SIESTA (Second Ion Experiment for Sputtering and TDS Analysis) is a high-current ion source for erosion and retention studies with focus on wall materials for fusion devices. The system is composed of a DuoPIGatron type ion source, three consecutive grids for ion extraction as well as acceleration and beam focusing, a differential pumping stage, a dipole magnet for mass filtering, a quadrupole doublet lens, a target chamber, a load-lock and a chamber for thermal desorption spectrometry. The potential of the source can be varied between 200 V and 10 kV. The target chamber has a base pressure of 10 −8 mbar, and an operating pressure of 10 −7 − 10 −6 mbar. The target can be rotated to study angle-dependent effects, heated via electron-impact heating up to 1300 K for high temperature erosion and implantation studies. The target chamber is equipped with an in-situ magnetic suspension balance. The operating parameters of the ion source were mapped to achieve the maximum ion current at the target for various gas species and accelerating potentials. The beam emittance for a D + 3 ion beam was measured after deflection in the dipole magnet. This was used for ion beam simulations, which aided the design of the quadrupole lenses. If the quadrupole doublet is used, the ion flux to the target is increased by up to a factor of 4. Additionally, the relative population of neutral particles present in the beam at the target was quantified. The typical beam footprint at the target under normal incidence has an area of 0.5 cm 2. The ion current reaching the target increases with the accelerating potential. Due to this effect, the ion flux density at the target in the low-ion-impact-energy range can be increased by operating the source at a higher extraction potential and by applying a (decelerating) potential to the target, rather than directly operating the ion source at a lower potential. Ion impact energies as low as 200 eV/D are achieved this way with a D + 3 current of 100 µA when focusing the beam with the quadrupole doublet lens, equating to an ion flux density of 3.7 × 10 19 m −2 s −1 with a beam footprint of approximately 0.5 cm 2. At ion impact energies of 2 keV/D, the maximum achievable flux density with D + 3 is 6 × 10 19 m −2 s −1. Experimental determination of sputter yields was performed via in-vacuo and ex-situ weight loss measurement for bulk Au samples, showing reasonably good agreement with simulations and experimental data from literature.