Author Affiliations
1College of Precision Instrument and Optoelectronics Engineering, Tianjin University, Tianjin 300072, China2Civil Aviation Meteorological Institute, Key Laboratory of Operation Programming & Safety Technology of Air Traffic Management, Civil Aviation University of China, Tianjin 300300, Chinashow less
Fig. 1. Photoelectron momentum distributions in the polarization plane for ionization of hydrogen by right–left circularly polarized attosecond pulses with the ellipitcity (a) η1=1, η2=−1, (b) η1=0.75,η2=−0.75, (c) η1=0.5, η2=−0.5, (d) η1=0.25, η2=−0.25, (e) η1=0, η2=0, which are delayed in time by 2478 as.
Fig. 2. Photoelectron momentum distributions in the polarization plane for ionization of H by right–left circularly polarized attosecond pulses with the ellipitcity (a) η1=1, η2=−1, (b) η1=1, η2=−0.5, (c) η1=0.5, η2=−0.5, (d) η1=0.25, η2=−0.25, (e) η1=0.25, η2=−0.25, which are delayed in time by 2478 as.
Fig. 3. Photoelectron momentum distributions in the polarization plane for ionization of H by right–right circularly polarized attosecond pulses with the ellipitcity (a) η1=η2=1, (b) η1=η2=0.5, (c) η1=0.5, η2=0.25, (d) η1=η2=0.25, which are delayed in time by 2478 as.
Fig. 4. Photoelectron momentum distributions in the polarization plane for ionization of H by a linearly polarized attosecond pulse and a circularly polarized attosecond pulse with the ellipitcity (a) η1=0.5, and (b) η1=1, which are delayed in time by 2478 as.
Fig. 5. Photoelectron momentum distributions in the polarization plane for ionization of H by a right–left elliptically polarized attosecond pulse with the ellipitcity (a)–(c) η1=0.5, η2=−0.5, and (d)–(f) η1=1, η2=−1, delayed in time by (a) and (d) 826 as, (b) and (e) 1652 as, and (c) and (f) 2478 as.