photons, incoherent nonlinear processes such as two-photon fluorescence or hyper Raman scattering (HRS) [2] are very weak. Nonresonant HRS, with extremely small cross sections on the order of 10 −65 cm 4 s photon −1 , does not constitute a useful spectroscopic tool, unless molecular resonance is exploited. [3] Nevertheless, since nonlinear, two-photon processes depend on the square of the excitation photon flux density, they benefit extremely from an enhancement by high local optical fields. [4] Thereby, they gain practical importance: Surface enhanced hyper Raman scattering (SEHRS), [5] the spontaneous two-photon excited Raman process occurring in the highly confined electromagnetic fields of plasmonic nanostructures [4c] is a complementary approach to (one-photon excited) surface enhanced Raman scattering (SERS). [6] It provides additional vibrational information due to the different selection rules acting in Raman and HRS. [7] In particular, SEHRS is more sensitive than SERS with respect to molecular orientation and surface environmental changes. [8] Therefore, SEHRS is often used in combination with SERS for the structure elucidation of organic and bioorganic molecules, [8d,9] microenvironmental sensing, [8b,10] and spectroscopic imaging. [11] Obtaining comprehensive vibrational and imaging information by means of SEHRS requires plasmonic nanostructures that provide homogeneous and strong plasmonic enhancement. The morphology of roughened electrodes used in early SEHRS experiments [8a,12] and of typical nanoparticle substrates for SEHRS [8e,13] is controllable only to a limited extent, and the enhancement by nanoparticles is strongly influenced by the presence and interaction of analyte molecules. [13] Well-defined, topdown fabricated plasmonic structures with nanoscale gaps that are used in SERS [14] could be also beneficial for SEHRS experiments. [15] Nevertheless, apart from the requirements of fabrication by lithography, recent theoretical and experimental work [9c,10c,16] indicates that an independent design and optimization of SEHRS substrates would be useful, due to the nonlinear dependence of SEHRS on the excitation field |E(ν L )| 4 |E(2ν L − ν HRS )| 2 and the wide spectral separation of excitation and scattered light.During excitation of incoherent HRS or two-photon fluorescence, also other nonlinear, coherent optical signals can be obtained from a sample. Second-harmonic generation (SHG) is a two-photon process, where a non-centrosymmetric macromolecule or nanostructure yields an effective combination of Nonlinear optical signals benefit greatly from the enhanced local optical fields in the vicinity of plasmonic nanostructures. Gold and silver nanovoid arrays of varying size and thickness, fabricated by electrochemical deposition are shown here to act as stable plasmonic nanostructures and to enhance the weak, incoherent two-photon excited process of surface-enhanced hyper Raman scattering (SEHRS) with high microscopic homogeneity and reproducibility that typical SEHRS experiments...