The theory describing quantum smectics in 2 1 dimensions, based on topological quantum melting is presented. This is governed by a dislocation condensate characterized by an ordering of Burger's vector and this ''dual shear superconductor'' manifests itself in the form of a novel spectrum of phononlike modes. DOI: 10.1103/PhysRevLett.97.045701 PACS numbers: 64.60.ÿi, 71.10.Hf, 71.27.+a, 74.20.Mn Different from classical liquid crystals [1,2], the quantum smectic and nematic type orders occurring at zero temperature are far from understood. These came into focus recently, motivated by empirical developments in high T c superconductivity and quantum-Hall systems [3]. Fundamentally, it is about the partial breaking of the symmetries of space itself, and on the quantum level this might carry consequences which cannot be envisaged classically.The ''most ordered'' liquid crystal is the smectic, which can be pictured as lines in two dimensions (or layers in three dimensions) of liquid forming a periodic array in one spatial direction. Emery et al. [4] (for doped Mott insulators) and MacDonald and Fisher [5] (for quantumHall systems), delivered proof of principle that things are different on the quantum level by showing that a twodimensional quantum system can organize spontaneously into an array of one-dimensional metals. Here we will present a description of the quantum smectic which is complementary to these earlier works. It rests on KramersWannier duality [6,7], the field-theoretical fact that the disordered state (the smectic) corresponds to an ordered state (in fact, the Higgs phase) formed from the topological excitations (dislocations) of the ordered state (the crystal), and as such it can be viewed as a quantum extension of the famous Nelson-Halperin-Young [8] theory of twodimensional melting.The theory is completely tractable for a system of bosons living in the 2 1D Galilean invariant continuum [9], in the limit that all characteristic length scales are large compared to the lattice constant. The outcome is a spectrum of propagating long-wavelength collective modes [10], which should have a universal status in the scaling limit. Before discussing the theory, let us first present this mode spectrum. The quantum smectic in (2 1)D is characterized by a ''crystalline'' and an orthogonal ''liquid'' direction [see Fig. 1(d)]. For simplicity we assume that the quantum smectic is associated with a reference crystal described by isotropic quantum elasticity (e.g., a hexagonal crystal) characterized by just a shear ( ) and compression ( ) modulus, and a mass density , such that the longitudinal and transversal phonon velocities are given by c L