Hyper bolic metamaterials (HMMs) have recently gained extensive research attention because of their highly anisotropic structures that lead to metallic behavior in one or two directions and dielectric features in the other(s). HMMs have great potential in applications ranging from fluorescence engineering, [7,8] nanoimaging, [2,9] sub surface sensing, [10] spontaneous [11] and thermal emissions [12,13] to single photon resources. [14] Two typical artificial struc tures including metallic nanowires (NWs) embedded in dielectric matrix (Type I: ε xx , ε yy > 0, ε zz < 0) and dielectric/metallic multi layers (MLs) (Type II: ε xx , ε yy < 0, ε zz > 0) have been shown to present hyperbolic dis persion. [15,16] Based on the hyperbolic dis persion wavelength ranges of interest, plasmonic metals such as Ag, Au, and Cu are among the best candidates in the UVvis region, and transparent conducting oxides (i.e., ITO, AZO) and transitionmetal nitrides (i.e., TiN, ZrN) are alternative plas monic materials in the nearIR wavelength region, while highly doped semiconductors are found to be alternative hyperbolic metamaterials in the midIR and longwavelength regions. [17-19] Different from the typical "topdown" techniques such as electron beam lithography (EBL), [20,21] focused ion beam (FIB), [22,23] and "bottomup" electrochemical templating methods, [24,25] the direct growth of selfassembled oxidemetal hybrid metamaterials in the vertically aligned nanocomposite (VAN) thin film form has been demonstrated as an alternative "bottomup" approach. [26-30] Interestingly, highly tunable optical properties such as localized surface plasmon resonance (LSPR) and hyperbolic dispersion shift in the UV-Vis-NIR wavelength region achieved by varying nanostructure aspect ratios, [31,32] pillar density, [32-34] and substrate selections [35,36] all present enormous potentials for these new class of hybrid thin films. Furthermore, by properly selecting the metal nanopillar phase and oxide or nitride matrix, other novel functionalities such as tunable ferroelectric, ferromagnetic, and magnetoelectric cou pling and thermal stability can also be enabled. [37-41] Very recently, a new 3D framework strain engineering has been demonstrated in oxideoxidebased thin films by stacking Dielectric-metallic hybrid metamaterials exhibit extraordinary optical properties due to the light-matter interactions at the dielectric-metallic interfaces. The ability in precision control of the light-matter interactions in nanoscale is key to tailor the optical properties of hybrid metamaterials. In this work, a complex 3D framework of multilayered self-assembled BaTiO 3 (BTO)-Au hybrid thin films is demonstrated with such precision control of the lightmatter interaction in nanoscale. Unique "bamboo-like" Au nanostructures are formed via the bilayer and trilayer stacking of BTO-Au hybrid layers with interlayers of SrTiO 3 , CeO 2 , or MgO. Different film strain states introduced by the three interlayers result in variable diameter and density of Au nanopillars. Both simulate...