We present a systematic investigation of tunable magnetization dynamics of coupled magnetic nanostructures, arranged in onedimensional arrays of horizontally and vertically coupled linear chains, and in two-dimensional arrays of square artificial spin ice lattice. The spatial distribution of the demagnetization field is markedly sensitive to the lattice arrangement, leading to a significant modification of the collective behavior of static and dynamic properties of the arrays. Using ferromagnetic resonance spectroscopy, the engineering of demagnetizing factors with various lattice arrangements has been established quantitatively.The signature of distinct spin wave modes, spatially localized in the constituent nanomagnets, were observed and tuned by the lattice arrangements and applied field orientation. The experimental results are well complemented with micromagnetic simulations.The arrays of coupled nanomagnets (NMs) have shown multifaceted potential applications in the field of highdensity patterned media 1 , logic devices 2,3 , and microwave filters with magnonic crystals. [4][5][6] The magnetization reversal in magnetic thin films is governed by energetics, primarily consisting of magnetocrystalline anisotropy, the exchange between neighboring spins, and magnetostatic energy. On the contrary, the shape anisotropy or the configurational anisotropy plays a key role to determine the magnetic behavior of a single nanostructure. The geometry of a NM is an important parameter to tune the demagnetization field which is directly proportional to the magnetization. Compared with non-interacting nanomagnets, magnetostatic interactions between the neighboring elements can lead to collective magnetic behavior with complex spin configurations and reversal processes. This effect becomes considerably important when the spacing between the neighboring NMs is less than the lateral dimensions of individual NM and results in the broadening of switching field distribution. [7][8][9] Thus, the geometry of a single NM and the lattice arrangements in an array dominate the collective static and dynamic magnetic properties. Magnetostatic interaction, being long-ranged in nature, enables the design of miniaturized magnetic devices using physically isolated but magnetostatically coupled NMs. The shape anisotropy is important in tuning the non-degenerate magnetic ground states, achieved by applying initializing fields in a specific direction for distinct magnetization dynamics. 10 The stacking sequence of the NMs also becomes a tuning factor of the effective magnetic anisotropy when the shape anisotropy is induced. 11 The reconfigurable microwave properties with bias-field-free operations have been shown with coupled rhomboid NMs, 12 demonstrating the spin wave transmission in arbitrary directions. 13 The change in periodicity and the direction of the stacking sequence in one-dimensional (1D) arrays of ellipsoid linear chains (LC) can also sculpt different remanent states due