By Hawkes, P. W.; Lochak, Georges; Stumpf, Harald
ISBN-10: 0128024631
ISBN-13: 9780128024638
ISBN-10: 0128025913
ISBN-13: 9780128025918
Advances in Imaging and Electron Physics merges long-running serials-Advances in Electronics and Electron Physics and Advances in Optical and Electron Microscopy. The sequence good points prolonged articles at the physics of electron units (especially semiconductor devices), particle optics at low and high energies, microlithography, picture technology and electronic picture processing, electromagnetic wave propagation, electron microscopy, and the computing equipment utilized in a majority of these domains.
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Extra resources for The leptonic magnetic monopole : theory and experiments
Sample text
8)] of Poincaré, which shows that the total Lagrange moment increases with the Poincaré constant l (proportional to the magnetic charge, as will be confirmed in quantum mechanics), the vertex angle Q0 of the cone decreases with the charge because it varies as lÀ1 . Finally, it is the angle Q0 that gives the deviation of monopoles by an electric charge. It is noteworthy that Dirac’s condition [Eq. 30). Nevertheless, we cannot forget that it was not systematically proveddand indeed, it has even been contradicted by many authors.
8 THE PROBLEM OF THE LINK BETWEEN A LEPTONIC MAGNETIC MONOPOLE, A NEUTRINO, AND WEAK INTERACTIONS The problem being explored in this chapter may be summarized as follows: 40 Georges Lochak 1. The Weyl representation splits the massless Dirac equation into two independent, two-component equations, which are considered since 1956 (by Lee and Yang and Landau) as the “neutrino two-component theory”: one equation describes the neutrino and the other one the anti-neutrino. 2. We have shown that the massless Dirac equation admits a second gauge invariance: the chiral gauge.
23). 28 Georges Lochak Therefore, our magnetic current, Km ¼ g Sm , may be spacelike because the true magnetic currents are the isotropic currents g Xm and Àg Ym , corresponding to the spinor states x and h. The pseudovector Km is only their difference, so it has no reason to be spacelike or timelike. Therefore, the relativistic type of the magnetic current Km has no importance; on the contrary, the fact that Jm is timelike is very important because owing to this property, Jm may be interpreted as a current density of probability or electricity.
The leptonic magnetic monopole : theory and experiments by Hawkes, P. W.; Lochak, Georges; Stumpf, Harald
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