The recent developments in topological insulators have highlighted the important role of topology in defining phases of matter (for a concise summary, see Chapter 1 in this volume). Topological insulators are classified according to the qualitative properties of their bulk band structure; the physical manifestations of this band topology are special surface states 1 and quantized response functions 2 . A complete classification of free fermion topological insulators that are well defined in the presence of disorder has been achieved 3,4 , and their basic properties are well understood. However, if we loosen these restriction to look beyond insulating states of free fermions, do new phases appear? For example, are there topological phases of free fermions in the absence of an energy gap? Are there new gapped topological phases of interacting particles, for which a band structure based description does not exist? In this chapter we will discuss recent progress on both generalizations of topological insulators.In Part 1 we focus on topological semimetals, which are essentially free fermion phases where band topology can be defined even though the energy gap closes at certain points in the Brillouin zone. We will focus mainly on the three dimensional Weyl semimetal and its unusual surface states that take the form of 'Fermi arcs' 5 as well as its topological response, which is closely related to the Adler-Bell-Jackiw (ABJ) 6 anomaly. The low energy excitations of this state are modeled by the Weyl equation of particle physics. The Weyl equation was originally believed to describe neutrinos, but later discarded as the low-energy description of neutrinos following the discovery of neutrino mass. If realized in solids, this would provide the first physical instance of a Weyl fermion. We discuss candidate materials, including the pyrochlore iridates 5 and heterostructures of topological insulators and ferromagnets 7 . We also discuss the generalization of the idea of topological semimetals to include other instances including nodal superconductors.In Part 2, we will discuss the effect of interactions. First, we discuss the possibility that two phases deemed different from the free fermion perspective can merge in the presence of interactions. This reduces the possible set of topological phases. Next, we discuss physical properties of gapped topological phases in 1D and their classification 8-11 . These include new topological phases of bosons (or spins), which are only possible in the presence of interactions. Finally we discuss topological phases in two and higher dimensions. A surprising recent development is the identification of topological phases of bosons that have no topological order 12,13 . These truly generalize the concept of the free fermion topological insulators to the interacting regime. We describe properties of some of these phases in 2D, including a phase where the thermal Hall conductivity is quantized to multiples of 8 times the thermal quantum 12 , and integer quantum Hall phases of bosons where only...