“…While the pulse duration of a typical few-cycle pulse is IR ≃ 5 fs (the period IR of an optical cycle for 800 nm radiation is IR = 2.7 fs), its oscillating field, controlled to within a small fraction of one radian, offers a convenient route to attosecond time resolution. The three different approaches utilized so far, linear momentum attosecond streaking with linearly polarized IR fields Drescher et al, 2001;Kienberger et al, 2004;Sansone et al, 2006;Cavalieri et al, 2007;Schultze et al, 2010;Sabbar et al, 2015), angular streaking ("attoclock"; Eckle et al, 2008a,b;Pfeiffer et al, 2011aPfeiffer et al, ,b, 2013 with circularly polarized IR fields, and the interferometric RABBIT technique (Paul et al, 2001;Toma and Muller, 2002;Mauritsson et al, 2005;Swoboda et al, 2010;Klünder et al, 2011;Guénot et al, 2012Guénot et al, , 2014Palatchi et al, 2014), have in common that the IR field probes the evolution during the emission, as implied by Eq. (2.18), without, however, necessarily performing a projective measurement which would lead to the "collapse of the wavepacket", i.e., to the reduction of the density operator.…”