By Yunquan Liu
This quantity offers the newest developments and destiny views of atomic, molecular and optical (AMO) physics and its important position in glossy sciences and applied sciences. The chapters are dedicated to quite a lot of quantum platforms, with an emphasis at the figuring out of ionization, high-harmonic iteration, molecular orbital imaging and coherent keep an eye on phenomena originating from light-matter interactions. The publication overviews present study panorama and spotlight significant medical traits in AMO physics interfacing with interdisciplinary sciences. it can be fairly fascinating for younger researchers engaged on setting up their medical pursuits and goals.
Readership: This publication is most fitted for the energetic scientists and graduates in strong-field neighborhood and likewise for different scientists who paintings with the ultrafast lasers in biology and chemistry.
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Extra resources for Advances of Atoms and Molecules in Strong Laser Fields
The recollision wave packet serves as a signal wave and the non-recollision wave packet serves as a reference wave. Because the reference wave might be the direct trajectory or the indirect trajectory, there will be two forward rescattering holographic interferences. ) One can perform a simulation starting with the classical rescattering model  with further including the interference effect [10, 23, 24] and the weight of each trajectory according to the Ammosov-Delone-Krainov (ADK) tunneling theory [25, 26].
The Pz and P⊥ P⊥ = Px2 + Py2 represent the momentum distribution parallel and perpendicular to the laser polarization direction, respectively. , in the multiphoton ionization regime, the PADs reveal ring-like multiphoton structures. The PADs of molecules reveal similar lowenergy resonant structure at the wavelength of 800 nm [29–31]. At 1320 nm, the PADs of molecules (see the top panels of Fig. 7) are similar to those of atoms at low laser intensities . Interesting, with increasing the laser intensity, an interference stripe structure is enhanced for strong-field ionization of molecules, which is nearly perpendicular to the laser polarization axis.
Førre, Phys. Rev. A 84, 033423 (2011). M. Gavrila, I. Simbotin, and M. Stroe, Phys. Rev. A 78, 033404 (2008); M. Stroe, I. Simbotin, and M. Gavrila, Phys. Rev. A 78, 033405 (2008). L. V. Keldysh, Zh. Eksp. Teor. Fiz. 47, 1945 (1964) [Sov. Phys. JETP 20, 1307 (1965)]. R. V. Kulyagin and V. D. Taranukhin, Laser Phys. 3, 644 (1993). V. P. Gavrilenk and E. Oks, Can. J. Phys. 89, 849 (2011). A. Rudenko, K. Zrost, C. D. Schröter, V. L. B. de Jesus, B. Feuerstein, R. Moshammer, and J. Ullrich, J. Phys.
Advances of Atoms and Molecules in Strong Laser Fields by Yunquan Liu
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