Low-frequency atomic stabilization and dichotomy in superintense laser fields from the high-intensity high-frequency Floquet theory

Physical Review A - Atomic, Molecular, and Optical Physics

Volumn 78, Issue 3, 2008, Pages

  Gavrila, M ^a,b   Simbotin, I ^a   Stroe, M ^c  

^a HARVARD SMITHSONIAN CENTER FOR ASTROPHYSICS   (United States)

^b FOM INSTITUTE AMOLF   (Netherlands)

^c UNIVERSITY OF BUCHAREST   (Romania)

Author keywords

[No Author keywords available]

Indexed keywords

ATOMIC PHYSICS; ATOMS; COMPUTER NETWORKS; DIFFERENTIAL EQUATIONS; ELECTRIC FIELDS; LASER OPTICS; LASERS; STABILIZATION; THEOREM PROVING; TOKAMAK DEVICES; WAVE FUNCTIONS;

FLOQUET THEORY; HIGH FREQUENCIES;

LASER THEORY;

EID: 51649091700     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.78.033404     Document Type: Article

References (18)

1. M. Gavrila, J. Phys. B JPAPEH 0953-4075 10.1088/0953-4075/35/18/201 35, R147 (2002).
2. M. Gavrila and J. Z. Kaminski, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.52.613 52, 613 (1984).
3. M. Gavrila, in Atoms in Intense Laser Fields, edited by, M. Gavrila, (Academic Press, New York, 1992), p. 435.
4. M. Gavrila and J. Z. Kaminski (unpublished).
5. P. S. Krstic and M. H. Mittleman, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.42.4037 42, 4037 (1990).
6. M. Pont, N. R. Walet, M. Gavrila, and C. W. McCurdy, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.61.939 61, 939 (1988).
7. M. Pont, N. R. Walet, and M. Gavrila, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.41.477 41, 477 (1990).
8. M. Pont and M. Gavrila, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.65.2362 65, 2362 (1990).
9. I. S. Gradshteyn and I. M. Ryzhik, Tables of Integrals, Series and Products (Academic Press, New York, 1965).
10. M. Gavrila and J. Shertzer, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.53.3431 53, 3431 (1996).
11. See, Eqs. 3.137.7, 8.112.1, and 8.121.3.
12. See, Eq. 8.113.1 for x>0, and Eq. 8.113.3 for x<0.
13. In the case of the 1D model with a potential V (x) =- V0 δ (x), the scaling law of the levels is exactly α0 -23 as in the 3D case; see T. P. Grozdanov, P. S. Krstic, and M. H. Mittleman, Phys. Lett. A PYLAAG 0375-9601 10.1016/0375-9601(90)90541-U 149, 144 (1990).
14. A. Klein and C. Zemach, Ann. Phys. (N.Y.) APNYA6 0003-4916 10.1016/0003-4916(59)90053-3 7, 440 (1959), Sec. 3.
15. J. C. Wells, I. Simbotin, and M. Gavrila, Laser Phys. LAPHEJ 1054-660X 7, 525 (1997).
16. J. C. Wells, I. Simbotin, and M. Gavrila, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.56.3961 56, 3961 (1997).
17. H. C. Day, B. Piraux, and R. M. Potvliege, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.61.031402 61, 031402 (R) (2000).
18. M. Stroe, I. Simbotin, and M. Gavrila Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.78.033405 78, 033405 (2008).