We report measurements of Hanbury-Brown and Twiss correlation of coherent light transmitted through disordered one-dimensional photonic lattices. Although such a lattice exhibits transverse Anderson localization when a single input site is excited, uniform excitation precludes its observation. By examining the Hanbury-Brown Twiss correlation for a uniformly excited disordered lattice, we observe intensity anti-correlations associated with photon anti-bunching -a signature of nonGaussian statistics. Although the measured average intensity distribution is uniform, transverse Anderson localization nevertheless underlies the observed anti-correlation. [5][6][7], atoms in cold Fermi gases [8,9], as well as interacting photons in nonlinear media [10]. In typical optical HBT scenarios, such as the original determination of the angular size of the star Sirius A [2], the radiation source is random while the medium transmitting the incoherent wave is deterministic. One might consider an alternative scenario in which a deterministic coherent input probes a scattering medium, which becomes itself the source of randomness. HBT measurements carried out on the emerging partially coherent light can provide insights into the nature of the disorder in the medium.A particularly useful system for testing the impact of disorder on optical statistics is that of evanescently coupled waveguide arrays (or photonic lattices) with randomness introduced in the transverse direction [11]. This setting emulates time evolution of quantum-mechanical waves in time-independent disordered potentials. Indeed, by coupling a coherent input to a single lattice site, Anderson localization [12] has been observed in the transverse direction upon ensemble averaging [13][14][15][16]. Beyond the mean intensity observed in such experiments, unique features of the higher-order field correlations involved in the HBT effect have only recently been explored [17][18][19][20][21][22][23]. Indeed, HBT measurements can distinguish between the so-called 'diagonal' and 'off-diagonal' classes of lattice disorder, whereas such a delineation is not possible by observing the mean field alone [18]. Furthermore, path-entangled photon pairs propagating along such lattices can emulate the quantummechanical waves associated with fermions and bosons [17], and can exhibit co-localization and anti-localization when the illumination is extended [19,21].In this letter, we report measurements of HBT interference in disordered photonic lattices excited uniformly with an extended coherent optical field. Light emerging from such a system is no longer coherent after ensemble averaging. The intensity fluctuations at any site indicate a thermalization of optical statistics [24,25]. Here we measure the correlations between fluctuations at pairs of lattice sites. It is revealed -surprisingly -that at certain separations anti-correlations emerge. This result implies that the optical field exiting the lattice is characterized by non-Gaussian statistics that correspond to photon antibunching....