Motivated by the problem of finding explicit q-hypergeometric series which give rise to quantum modular forms, we define a natural generalization of Kontsevich's "strange" function. We prove that our generalized strange function can be used to produce infinite families of quantum modular forms. We do not use the theory of mock modular forms to do so. Moreover, we show how our generalized strange function relates to the generating function for ranks of strongly unimodal sequences both polynomially, and when specialized on certain open sets in C. As corollaries, we reinterpret a theorem due to Folsom-Ono-Rhoades on Ramanujan's radial limits of mock theta functions in terms of our generalized strange function, and establish a related Hecke-type identity.
We study the entanglement properties of quantum phases of bosonic 1d lattice systems in infinite volume. We show that the ground state of any gapped local Hamiltonian is Short-Range Entangled: it can be disentangled by a fuzzy analog of a finite-depth quantum circuit. We characterize Short-Range Entangled states in terms of decay properties of their Schmidt coefficients. If a Short-Range Entangled state has symmetries, it may be impossible to disentangle it in a way that preserves the symmetries. We show that in the case of a finite unitary symmetry G the only obstruction for the existence of a symmetry-preserving disentangler is an index valued in degree-2 cohomology of G. We show that two Short-Range Entangled states are in the same phase if and only if their indices coincide.
We study two 2-dimensional Teichmüller spaces of surfaces with boundary and marked points, namely, the pentagon and the punctured triangle. We show that their geometry is quite different from Teichmüller spaces of closed surfaces. Indeed, both spaces are exhausted by regular convex geodesic polygons with a fixed number of sides, and their geodesics diverge at most linearly.
Kubo's canonical correlation functions (canonical correlators) describe the static response of a system in equilibrium to infinitesimal local perturbations. Knowing their decay properties with respect to spatial distance is important for many theoretical and experimental applications. For a thermal state of a system with short-range interactions, we prove that any knowledge of the decay rate of ordinary correlators readily translates into that of canonical correlators. As the former have been extensively studied, our result can lead to many new results on the latter.
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