Optical fibers represent efficient and compact photonic devices for the transportation of light, with widespread use in numerous areas and emerging applications particularly within bioanalytics and quantum technology that demand to shape the light at the fiber end. A relevant challenge is to focus light remotely without bulk optical components, which is difficult to achieve using fibers with flat end faces. This example emphasizes the importance of functionalizing fiber end faces, which is currently addressed by technologies such as focused ion beam milling, [1] 3D printing, [2] self-assembly, [3] or microstructuring the interior of fibers. [4] Recently, wafer-compatible planarization strategies were introduced to use electron beam lithography (EBL) within the context of fiber functionalization. This has allowed, for instance, boosting light incoupling efficiencies into the fiber modes by orders of magnitude via periodic metallic or dielectric nanostructures. [5,6] The advantage of our EBL approach compared with other patterning methods is that it is a wellestablished technology within the context of nanostructure implementation, which is scalable to larger areas (i.e., bundles of many fibers), technologically flexible in terms of the actual implementation strategy, and customizable for more sophisticated material combinations.A recently introduced scheme to tailor the properties of light beams relies on metasurfaces (MSs). [7][8][9][10][11][12][13][14] These ultraflat nanoscale elements represent a promising approach to shape light fields in an unprecedented manner via managing their scattering properties. MSs are typically realized by well-established nanostructuring technologies (e.g., EBL) in combination with dry or wet etching and consist of ensembles of subwavelength scatterers with nanometer dimensions having well-controlled interelement phase relations and scattering amplitudes. By tuning the properties of the individual element, a superposition of the scattered waves of all elements of the entire ensemble-an Ansatz associated with Huygens' principle-leads to an unprecedented freedom regarding beam shaping. The operation principle of a MS can be understood on the basis of the generalized law of refraction, [7] which includes the MS by an additional phase ΔΦ that contributes to the wave passing through this surface. This phase reveals an in-plane spatial distribution ΔΦ ¼ ΔΦðx, yÞ across the area of the MS, allowing for applications such as cylindrical and spherical lenses, [10,[15][16][17] generation of orbital angular momentum states, [18][19][20] or sophisticated polarization and beam control. [21] Therefore, the combination of optical fibers with MSs represents a promising approach to