The topology of a single-particle band structure plays a fundamental role in understanding a multitude of physical phenomena. Motivated by the connection between quantum walks and such topological band structures, we demonstrate that a simple time-dependent, Bloch-oscillating quantum walk enables the direct measurement of topological invariants. We consider two classes of one-dimensional quantum walks and connect the global phase imprinted on the walker with its refocusing behavior. By disentangling the dynamical and geometric contributions to this phase we describe a general strategy to measure the topological invariant in these quantum walks. As an example, we propose an experimental protocol in a circuit QED architecture where a superconducting transmon qubit plays the role of the coin, while the quantum walk takes place in the phase space of a cavity.Much like their classical stochastic counterparts, discrete-time quantum walks [1] have stimulated activity across a broad range of disciplines. In the context of computation, they provide exponential speedup for certain oracular problems and represent a universal platform for quantum information processing [2][3][4]. Quantum walks also exhibit features characteristic of a diverse set of physical phenomena, ranging from localization to molecule formation [5,6]. At their core, discrete-time quantum walks (DTQW) are dynamical protocols associated with spinful particles on a lattice, where the internal spin state controls the direction of motion [5][6][7][8][9][10][11][12][13][14][15][16][17][18][19]. Motivated by this intrinsic spin-orbit coupling, a tremendous body of recent work has focused on exploring the topological features of DTQWs both theoretically and experimentally [5,[11][12][13][14][15].A connection between quantum walks and topology has been made by mapping the unitary evolution of the DTQW protocol to stroboscopic evolution under an effective Hamiltonian. In certain cases-distinguished by a combination of symmetry and dimensionality-the effective Hamiltonian's bandstructure exhibits a quantized invariant, analogous to those found in topological insulators [5,11,12,14]. On one hand, these invariants have helped to enable a sharp classification of non-interacting topological phases, which unlike conventional symmetry breaking phases, do not exhibit any local order parameters [20,21]. On the other, they underly a multitude of exotic physical phenomena ranging from protected edge modes and quantized conductance to fractional charges and magnetic monopoles [22,23]. Despite their importance and owing to their non-locality, bulk topological invariants have been directly probed in only a handful of quantum optical systems [24][25][26][27] and a generic blueprint for their measurement remains an outstanding challenge.In this Letter, we demonstrate that the simulation platform associated with discrete-time quantum walks is naturally suited for the direct extraction of topolog- ical invariants. We analyze a time-dependent,"Blochoscillating" generalization of t...