Multiply charged negative ions of hydrogen in linearly polarized laser fields

Physical Review A - Atomic, Molecular, and Optical Physics

Volumn 56, Issue 3, 1997, Pages 2192-2204

  van Duijn, Ernst ^a   Muller, H G ^a  

^a FOM INSTITUTE AMOLF   (Netherlands)

Author keywords

[No Author keywords available]

Indexed keywords

APPROXIMATION THEORY; ATOMS; BINDING ENERGY; ELECTRON ENERGY LEVELS; ELECTRONS; HYDROGEN; LASERS; OSCILLATIONS; QUANTUM THEORY;

ATOMIC MULTIPLY CHARGED NEGATIVE ION; HIGH FREQUENCY FLOQUET THEORY;

IONS;

EID: 0031233991     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.56.2192     Document Type: Article

References (16)

1. The distortion and Stark shifts of atomic hydrogen have been studied accurately by M. Pont, N. Walet, M. Gavrila, and C. W. McCurdy, Phys. Rev. Lett. 61, 939 (1988); PRLTAO
2. M. Pont, N. Walet, and M. Gavrila, Phys. Rev. A 41, 477 (1990).PLRAAN
3. The appearance of light-induced excited states of (Formula presented) in a linearly polarized field is predicted, based on a fully correlated calculation, by H. G. Muller and M. Gavrila, Phys. Rev. Lett. 71, 1693 (1993); PRLTAO
4. see also Martin Dörr, R. M. Potvliege, Daniel Proulx, and Robin Shakeshaft, Phys. Rev. A 43, 3729 (1991).PLRAAN
5. For the proof that AMCNI of hydrogen do not exist in vacuum, see E. Lieb, Phys. Rev. Lett. 52, 315 (1984).PRLTAO
6. The appearance of light-induced bound states for AMCNI of hydrogen is predicted by Ernst van Duijn, M. Gavrila, and H. G. Muller, Phys. Rev. Lett. 77, 3759 (1996).PRLTAO
7. Light-induced excited states are closely related to shadow states that were first introduced by R. J. Eden and J. R. Taylor, Phys. Rev. 133, B1575 (1964); PHRVAO
8. for the application of shadow states of an electron interacting with an atomic potential in the presence of a radiation field, see R. M. Potvliege and Robin Shakeshaft, Phys. Rev. A 38, 6190 (1988); PLRAAN
9. for the connection with light-induced (excited) states, see, for example, Marcel Pont and Robin Shakeshaft, 43, 3764 (1991);
10. A. S. Fearnside, R. M. Potvliege, and Robin Shakeshaft, 51, 1471 (1995).
11. (a) For the induction of AMCNI in circularly polarized fields, see Ernst van Duijn and H. G. Muller, Phys. Rev. A, preceding paper 56, 2192 (1997); PLRAAN
12. (b) The distortion of atomic hydrogen in a circularly polarized field has been studied extensively by M. Pont, 40, 5659 (1989).
13. For applications of HFFT on superintense high-frequency phenomena, see M. Gavrila in Atoms in Intense Laser Fields, edited by M. Gavrila (Academic, New York, 1992), p. 435.
14. For the adiabatic approximation, see for example, A. Messiah, Quantum Mechanics (North-Holland, Amsterdam, 1964), Chapter XVII, Sec. II, par. 13.
15. For linear polarization the atomic distortion of hydrogen, leading to dichotomy, is studied by M. Pont, N. R. Walet, and M. Gavrila, Phys. Rev. A 41, 477 (1990); PLRAAN
16. For circular polarization, see M. Pont, 40, 5659 (1989).