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The Exact Theory of the Stern–Gerlach Experiment and Why It Does Not Imply That a Fermion Can Only Have Its Spin Up or Down

Authors :
Gerrit Coddens
Laboratoire des Solides Irradiés (LSI)
École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS)-Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)
Coddens, Gerrit
Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS)
Source :
Symmetry, Vol 13, Iss 134, p 134 (2021), Symmetry, Volume 13, Issue 1
Publication Year :
2021
Publisher :
MDPI AG, 2021.

Abstract

The Stern&ndash<br />Gerlach experiment is notoriously counter-intuitive. The official theory is that the spin of a fermion remains always aligned with the magnetic field. Its directions are thus quantized: It can only be spin-up or spin-down. However, that theory is based on mathematical errors in the way it (mis)treats spinors and group theory. We present here a mathematically rigorous theory for a fermion in a magnetic field, which is no longer counter-intuitive. It is based on an understanding of spinors in SU(2) which is only Euclidean geometry. Contrary to what Pauli has been reading into the Stern&ndash<br />Gerlach experiment, the spin directions are not quantized. The new corrected paradigm, which solves all conceptual problems, is that the fermions precess around the magnetic-field just as Einstein and Ehrenfest had conjectured. Surprisingly, this leads to only two energy states, which should be qualified as precession-up and precession-down rather than spin-up and spin-down. Indeed, despite the presence of the many different possible angles &theta<br />between the spin axis s and the magnetic field B, the fermions can only have two possible energies m0c2&plusmn<br />&mu<br />B. The values &plusmn<br />B thus do not correspond to the continuum of values &minus<br />&middot<br />B Einstein and Ehrenfest had conjectured. The energy term V=&minus<br />B is a macroscopic quantity. It is a statistical average over a large ensemble of fermions distributed over the two microscopic states with energies &plusmn<br />B, and as such not valid for individual fermions. The two fermion states with energy &plusmn<br />B are not potential-energy states. We also explain the mathematically rigorous meaning of the up and down spinors. They represent left-handed and right-handed reference frames, such that now everything is intuitively clear and understandable in simple geometrical terms. The paradigm shift does not affect the Pauli principle.

Details

Language :
English
ISSN :
20738994
Volume :
13
Issue :
134
Database :
OpenAIRE
Journal :
Symmetry
Accession number :
edsair.doi.dedup.....6fd3433fa1d2294896c591c237e3cc4e