The growth of ferromagnetic nanostructures by means of focused-Ga + -beam-induced deposition (Ga + -FIBID) using the Co 2 (CO) 8 precursor has been systematically investigated. The work aimed to obtain growth conditions allowing for the simultaneous occurrence of high growth speed, good lateral resolution, low electrical resistivity, and ferromagnetic behavior. As a first result, it has been found that the competition between deposition and milling that is produced by the Ga + beam is a limiting factor. In our working conditions, with the maximum available precursor flux, the maximum deposit thickness has been found to be 65 nm. The obtained volumetric growth rate is at least 50 times higher than in the case of deposition by focused-electron-beam-induced deposition. The lateral resolution of the deposits can be as good as 50 nm while using Ga + -beam currents lower than 10 pA. The high metallic content of the as-grown deposits gives rise to a low electrical resistivity, within the range 20-40 µΩ·cm. Magnetic measurements confirm the ferromagnetic nature of the deposits at room temperature. In conclusion, the set of obtained results indicates that the growth of functional ferromagnetic nanostructures by Ga + -FIBID while using the Co 2 (CO) 8 precursor is a viable and competitive technique when compared to related nanofabrication techniques. Nanomaterials 2019, 9, 1715 2 of 12 magnetic resonance force microscopy, in sharp contrast to other nanofabrication techniques requiring resists [19]. Other reported applications of magnetic FEBID deposits comprise nanoactuation [20], domain-wall pinning [21], nano-Hall sensors [22], nanomagnetic logic [23], superconducting-vortex pinning [24,25], etc. In addition, the capability of FEBID for the growth of complex three-dimensional (3D) magnetic structures is being explored in the rising field of 3D nanomagnetism [26].FEBID has long suffered from two disadvantages when compared to other nanofabrication techniques: the material purity and the growth speed. In the last years, various growth strategies and post-growth purification treatments have been successfully developed to enhance the material purity of magnetic deposits that are grown by FEBID [27][28][29][30][31][32]. However, the growth speed of magnetic nanostructures by FEBID continues to be a bottleneck regarding its broader use. Existing literature on the topic indicates that the volumetric growth rate of nanostructures with the widely-used Co 2 (CO) 8 precursor is in the range of 0.002 µm 3 /nC [33]. Low electron currents must be used to obtain magnetic structures with good lateral resolution (below 1 nA), which gives rise to long growth times. As an example, the growth of a 100 nm-thick 1 µm 2 -rectangle takes 8 min. if an electron beam current of 100 pA is used.In the present work, we have systematically explored the possibility of using a Ga + focused ion beam to grow Co magnetic nanostructures with good lateral resolution, low electrical resistance, and high growth speed by means of the Focused Ion Beam Induced De...