We address an imbalanced two-component atomic Fermi gas restricted by a one-dimensional (1D) optical lattice and an external harmonic potential, within the mean-field Bogoliubov-de Gennes formalism. We show that characteristic features of the Fulde-Ferrell-Larkin-Ovchinnikov state are visible in the RF-spectra and in the momentum resolved photoemission spectra of the gas. Specially, Andreev states or mid-gap states can be clearly resolved, which gives a direct experimentally observable signature of the oscillating order parameter.PACS numbers: 03.75. Ss, 78.90.+t, 74.45.+c Experimental realization of spin-density imbalanced Fermi gases [1,2,3] has opened exciting new possibilities to study pairing in systems where matching of spinresolved Fermi surfaces, which is the base of BardeenCooper-Shreffer (BCS) theory, is not valid. Either phase separation or extension of the BCS pairing to some other, exotic mechanism is inevitable. The question is of interest in context of various solid state materials [4,5,6,7] as well as in hight-energy and astrophysics [8]. One of the main candidates for the non-BCS pairing is the so-called Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) state [9,10]. The zero temperature ground state properties of the FFLO state in the context of 1D Fermi gases have been studied extensively within mean-field, exact, and DMRG approaches [11]. The rapid development of experiments on Fermi gases in optical lattices [12,13,14,15] suggests that such systems will be available soon. However, it is not obvious how to observe e.g. the spatially varying order parameter and other characteristics of the FFLO state, although noise correlations have been proposed to provide information about the pairing correlations [16]. In this letter we show how the characteristics of the FFLO state are prominently reflected in RFspectroscopy [17] and in the recently introduced [18] photoemission spectroscopy of Fermi gases. Unlike the BCS, the FFLO state allows population of single-particle excitations even at zero temperature, corresponding to unpaired particles. For a spatially non-uniform order parameter, some of these excitations can be understood as Andreev bound states residing close to the nodes of the order parameter. We show that such excitations produce distinct features in the spectra, at negative energies, and thus provide a signature of oscillations of the order parameter that is easily distinguishable from the usual pairing signatures at positive energies. Furthermore, by calculating spectra also at finite temperatures, we show that such features are uniquely related to oscillations of the order parameter.We consider a two-component attractive Fermi gas confined by an external potential in a 1D lattice with L sites. At low filling, this corresponds to a onedimensional gas without the lattice. Our qualitative results concerning the spectral signatures should be valid in this case as well. We apply a mean-field Bogoliubovde Gennes (BdG) approach. In 1D, long range order is absent and the mean-field approximation is n...