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C-symmetry

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Charge conjugation is a transformation that switches all particles with their corresponding antiparticles, and thus changes the sign of all charges: not only electric charge but also the charges relevant to other forces. In physics, C-symmetry means the symmetry of physical laws under a charge-conjugation transformation. Electromagnetism, gravity and the strong interaction all obey C-symmetry, but weak interactions violate C-symmetry.

Charge reversal in electroweak theory[edit source | edit]

The laws of electromagnetism (both classical and quantum) are invariant under this transformation: if each charge q were to be replaced with a charge −q, and thus the directions of the electric and magnetic fields were reversed, the dynamics would preserve the same form. In the language of quantum field theory, charge conjugation transforms:[1]

  1. <math>\psi \rightarrow -i(\bar\psi \gamma^0 \gamma^2)^T</math>
  2. <math>\bar\psi \rightarrow -i(\gamma^0 \gamma^2 \psi)^T</math>
  3. <math>A^\mu \rightarrow -A^\mu</math>

Notice that these transformations do not alter the chirality of particles. A left-handed neutrino would be taken by charge conjugation into a left-handed antineutrino, which does not interact in the Standard Model. This property is what is meant by the "maximal violation" of C-symmetry in the weak interaction.

(Some postulated extensions of the Standard Model, like left-right models, restore this C-symmetry.)

Combination of charge and parity reversal[edit source | edit]

It was believed for some time that C-symmetry could be combined with the parity-inversion transformation (see P-symmetry) to preserve a combined CP-symmetry. However, violations of this symmetry have been identified in the weak interactions (particularly in the kaons and B mesons). In the Standard Model, this CP violation is due to a single phase in the CKM matrix. If CP is combined with time reversal (T-symmetry), the resulting CPT-symmetry can be shown using only the Wightman axioms to be universally obeyed.

Charge definition[edit source | edit]

To give an example, take two real scalar fields, φ and χ. Suppose both fields have even C-parity (even C-parity refers to even symmetry under charge conjugation e.g., <math>C\psi(q) = C\psi(-q)</math>, as opposed to odd C-parity which refers to antisymmetry under charge conjugation, e.g., <math>C\psi(q)=-C\psi(-q)</math>).

Define <math>\psi\ \stackrel{\mathrm{def}}{=}\ {\phi + i \chi\over \sqrt{2}}</math>. Now, φ and χ have even C-parities, and the imaginary number i has an odd C-parity (C is anti-unitary). Under C, ψ goes to ψ*.

In other models, it is also possible for both φ and χ to have odd C-parities.

See also[edit source | edit]

References[edit source | edit]

  1. Peskin, M.E.; Schroeder, D.V. (1997). An Introduction to Quantum Field Theory. Addison Wesley. ISBN 0-201-50397-2.
  • Sozzi, M.S. (2008). Discrete symmetries and CP violation. Oxford University Press. ISBN 978-0-19-929666-8.