An elementary treatise on cubic and quartic curves by A. B. Basset

By A. B. Basset

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Thus, we do not believe that this explanation can be considered seriously, t In the same year (1932) Anderson discovered the positron! e. C conjugation, was extended to bosons and other fermions. The discovery of "charge-mirror" pairs μ + , μ~, π+, π~, Κ+, Κ~ and the discovery of antiprotons and antineutrons and anti-hyperons de­ finitely convinced physicists that the universe is symmetric with respect to charge conjugation. Charge conjugation does not mean simply a change in the sign of the electric charge or magnetic moment of the particle; other "charge" quantum numbers—baryonic charge, leptonic charge, strangeness—also change their sign.

In the next order of perturbation theory this amplitude already 36 INTERACTION OF ELEMENTARY PARTICLES contains corrections of order oc, due to virtual photons. These corrections have been calculated, and are in excellent agreement with the relevant experimental data. Unfortunately, the problem of finding the amplitude from a given Lagrangian has been solved only in quantum electrodynamics. For the present, we are still very far from solving this problem for strong interaction. However, quite a number of general require­ ments which must be satisfied by the amplitudes of one or another process are well established.

When ξχ = £y = 0, ξ2 = 1. Then Λ* = UP + μ)(ΐ- y5s) = iMi + yd (i + r 5 r 3 ) = f(22o0)(2Oo2H,(Io°o)· which is the same as the expression for the matrix uü, obtained in the system in which the particle is at rest. But As is covariant, and, if two covariant quantities are equal in any coordinate system they are identical. Consequently, uü can indeed be replaced by A*. e. it is necessary to take the sum Λ* + Λ- = UP + μ)(\y5s) + HP + μ) (i + y5s) = (β+μ)=Λ. REDUCTION TO TRACES We shall calculate \M\2 for the case when a polarized muon decays and the polarization of the electron and neutrinos is not measured.

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