How the geometry of electron
wavefunctions underlies topological effects in metals.
An electron moving through a crystal ceases to be a
featureless point particle and acquires structure within
the unit cell, with far-reaching consequences.In insulators,
these include the existence of topological phases with
quantized transport properties. The same concepts have turned
out to be useful in understanding metals, including two newly
discovered classes of three-dimensional materials (Weyl and
Dirac semimetals) that generalize the famous massless
electronic structure of graphene. We discuss how some
long-standing observations of optical properties may actually
have a topological origin, which would explain some mysterious
properties of the optical activity of quartz. The last part of
the talk explains how a classic piece of physics in metals,
"the orthogonality catastrophe" that determines the absorption
spectrum of X-rays, becomes modified in the presence of
topological excitations.