Standard Model and Beyond · Problem 2.30

Lie Groups, Lie Algebras, and Symmetries

Physics — Particle Physics · electron-vertex-non-relativistic-edm

Problem

Consider the non-relativistic limit of the matrix element (2.356) for an e−e^- in a static external field. (a) Compute the limit to linear order in the momenta. Hint: use the explicit forms for the spinors in the Pauli-Dirac representation. It simplifies the calculation to rewrite uˉ2Γμu1\bar{u}_2\Gamma^\mu u_1 using the Gordon decomposition. (b) Suppose that Γμ(p2,p1)\Gamma^\mu(p_2,p_1) in (2.352) contained a term iσμν2mqνγ5G2(q2)\frac{i\sigma^{\mu\nu}}{2m}q_\nu\gamma^5 G_2(q^2). This violates PP and TT but in principle could be generated by a new interaction. Show how G2(0)G_2(0) is related to the electric dipole moment d⃗e\vec{d}_e of the electron, which is defined by the non-relativistic interaction HEDM=−d⃗e⋅E⃗(x⃗)H_{EDM} = -\vec{d}_e\cdot\vec{E}(\vec{x}), where E⃗\vec{E} is an external electric field. Note that the Hermiticity condition (2.354) requires that G2G_2 is pure imaginary.

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