devices, [6] and Raman, [7] fluorescence, [8,9] even infrared [10] spectroscopy. Nonetheless, the lack of high-efficiency substrates with uniformly distributed hotspots greatly hinders the widespread and practical application of plasmon-enhanced spectroscopies (PESs), such as plasmon enhanced second harmonic generation (PESHG) and surface-enhanced Raman scattering (SERS). Hence, constructing hotspot platforms with high-efficiency is of great importance. At present, 0D, 1D, and 2D hotspots based on different types of metal nanostructures are the most frequently used enhancement structures, such as 0D single isolated nanospheres, [11] 1D nanowires [12] or nanorods, [13,14] and 2D nanoarrays, [15][16][17][18] synthesized using various nanofabrication techniques. However, these low spatial dimensions limit the number of hotspots that can be generated and thus impede further improvements in the detection sensitivity of PESs.Due to the higher density of hotspots and larger surface area for adsorbing probe molecules, 3D hotspot platforms can give stronger and more stable SERS signals than that of 0D, 1D, or 2D nanostructures. However, the rational design and simple construction of 3D SERS substrates with controllable and reproducible nanoscale hotspots and stronger Raman enhancement factors via a facile and green approach is a longstanding challenge and numerous efforts have been devoted to their fabrication. Ag NP decorated cactus-like 3D SERS substrates [19] and 3D hot-junction formation of gold nanoparticles on 2D silicate nanoplatelets [20] had been designed, which exhibited good reproducibility and considerable SERS signal amplification. Also, it had been demonstrated that SERS enhancements of 3 orders of magnitude could be generated during evaporation of a drop containing pure Ag NPs solution compared with the dried substrate. [21] Unfortunately, the SERS signals were not stable and rapidly decreased after the complete evaporation of water. To alleviate this drawback, aqueous glycerol was added in the Ag NPs sol to slow the evaporation, [22] which extended the duration of maximum Raman signal. However, the Raman signal kept decreasing with time due to charge exchange among aggregated Ag NPs. Considering this charge