Fig. 1. Quasi-probability distribution function of coherent state light and BSV light fields

Fig. 2. Photoelectron energy spectra of hydrogen atoms driven by a laser field in coherent state light and BSV light. In the simulation, the driving light has an intensity of I=5.6×10¹³ W/cm², a wavelength of λ=400nm, 12 cycles, and envelope form of sin²（·）

Fig. 3. Photoelectron momentum distribution of hydrogen atoms driven by a laser field in different quantum states. (a) Coherent state light; (b) BSV light

Fig. 4. Photoelectron ionization rate of hydrogen atom. (a) Ionization rate as a function of the electric field intensity; (b) final ionization rate of hydrogen photoelectrons varied with electric field intensity under different quantum lights

Fig. 5. Photoelectron energy spectra of hydrogen atoms driven by a 800 nm wavelength laser field in coherent state light and BSV light

Fig. 6. Photoelectron ionization rate of hydrogen atom under 800 nm wavelength laser. In the simulation, the driving light has an intensity of I=5.6×10¹³ W/cm², 6 cycles, and envelope form of sin²（·）. (a) Ionization rate as a function of electric field intensity; (b) final ionization rate of hydrogen photoelectrons varied with electric field intensity under different quantum lights

Fig. 7. Photoelectron momentum distribution of hydrogen atoms driven by a 800 nm wavelength laser field in different quantum states. (a) Coherent state light; (b) BSV light