Above-threshold ionization

In the case of ATI the photoelectron peaks should appear at

${\displaystyle E_{s}=(n+s)\hbar \omega -W,}$

where the integer n represents the minimal number of photons absorbed, and the integer s represents the number of additional photons absorbed. W is the ionization energy, and ${\displaystyle E_{s}}$ is the electron kinetic energy of the peak corresponding to s additional photons being absorbed.^[3]

It typically has a strong maximum at the minimal number of photons to ionize the system, with successive peaks (known as ATI peaks) separated by the photon energy and thus corresponding to higher numbers of photons being absorbed.^[1][4]

In the non-perturbative regime the bound states are dressed with the electric field, shifting the ionization energy. If the ponderomotive energy of the field is greater than the photon energy ${\displaystyle \omega }$ , then the first peak disappears.^[3]

High intensity ultrashort pulse lasers can create ATI features with 20 or more peaks.^[5] The photoelectron spectrum of electron energies is continuous since actual light sources contain a spread of energies.

• Above threshold ionization photoelectron spectra