We have obtained exact analytical expressions in closed form, for the linear modes excited in finite and discrete systems that are driven by a spatially homogeneous alternating field. Those modes are extended for frequencies within the linear frequency band while they are either end-localized or end-avoided for frequencies outside the linear frequency band. The analytical solutions are resonant at particular frequencies, which compose the frequency dispersion relation of the finite system. Introduction.-The calculation of the linear modes which can be excited in finite and discrete systems that are driven by a spatially homogeneous alternating (AC) field is of great interest. That problem arises in the lowamplitude limit of several model equations of physical systems, which are comprised of elements that are either directly or indirectly coupled (i.e., the so called magnetoinductive systems). In that limit, it is a common practice to omit the nonlinear terms ending up with a linear non-autonomous system of equations that accept linear wave solutions called in the following driven linear modes (DLM). Such a linearized problem may arise, for example, from the AC driven Frenkel-Kontorova model 1-3 , which has been widely used to model rf-driven parallel arrays of Josephson junctions (JJs) 4-6 , or from more general models of AC driven anharmonic lattices with realistic potentials 7,8 . It may also arise from models of inductively coupled AC driven rf-SQUID arrays 9-11 , from models of inductively coupled intrinsic Josephson junctions supplied by AC current 12-15 , and also from nonlinear magnetic metamaterial models that are comprised of split-ring resonators placed in an AC magnetic field [16][17][18] . In the latter case, those linear waves are known as (linear) magnetoinductive waves 19,20 , and they have phononlike dispersion curves 21 and many prospects for device applications [22][23][24] . In the present work we present analytical solutions that we have obtained for DLMs in finite and discrete systems, with frequencies either in the linear wave band (LWB) obtained in the usuall way, or outside that band. We find that the former ones are extended modes as it is expected, while the latter ones are either end-localized or end-avoided modes. The results are illustrated using as a paradigmatic example the driven FK chain 2 , which in a standard normalization form reads