Srednicki — Quantum Field Theory · Problem 11.4

Canonical Quantization of Scalar Fields — Mark Srednicki

Physics — QFT · three-scalar-field-scattering-amplitudes

Problem

Consider a theory of three real scalar fields (AA, BB, and CC) with L=−12∂μA∂μA−12mA2A2−12∂μB∂μB−12mB2B2−12∂μC∂μC−12mC2C2+gABC.(11.57)\begin{aligned} \mathcal{L} &= -\tfrac{1}{2}\partial^\mu A\partial_\mu A - \tfrac{1}{2}m_A^2 A^2 \\ &\quad - \tfrac{1}{2}\partial^\mu B\partial_\mu B - \tfrac{1}{2}m_B^2 B^2 \\ &\quad - \tfrac{1}{2}\partial^\mu C\partial_\mu C - \tfrac{1}{2}m_C^2 C^2 \\ &\quad + gABC . \tag{11.57} \end{aligned} Write down the tree-level scattering amplitude (given by the sum of the contributing tree diagrams) for each of the following processes: AA→AA,AA→AB,AA→BB,AA→BC,AB→AB,AB→AC.(11.58)\begin{aligned} AA &\to AA , \\ AA &\to AB , \\ AA &\to BB , \\ AA &\to BC , \\ AB &\to AB , \\ AB &\to AC . \tag{11.58} \end{aligned} Your answers should take the form T=g2[csms2−s+ctmt2−t+cumu2−u],(11.59)\mathcal{T} = g^2\left[\frac{c_s}{m_s^2 - s} + \frac{c_t}{m_t^2 - t} + \frac{c_u}{m_u^2 - u}\right], \tag{11.59} where, in each case, each cic_i is a positive integer, and each mi2m_i^2 is mA2m_A^2 or mB2m_B^2 or mC2m_C^2. Hint: T\mathcal{T} may be zero for some processes.

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