“…Advances in laser technology have led to the emergence of high-power Ti:Sa laser systems [1][2][3][4][5][6][7][8][9] that are able to deliver laser pulses up to several PW at a high-repetition rate of 0.05 Hz to 1 Hz. In principle, these systems allow for the generation of secondary sources that exist in a wide range, from ionizing radiation [10][11][12][13] to XUV-and THzpulses [14][15][16][17], as well as current pulses [18] when they are focused to relativistic intensities. Recent developments toward high-repetition-rate ion sources [19,20] have aimed at the generation of pulsed, bright ion beams by well-known mechanisms such as Target Normal Sheath Acceleration (TNSA) [21,22], Radiation Pressure Acceleration [23], etc.…”