A particle with charge $q$ in a magnetic field $B$ perpendicular to its momentum $p$ will have a circular trajectory with radius $R$, and this relation should hold $$ p = qRB $$
and in the relativistic limit $p \simeq E/c$ thus $$ \frac{E}{c} = q R B \implies B = \frac{E}{qRc} $$ which I assume will hold for SI units so
$$ B(T) = \frac{E(J)}{q(C)R(m)c(m/s)} $$
now my textbook reference and lecture slides say that if we want to use this formula with practical and useful dimensions, it turns into this $$ B(T) = \frac{E(GeV)}{0.3 R(m)} $$ assuming that $q=|e|$.
I was not able to reproduce this conversion, it seems rather simple and I do know how to convert from $eV$ to $J$ and such, but somehow it does not work in the end. If someone could show the steps explicitly it would be very useful