The modern semiclassical theory of a Bloch electron in a magnetic field
encompasses the orbital magnetization and geometric phase. Beyond this
semiclassical theory lies the quantum description of field-induced tunneling
between semiclassical orbits, known as magnetic breakdown. Here, we synthesize
the modern semiclassical notions with quantum tunneling -- into a single
Bohr-Sommerfeld quantization rule that is predictive of magnetic energy levels.
This rule is applicable to a host of topological solids with \emph{unremovable}
geometric phase, that also \emph{unavoidably} undergo breakdown. A notion of
topological invariants is formulated that nonperturbatively encode tunneling,
and is measurable in the de-Haas-van-Alphen effect. Case studies are discussed
for topological metals near a metal-insulator transition and over-tilted Weyl
fermions.Comment: 5 pages, 2 figure