules as random variables. This "position-phase (probability) density" (PPD) is shown to encode solutions to a family of Bloch-Torrey equations (BTE) for transverse magnetization density, which is because the PPD is a more fundamental quantity than magnetization density; the latter emerges from the former upon averaging. The present paradigm represents a conceptual advantage, since the PPD is a true probability density subject to Markovian dynamics, rather than an aggregate magnetization density whose evolution is less intuitive. We also work out the analytical solution for suitable special cases.