We propose a realistic scheme to detect topological edge states in an optical lattice subjected to a synthetic magnetic field, based on a generalization of Bragg spectroscopy sensitive to angular momentum. We demonstrate that using a well-designed laser probe, the Bragg spectra provide an unambiguous signature of the topological edge states that establishes their chiral nature. This signature is present for a variety of boundaries, from a hard wall to a smooth harmonic potential added on top of the optical lattice. Experimentally, the Bragg signal should be very weak. To make it detectable, we introduce a "shelving method", based on Raman transitions, which transfers angular momentum and changes the internal atomic state simultaneously. This scheme allows to detect the weak signal from the selected edge states on a dark background, and drastically improves the detectivity. It also leads to the possibility to directly visualize the topological edge states, using in situ imaging, offering a unique and instructive view on topological insulating phases. [2] have been realized for ultra cold atoms using suitably arranged lasers that couple different internal states [3]. This opens the path to the experimental investigation of topological phases, such as quantum Hall (QH) states, topological insulators and superconductors, in a clean and highly controllable environment [4,5]. Topological phases currently attract the attention of the scientific community for their remarkable properties, such as dissipationless transport and quantized conductivities [6,7]. In this context, the recent experimental realization of a staggered magnetic field in a 2D optical lattice, exploiting laser-induced gauge potentials, constitutes an important step in the field [8] (cf. also [9,10]). In the near future, large uniform magnetic flux should be reachable using related proposals [9][10][11][12], allowing optical-lattice experiments to explore the Hofstadter model [13]. The latter is the simplest tight-binding lattice model exhibiting topological transport properties: well-separated energy bands are associated to non-trivial topological invariants, the Chern numbers, leading to a quantized Hall conductivity when the Fermi energy is located in the bulk gaps [14,15]. These transport properties are directly related to the existence of chiral edge states: while bulk excitations remain inert, these gapless states carry current along the edge of the system. According to the bulk-edge correspondence [16,17], the Chern numbers characterizing the bulk bands determine the number of edge excitations and their chirality, which protects the edge transport against small perturbations.In view of the experimental progress [8][9][10], an important issue is to identify observables that provide unambiguous signatures of topological phases in a cold-atom framework [18][19][20][21][22][23][24][25][26][27]. This is a crucial topic from an experimental point of view: Measuring the Hall conductivity is more difficult than for solid-state systems due to the absenc...