It is customary to couple a quantum system to external classical
fields. One application is to couple the global symmetries of the system
(including the Poincaré symmetry) to background gauge fields (and a
metric for the Poincaré symmetry). Failure of gauge invariance of the
partition function under gauge transformations of these fields reflects
’t Hooft anomalies. It is also common to view the ordinary (scalar)
coupling constants as background fields, i.e. to study the theory when
they are spacetime dependent. We will show that the notion of ’t Hooft
anomalies can be extended naturally to include these scalar background
fields. Just as ordinary ’t Hooft anomalies allow us to deduce dynamical
consequences about the phases of the theory and its defects, the same is
true for these generalized ’t Hooft anomalies. Specifically, since the
coupling constants vary, we can learn that certain phase transitions
must be present. We will demonstrate these anomalies and their
applications in simple pedagogical examples in one dimension (quantum
mechanics) and in some two, three, and four-dimensional quantum field
theories. An anomaly is an example of an invertible field theory, which
can be described as an object in (generalized) differential cohomology.
We give an introduction to this perspective. Also, we use Quillen’s
superconnections to derive the anomaly for a free spinor field with
variable mass. In a companion paper we will study four-dimensional gauge
theories showing how our view unifies and extends many recently obtained
results.