Abstract
We argue that the velocity gauge is the natural one in which to formulate the theory of multiphoton ionization of atoms by intense fields. If the length gauge is used, careful attention must be paid to the time evolution of the eigenvector which characterizes the state in which the photoelectron emerges when the atom is ionized.
Similar content being viewed by others
References
Schlicher, R.R., Becker, W., Bergou, J., Scully, M.O.: In: Quantum electrodynamics and quantum optics. Barut A.O. (ed.), p. 405. New York: Plenum 1984
Lamb, W.E. Jr.: Phys. Rev.85, 259 (1952)
Shakeshaft, R., Tang, X.: Phys. Rev. A36, 3193 (1987)
Spruch, L.: In: Lectures in theoretical physics. Geltman, S., Manhanthappa, K.T., Britten, W.E., (eds.), Vol. XIC, p. 77. New York: Gordon and Breach 1969
Shakeshaft, R.: J. Opt. Soc. Am. B4, 705 (1987)
Cohen-Tannoudji, C., Diu, B., Laloe, F.: Quantum mechanics. Vol. 1, p. 315. Paris: Hermann/Wiley 1977
Aymar, M., Crance, M.: J. Phys. B14, 3585 (1981)
Edwards, M., Shakeshaft, R.: Z. Phys. D — Atoms, Molecules and Clusters8, 51 (1988)
Berson, I.J.: J. Phys. B8, 3078 (1975); Shakeshaft, R.: Phys. Rev. A28, 667 (1983)
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Shakeshaft, R. Multiphoton ionization of an atom; the choice of gauge. Z Phys D - Atoms, Molecules and Clusters 8, 47–50 (1988). https://doi.org/10.1007/BF01384522
Received:
Revised:
Issue Date:
DOI: https://doi.org/10.1007/BF01384522