We study numerically the one-dimensional Kondo and Hund lattices consisting of localized spins interacting antiferro or ferromagnetically with the itinerant electrons, respectively. Using the Density Matrix Renormalization Group we find, for both models and in the small coupling regime, the existence of new magnetic phases where the local spins order forming ferromagnetic islands coupled antiferromagnetically. Furthermore, by increasing the interaction parameter |J| we find that this order evolves toward the ferromagnetic regime through a spiral-like phase with longer characteristic wave lengths. These results shed new light on the zero temperature magnetic phase diagram for these models. The interplay between charge and spin degrees of freedom in strongly correlated systems has triggered enormous interest in recent years due to the rich variety of phases found in a plethora of compounds. Charge and spin superstructures with a doping dependent wavevector were found for example in La 2−x Sr x NiO 4 using neutron scattering 1 and electron diffraction 2 . Stripe formation together with incommensurate spin fluctuations in High-Tc superconductors can also be regarded as a manifestation of similar phenomena 3 as well as the charge and spin ordering found in many of the doped manganese perovskites. Another large group of compounds, the heavy fermion materials, present various types of ground states including antiferromagnetically ordered states, the normal heavy fermion state as well as superconducting and insulating phases. Heavy-fermion systems and Kondo insulators are typical examples of systems in which the interactions between conduction electrons and quantum localized spins are essential 4,5 . Their physical properties result from an antiferromagnetic coupling J between these two types of particles, the so-called Kondo lattice model (KLM). The corresponding Hamiltonian has the well-known form:The first term represents the conduction electron hopping between nearest-neighbor sites, c † iσ ( c iσ ) being standard creation (annihilation) operators. In the second term the exchange interaction J is antiferromagnetic (J < 0), andIt is interesting to note that, in recent years, the same model Hamiltonian with ferromagnetic coupling (J > 0) has been considered to contain the basic physics of manganites exhibiting the "colossal" magnetoresistance effect 6,7,8,9 . In this case, both localized spins and itinerant electrons originate from manganese d-states. The system is assumed to contain essentially Mn 4+ ions with three localized t 2g orbitals represented as local spins S i and additional itinerant electrons in the e g orbital. Due to the strong Hund coupling the spin of the e g electron is constrained to be parallel to the local spin on that site. Hund's rule together with the hopping term give rise to the "double-exchange" (DE) interaction that favors ferromagnetic ordering of the local spins 10 . In recent literature this model is often referred to as the ferromagnetic Kondo lattice (FKLM), however to avoid confusion ...