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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 the 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 an 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 quantum mechanics not been invented?".[1]

Model

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

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

𝐋=12m𝐯2+Ze2r+Zec[𝐯(μ×𝐫r3)]

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

History

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

The classical approximation of electron dynamics in atoms led him to the free-fall atomic model to improve agreement with scattering experiments compared 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 low-energy scattering (1975). His later articles attempt to expand these classical approximations to multielectron atoms and molecules.

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