Download Classical Trajectory Perspective of Atomic Ionization in by Jie Liu PDF
By Jie Liu
The ionization of atoms and molecules in robust laser fields is an energetic box in glossy physics and has flexible functions in comparable to attosecond physics, X-ray iteration, inertial restricted fusion (ICF), clinical technological know-how and so forth. Classical Trajectory standpoint of Atomic Ionization in powerful Laser Fields covers the elemental innovations during this box and discusses many attention-grabbing issues utilizing the semiclassical version of classical trajectory ensemble simulation, that is some of the most profitable ionization versions and has some great benefits of a transparent photograph, possible computing and accounting for plenty of beautiful experiments quantitatively. The booklet additionally provides many functions of the version in such subject matters because the unmarried ionization, double ionization, impartial atom acceleration and different well timed concerns in robust box physics, and provides worthy messages to readers with offering the classical trajectory viewpoint at the powerful box atomic ionization. The publication is meant for graduate scholars and researchers within the box of laser physics, atom molecule physics and theoretical physics. Dr. Jie Liu is a professor of Institute of utilized Physics and Computational arithmetic, China and Peking University.
Read or Download Classical Trajectory Perspective of Atomic Ionization in Strong Laser Fields: Semiclassical Modeling PDF
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Extra info for Classical Trajectory Perspective of Atomic Ionization in Strong Laser Fields: Semiclassical Modeling
Its percentage over the total NSDI events increases monotonically as the laser intensity decreases. 17U p − |I p2 |. Here, Er and E s denote the energy of returned electron and struck electron after recollision, respectively. , min(Er /4, E s /4) ≥ Vb . Obviously, the solution of the above 44 3 Double Ionization in Strong Laser Fields Fig. 6 Percentile map for doubly ionizing trajectories at three different laser intensities. All trajectories are classified into two categories based on whether the inner electron is freed through RIDI (hatched area) or RIET (color-filled area).
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The binding energies of the Rybderg states are much smaller than the photon energy. Because the classical elliptic orbit frequencies ( 1/a 3/2 ) are much smaller than the laser frequency, the fast oscillating motion driven by laser field can be safely averaged out and the electrons will finally remain on the elliptical orbits (see Fig. 6b). This is analogous to the stabilization condition for the Rydberg atoms in the low-frequency light field [27– 30]. However, in our case, the electrons are released from the ground state through tunneling rather than prepared in the Rydberg states directly, the stringent atomic stabilization can not be observed.