The βπ-field is an auxiliary field defined as
βπ=βππ0ββπ
where βπ is the magnetic field and βπ is the magnetization.
βπ satisfies AmpΓ¨reβs law for magnets which is analogous to AmpΓ¨reβs law satisfied by βπ,
however unlike βπ it is not in general divergenceless (ββΓβπ=βββΓβπ).