Griffiths Introduction to Elementary Particles · Problem 7.9

Electrodynamics of Quarks and Hadrons — David J. Griffiths

Physics — QFT · charge-conjugation

Problem

The charge conjugation operator (CC) takes a Dirac spinor into the ``charge-conjugate'' spinor ψc\psi_c, given by ψc=iγ2ψ∗\psi_c = i\gamma^2\psi^* [See Halzen and Martin, ref. 7, Sect. 5.4.] Find the charge-conjugates of u(1)u^{(1)} and u(2)u^{(2)}, and compare them with v(1)v^{(1)} and v(2)v^{(2)}.
Intuitive explanation

Charge conjugation reveals a deep symmetry between particles and antiparticles in the Dirac equation. The key insight is that applying CC to a particle spinor (like uu) should yield an antiparticle spinor (like vv), up to phase and normalization—this is the physical content of ψc=iγ2ψ∗\psi_c = i\gamma^2\psi^*. You'll need to use the explicit forms of u(1,2)u^{(1,2)} and v(1,2)v^{(1,2)}, apply complex conjugation and the γ2\gamma^2 matrix, and then compare the results to see how the two spinor types are related by this symmetry operation.

Intuitive explanation

Charge conjugation reveals a deep symmetry between particles and antiparticles in the Dirac equation. The key insight is that applying CC to a particle spinor (like uu) should yield an antiparticle spinor (like vv), up to phase and normalization—this is the physical content of ψc=iγ2ψ∗\psi_c = i\gamma^2\psi^*. You'll need to use the explicit forms of u(1,2)u^{(1,2)} and v(1,2)v^{(1,2)}, apply complex conjugation and the γ2\gamma^2 matrix, and then compare the results to see how the two spinor types are related by this symmetry operation.

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