Multiphoton stripping of atoms appears as the competition between step processes (one-by-one removal of electrons) and direct processes (several electrons being removed at the same time). These two types of processes cannot be distinguished by time or intensity dependence but have quite different coherence properties.
We analyse the processes responsible for the formation of doubly charged ions by multiphoton absorption. A++ ions can be created through two different processes, either by a direct multiphoton absorption from A atoms (A → A++) or by a stepwise process via A + ions (A → A+, A+ → A++). By using a simple theoretical model we discuss the distinction between the two mecanisms : direct process corresponds to a yield of A++ ions proportional to the interaction time while stepwise process corresponds to a yield proportional to the square of the interaction time. We obtain a mathematical definition of the direct process and propose a method to calculate its probability. Quantitative results are presented for the case of the ionization of helium ground state, when double ionization by direct process requires two photons, while stepwise process involves two or three photons. These results can be generalized to more complicated processes. Direct process is expected to be negligible unless the number of photons it requires is smaller than the number of photons involved in stepwise process.
The non linear interaction between an intense laser radiation and atoms leads to ionization through the absorption of N photons from the laser radiation via laser-induced virtual states. The multiphoton ionization rate varies as a function of the laser intensity I as IN. We discuss the two most important effects which govern multiphoton ionization processes : resonance effects and laser-coherence effects. In a moderate laser intensity range (107 - 109 W cm-2) corresponding to the two, three or four-photon ionization of atoms, resonance effects play a dominant role while the photon statistics of the laser radiation are relatively unimportant. On the contrary, in the very high intensity range (1012 - 1013 W cm-2) required to observe large Nth - order ionization processes, coherence effects play a dominant role through N! enhancement in the N-photon ionization rate, while resonance effects are completely damped due to the high laser intensity. We conclude by reviewing the possible applications of multiphoton absorption processes in other fields.
The modification of the quantum properties of coherence of photons through their interaction with matter lies at the heart of the quantum theory of light. Indeed, the absorption and emission of photons by atoms can lead to different kinds of light with characteristic quantum statistical properties. As such, different types of light are typically associated with distinct sources. Here, we report on the observation of the modification of quantum coherence of multiphoton systems in free space. This surprising effect is produced by the scattering of thermal multiphoton wavepackets upon propagation. The modification of the excitation mode of a photonic system and its associated quantum fluctuations result in the formation of different light fields with distinct quantum coherence properties. Remarkably, we show that these processes of scattering can lead to multiphoton systems with subshot-noise quantum properties. Our observations are validated through the nonclassical formulation of the emblematic van Cittert–Zernike theorem. We believe that the possibility of producing quantum systems with modified properties of coherence, through linear propagation, can have dramatic implications for diverse quantum technologies.