  Weyl semimetals host linear energy dispersions around Weyl nodes, as well as
monopoles of Berry curvature in momentum space around these points. These
features give rise to unique transport signatures in a Weyl semimetal, such as
transverse transport without an applied magnetic field, known as anomalous
transport. The type-II Weyl semimetal, recently experimentally demonstrated in
several materials, is classified by a tilting of the Weyl nodes. This paper
provides a theoretical study on thermoelectric transport in time-reversal
breaking type-II Weyl semimetals. Our results examine the balance between
anomalous and non-anomalous contributions to the Nernst effect when subject to
an external magnetic field. We also show how increasing scattering times have
on enhancing effect on thermoelectric transport in these materials. Since a
temperature-dependent chemical potential has been theoretically shown to be
paramount when considering anomalous transport, we also study how similar
considerations impact the Nernst thermopower in the non-anomalous case.
