Super intense laseratom physics lhuillier a piraux bernard rzazewski kazimierz. Super 2019-01-24

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super intense laseratom physics lhuillier a piraux bernard rzazewski kazimierz

The strong field limit of atomic stabilization in ultrashort pulses; M. Energy distribution of two-electron ionization of helium in an intense field; R. Interference stabilization: Λ- and V-schemes, dynamics of ionization, initial coherent population of Rydberg levels and quantum phase control of the ionization yield; M. Nuclear fusion in gases of deuterium clusters and hot electron generation in droplet sprays under irradiation with an intense femtosecond laser; T. Tunnelling ionization and the Franck-Condon principle; J.

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A. L'Huillier & Bernard Piraux: Super

super intense laseratom physics lhuillier a piraux bernard rzazewski kazimierz

Electron momentum distributions for double ionization in the strong field limit; S. Dissociative ionization of few-electron molecules in intense laser fields; D. Strong field Coherent control; P. Computer experiments on atomic stabilization in a strong laser field; A. Under these conditions, very high peak intensities may be obtained and electric fields exceeding typical electron binding fields in atoms are generated.

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Table of contents for Library of Congress control number 2001029076

super intense laseratom physics lhuillier a piraux bernard rzazewski kazimierz

Part I: Double Ionization of Complex Atoms. A semi-classical model for high-harmonic generation; D. Part I: Double Ionization of Complex Atoms. Nuclear fusion in gases of deuterium clusters and hot electron generation in droplet sprays under irradiation with an intense femtosecond laser; T. Dissociative ionization of few-electron molecules in intense laser fields; D. Non-sequential double ionization: a minimal correlation approach; R.

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super intense laseratom physics lhuillier a piraux bernard rzazewski kazimierz

The interaction of such electromagnetic fields with an atomic system has a highly non-linear character which has led to the observation of to­ tally unexpected phenomena. Part V: Stabilization and Relativistic Effects in Super Strong Fields. The strong field limit of atomic stabilization in ultrashort pulses; M. The absorption of energy by large atomic clusters from superintense laser pulses; V. Calculation of double ionization of helium; H. Relativistic energy and angular distribution of electron in the ionization of atoms by super-intense laser radiation; V. Momentum space description of hydrogen atom interacting with a low frequency strong laser field; A.

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super intense laseratom physics lhuillier a piraux bernard rzazewski kazimierz

The interaction of an atom or a molecule with such electromagnetic fields has a highly non-linear character which leads to unexpected phenomena. Library of Congress subject headings for this publication: Laser beams -- Congresses. The rapid development of powerful pulsed lasers is at the origin of a conside- rable interest in studying the response of an atom, a molecule or a solid to a strong electromagnetic field. Angular distributions for double ionization by an ultrashort, intense laser pulse: the case of Li-; G. Two-and-three electron atoms in strong laser fields; P.

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super intense laseratom physics lhuillier a piraux bernard rzazewski kazimierz

Atomic wave packets created by short electric pulses; I. Relativistic effects in the atomic response to super-intense laser pulses; A. The helium atom in strong and short laser pulses: multielectron; H. Interference stabilization: Λ- and V-schemes, dynamics of ionization, initial coherent population of Rydberg levels and quantum phase control of the ionization yield; M. Position dependent tunneling speed for particles under a barrier; P. X-ray generation via stimulated recombination of electrons and Bohr's correspondence principle; A. Dynamics of a two-electron system driven by an ultrashort and intense laser pulse; B.

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super intense laseratom physics lhuillier a piraux bernard rzazewski kazimierz

Beyond the simple maris model for high harmonic generation; M. Part V: Stabilization and Relativistic Effects in Super Strong Fields. Dynamics of a two-electron system driven by an ultrashort and intense laser pulse; B. Two-and-three electron atoms in strong laser fields; P. Non-sequential double ionization of atoms in strong fields; K. Computer experiments on atomic stabilization in a strong laser field; A.

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Table of contents for Library of Congress control number 2001029076

super intense laseratom physics lhuillier a piraux bernard rzazewski kazimierz

It is now possible to produce at the laboratory scale, ultra-short 13 pulses with a duration of 100 femtoseconds 10- second and a power of the order 12 of 1 terawatt 10 Watt. Energy distribution of two-electron ionization of helium in an intense field; R. . Mechanism of the non sequential double ionization of helium; D. The two-electron response in laser driven helium; L. Beyond the simple maris model for high harmonic generation; M. Although the concept of super-intense field has no absolute meaning, it is now usual to call an electromagnetic field super-intense when it exceeds the atomic binding field.

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A. L'Huillier & Bernard Piraux: Super

super intense laseratom physics lhuillier a piraux bernard rzazewski kazimierz

Quasistationary stabilization of the decay of a weakly-bound level and its breakdown in a strong laser field; N. The two-electron response in laser driven helium; L. In the case of the simplest atomic system, hydrogen in its 16 2 ground state, this occurs above an intensity of 3. A semi-classical model for high-harmonic generation; D. Quasistationary stabilization of the decay of a weakly-bound level and its breakdown in a strong laser field; N. X-ray generation via stimulated recombination of electrons and Bohr's correspondence principle; A.

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