We consider the one-particle Schrödinger operator in two dimensions
with a periodic potential and a strong constant magnetic field
perturbed by slowly varying, nonperiodic scalar and vector potentials
and
for
. For
each isolated family of magnetic Bloch bands we derive an effective Hamiltonian that
is unitarily equivalent to the restriction of the Schrödinger operator to a
corresponding almost invariant subspace. At leading order, our effective
Hamiltonian can be interpreted as the Peierls substitution Hamiltonian widely used
in physics for nonmagnetic Bloch bands. However, while for nonmagnetic
Bloch bands the corresponding result is well understood, both on a heuristic
and on a rigorous level, for magnetic Bloch bands it is not clear how to
even define a Peierls substitution Hamiltonian beyond a formal expression.
The source of the difficulty is a topological obstruction: in contrast to the
nonmagnetic case, magnetic Bloch bundles are generically not trivializable. As a
consequence, Peierls substitution Hamiltonians for magnetic Bloch bands turn out
to be pseudodifferential operators acting on sections of nontrivial vector
bundles over a two-torus, the reduced Brillouin zone. Part of our contribution
is the construction of a suitable Weyl calculus for such pseudodifferential
operators.
As an application of our results we construct a new family of canonical one-band
Hamiltonians
for magnetic Bloch bands with Chern number
that generalizes the
Hofstadter model
for
a single nonmagnetic Bloch band. It turns out that
is isospectral
to
for
any
and all spectra agree with the Hofstadter spectrum depicted in his
famous (black and white) butterfly. However, the resulting Chern
numbers of subbands, corresponding to Hall conductivities, depend
on
and
,
and thus the models lead to different colored butterflies.
Keywords
Schrödinger equation, magnetic field, periodic potential,
Bloch bundle