Srednicki — Quantum Field Theory · Problem 52.3

Canonical Quantization of Scalar Fields — Mark Srednicki

Physics — QFT · fixed-points-yukawa-beta-functions

Problem

Consider the beta functions of eqs. (52.15) and (52.16). a) Let ρ≡λ/g2\rho \equiv \lambda/g^2, and compute dρ/dln⁡μd\rho/d\ln\mu. Express your answer in terms of gg and ρ\rho. Explain why it is better to work with gg and ρ\rho rather than gg and λ\lambda. Hint: the answer is mathematical, not physical. b) Show that there are two fixed points, ρ+∗\rho^*_+ and ρ−∗\rho^*_-, where dρ/dln⁡μ=0d\rho/d\ln\mu = 0, and find their values. c) Suppose that, for some particular value of the renormalization scale μ\mu, we have ρ=0\rho = 0 and g⋘1g \lll 1. What happens to ρ\rho at much higher values of μ\mu (but still low enough to keep g≪1g \ll 1)? At much lower values of μ\mu? d) Same question, but with an initial value of ρ=5\rho = 5. e) Same question, but with an initial value of ρ=−5\rho = -5. f) Find the trajectory in the (ρ,g)(\rho, g) plane that is followed for each of the three starting points as μ\mu is varied up and down. Hint: you should find that the trajectories take the form g=g0∣ρ−ρ+∗ρ−ρ−∗∣νg = g_0 \left|\frac{\rho - \rho^*_+}{\rho - \rho^*_-}\right|^\nu for some particular exponent ν\nu. Put arrows on the trajectories that point in the direction of increasing μ\mu. g) Explain why ρ−∗\rho^*_- is called an ultraviolet stable fixed point, and why ρ+∗\rho^*_+ is called an infrared stable fixed point.

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