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Porowski, Impurities in semiconductors: experimental, in W. ), Band Theory and Transport Properties, Amsterdam: North-Holland, 1982, pp. 330–357. 22. V. S. Lisitsa, Atoms in Plasmas, Berlin: Springer-Verlag, 1994. 23. K. R. Lang, Astrophysical Formulae, Berlin: Springer-Verlag, 1980. 24. G. V. Marr, Plasma Spectroscopy, Amsterdam: Elsevier, 1968. 25. I. I. Sobelman, Atomic Spectra and Radiative Transitions, Berlin: Springer-Verlag, 1979. 26. K. Bartschat, Excitation and ionization of atoms by interaction with electrons, positrons, protons and photons, Phys.
Norstedt, 1974. FIELD, MAGNETIC. See MAGNETIC FLUX. FIELD-ORIENTED CONTROL. See MAGNETIC VARI- 4. C. Cohen-Tannoudji, B. Diu, and F. Laloe¨, Quantum Mechanics, Paris: Hermann, 1977. FIELD PROGRAMMABLE CIRCUIT BOARDS. See IN- 5. R. Landauer, Barrier traversal time, Nature, 341: 567–568, 1989. 6. A. M. Steinberg, P. G. Kwiat, and R. Y. Chia, Measurement of the single-photon tunneling time, Phys. Rev. , 71: 708–711, 1993. ABLES CONTROL. TEGRATED SOFTWARE. FIELD-PROGRAMMABLE GATE ARRAYS. See PROGRAMMABLE LOGIC ARRAYS.
The angular return time depends on the electric field strength and is given to first order by τang = 2π 3 1 −2E 3/2 F (14) this yields typically values of 10 to 50 ps for electric field strengths of 200 V/cm to 900 V/cm; see Ref. 16 and references therein. Very recently, experimental (17) and theoretical (18) work has explored the evolution of Rydberg wave packets of alkalimetal atoms subject to subpicosecond ‘‘half-cycle’’ electromagnetic pulses. The characteristics of half-cycle pulses are very similar to electric field pulses generated by the passing-by projectile in an ion–atom collision.