patterns. However, they are limited in terms of combining materials, the typical crystallinity of the materials is usually poor, and 3D geometries such as spheres, nanostars, or core-shells are impossible or impractical to obtain. Electrochemical growth of NPs allows the fabrication of 3D geometries such as nanoflowers, but with limited possibilities of pattern design, material combination, and choice of substrate. [14][15][16] On the other hand, colloidal chemistry offers enormous versatility to obtain NPs with different shapes, compositions, and sizes by modulating the synthesis conditions. [17,18] Plasmon-driven reactions use light as an additional degree of freedom to tune the final morphology and size of colloidal metallic NPs. [19] For example, plasmon-driven reduction of Ag + has been used to produce colloidal Ag NPs of various shapes from Ag spherical seeds, [20,21] as well as Au@Ag coreshell NPs from Au seeds. [22] Then, the challenge of how to bring the colloidal NPs from the liquid phase to specific positions of a substrate remains.The simplest way to attach colloidal NPs to substrates is through electrostatic deposition, but obtaining ordered arrays is not possible this way. [23] Ordered arrays of NPs can be obtained by self-assembly methods, but the versatility is limited to their thermodynamically most stable configurations. [24] Templateassisted self-assembly adds flexibility of pattern design but requires additional steps than lengthen and complicate the fabrication procedure. [25,26] Maximum flexibility can be obtained by methods that utilize an AFM tip [27] or focused laser light [28] to drive deposition in specific regions of the substrate. In general, combining different NPs with all these methods remains a challenge.An emerging method to deposit colloidal NPs in predefined positions of a substrate with high accuracy and flexibility of pattern design is optical printing. [29][30][31][32][33][34] The technique is based on optical forces and allows the printing of virtually any kind of NP that interacts with light. This technique is also able to selectively print subpopulations of NPs out of a polydisperse suspension. [33,35] An appealing route for tailoring the optical properties of individual supported NPs is to perform controlled plasmondriven growth reactions on them. For example, the reduction of silver ions on Ag NPs, [36] the reduction of aqueous PtCl 4 2− on Au NPs, [37] and the copper oxide reduction on Cu NPs [38] were demonstrated by this approach. Also, supported Au nanoprisms,The morphology and composition of metallic nanoparticles (NPs) determine their optical response, so finely controlling them at the single particle level is the key to achieve tailored functionalities. Here, the control of plasmondriven growth of Au NPs is studied by live monitoring their photoluminescence emission in a closed-loop. It is found that the final emission maximum of single NPs can be tuned between 550 and 580 nm with a precision of 2-3 nm, and that the tuning is also reflected in their scattering ma...