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Free-fall atomic model

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The free-fall atomic model was introduced in 1965 by Michał Gryziński (1930-2004), a Polish nuclear and plasma physicist, as a result of adding electron's magnetic moment to Bohr's atomic picture. Gryziński proposed the model as a consequence of his classical scattering theory. In this classical approximation, electrons do not circulate as in the Bohr model, but enter in almost radial free-fall towards the nucleus. Due to their magnetic moment, the Lorentz force bends the electron trajectories to return them to their initial radius. This model has never been part of mainstream physics. It can be seen as an attempt to answer the question: "what would have happened had the QM not been invented?".[1]

Model[edit]

For simplicity, most of these considerations neglect small changes of orientation of the spin axis of electron, assuming that it is firmly oriented in space - it's called rigid top approximation. Magnetic moment of nucleus is thousands of times smaller than electron's, so such hyperfine corrections can be neglected in basic models.

Finally the basic considered Lagrangian for dynamics of single electron in these models is:

The last term describes interaction between magnetic field of traveling electron's magnetic moment and electric field of nucleus (spin-orbit interaction).

History[edit]

Michał Gryziński was working in group of hot plasma of Polish Academy of Science on approach to nuclear fusion which has later evolved to what is currently known as dense plasma focus. His experimental and theoretical consideration have led him to his 1957 "Stopping Power of a Medium for Heavy, Charged Particles" Physical Review article emphasizing importance of orbital motion of electrons of a medium for stopping of slow charged particles. This work has received great interest and led him to a series of articles about the problem of scattering with classical approximation of dynamics of electrons; his 1965 articles have received more than 2000 total citations.

Classical approximation of dynamics of electrons in atoms has led him to the free-fall atomic model to improve agreement with scattering experiments comparing to the popular Bohr approximation as circular orbits for electrons. This dominant radial dynamics of electrons makes the atom effectively a pulsating electric multipole (dipole, quadrupole), which allowed him to propose an explanation for the Ramsauer effect (1970) and improve agreement for modeling of low energy scattering (1975). His later articles try to expand these classical approximations to multielectron atoms and molecules.

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