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9.4. Charge Conjugation 255<br />

The π 0 and η 0 decay electromagnetically into two photons.<br />

π 0 −→ 2γ and η 0 −→ 2γ,<br />

and therefore must have positive C parity if C is conserved in the decay:<br />

ηc(π 0 )=1, ηc(η 0 )=1. (9.44)<br />

If C parity were applicable only to the photon, π 0 and η 0 ,itwouldnotbe<br />

very useful. However, there exist many particle–antiparticle systems that are fully<br />

neutral. Examples are positronium (e + e − ),π + π − ,pp, nn. The C parity of these<br />

systems depends on angular momentum and spin, and it is a useful quantity for<br />

discussing the possible decay modes.<br />

Use of charge parity for discussion of a decay requires ηc to be a good quantum<br />

number. It is conserved if C commutes with the Hamiltonian H. It is easy to see<br />

that C is not conserved in the weak interaction,<br />

[Hw,C] �= 0. (9.45)<br />

Fig. 7.2 shows that neutrino and antineutrino have opposite polarization (helicity).<br />

If charge conjugation were conserved in the weak interaction, the two particles would<br />

have to have the same helicity.<br />

C conservation in the hadronic interactions has been tested in numerous reactions,<br />

such as<br />

C acting on the reaction gives<br />

pp −→ π + π − π 0 . (9.46a)<br />

pp −→ π − π + π 0 . (9.46b)<br />

If the proton produces the π + forward and the p the π − backwards in the reaction<br />

(9.46a), then the reaction (9.46b) would give rise to π − forward and π +<br />

backward. Thus, if the hadronic Hamiltonian commutes with C, the angular distribution<br />

and energy spectra of the positive and negative pion must be identical.<br />

Comparison of the two distributions and similar tests in other reactions show the<br />

expected symmetry. The result can be stated as (16)<br />

�<br />

�<br />

�<br />

�<br />

C-nonconserving amplitude�<br />

�<br />

� C-conserving amplitude � � 0.01. (9.47)<br />

To test conservation of C in the electromagnetic interaction, charge–parityforbidden<br />

decays are looked for. Consider the decays<br />

π 0 −→ 3γ and η 0 −→ 3γ.<br />

16 C. Baltay, N. Barash, P. Franzini, N. Gelfand, L. Kirsch, G. Lütjens, J. C. Severiens, J.<br />

Steinberger, D. Tycko, and D. Zanello, Phys. Rev. Lett. 15, 591 (1965).

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