  A method was presented of profiling the magnetic field, with a zero vector of
magnetic flux density $B_{r}$ and strong gradient G, enabling conditions for
the Stern-Gerlach spectroscopy to be accomplished in condensed matter (the
method has been called magnetic field gradient spectroscopy - MGRS), as well
the previously proposed magnetic resonance spectroscopy for selected energy
states (SSMRS). Magnetic field distribution in a model electromagnet were shown
when condition $B_{r}= 0$ for resultant magnetic field was satisfied within the
sample
