applications in miniaturization of photonic circuits, near-field optics, surface-enhanced spectroscopy, plasmonic antennas and photovoltaics, among others. [1] Conventional SPPs and LSPs occur at the interface between two materials whose real parts of permittivities have opposite signs, for instance, metal/dielectric interfaces at optical frequencies. In this frequency range, however, large dissipative losses are generally expected, which severely limit the performance of these metal-based plasmonic devices. Particularly, when light impinges on deep subwavelength metal nanoparticles, high order sharp LSPs resonances are usually suppressed. On the other hand, metallic losses decrease towards low frequencies and metals behave akin to perfect electric conductors, which screen out electric fields. Consequently, metal/dielectric interfaces do not support surface plasmons at mid-infrared frequencies and below. To mimic the exotic properties of optical plasmons at low frequencies,