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John G. Webster (Editor) 's 45.Plasma Science PDF

By John G. Webster (Editor)

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P. Connerade, K. Dietz, and M. H. R. Hutchinson, Atoms in strong fields and the quest for high intensity lasers, Phys. , T58: 23–30, 1995. W. SCHWEIZER BIBLIOGRAPHY Universita¨t Tu¨bingen 1. J. R. Oppenheimer, Phys. , 31: 66–81, 1928. 2. G. , Phys. Rev. , 49: 57–61, 1982. 3. L. Esaki, Long journey into tunneling, Les Prix Nobel en 1973, Stockholm: Imprimerie Royale, P. A. Norstedt, 1974. FIELD, MAGNETIC. See MAGNETIC FLUX. FIELD-ORIENTED CONTROL. See MAGNETIC VARI- 4. C. Cohen-Tannoudji, B. Diu, and F.

Therefore the linear Stark effect can be observed only for those atoms and ions. For nonhydrogenic atoms, for example, alkali-metal atoms, the angular momentum degeneracy is removed due to the multielectron interaction of the atomic core and hence only the quadratic Stark effect can be observed. For stronger electric fields perturbation methods are no longer applicable and hence more advanced numerical methods have to be used to obtain the correct spectrum. One of the most challenging numerical methods is given by using complex coordinate rotations of the space coordinates in combination with computations of the Hamiltonian matrix.

Confinement in these systems is so good that the fusion reactions can proceed at very slow rates and still keep up with losses. Energy is produced by nuclear fusion in the core of the sun at a rate somewhat lower (per unit volume) than is produced by metabolism in the human body. Unfortunately, gravity is such a weak 47 v dv E + v × B) = Ze(E dt (5) where v is the velocity of the particle in meters per second, m is its mass, the charge on an electron is Ϫe, Z is the net ion charge in units of e, and B is the strength of the magnetic field in tesla.

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45.Plasma Science by John G. Webster (Editor)

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