Abstract
The ability to perform attosecond-pump attosecond-probe spectroscopy is a long-standing goal in attosecond science. First pioneering experiments based on high-harmonic generation (HHG) [1-3] and at the free-electron laser LCLS [4] have demonstrated the feasibility of this technique. A widespread application of all-attosecond spectroscopy, however, has so far been hindered by the requirement to build very large setups and by the low repetition rates (10 – 120 Hz) of the respective laser sources.
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