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Srednicki — Quantum Field Theory · Problem 27.1
Canonical Quantization of Scalar Fields — Mark Srednicki
Physics — QFT · renormalization-group-mass-running
Problem Suppose that we have a theory with
β ( α ) = b 1 α 2 + O ( α 3 ) , γ m ( α ) = c 1 α + O ( α 2 ) . (27.27) \begin{aligned}
\beta(\alpha) &= b_1\alpha^2 + O(\alpha^3) \,, \tag{27.27} \\
\gamma_m(\alpha) &= c_1\alpha + O(\alpha^2) \,.
\end{aligned} β ( α ) γ m ( α ) = b 1 α 2 + O ( α 3 ) , = c 1 α + O ( α 2 ) . ( 27.27 )
Neglecting the higher-order terms, show that
m ( μ 2 ) = [ α ( μ 2 ) α ( μ 1 ) ] c 1 / b 1 m ( μ 1 ) . (27.29) m(\mu_2) = \left[\frac{\alpha(\mu_2)}{\alpha(\mu_1)}\right]^{c_1/b_1} m(\mu_1) \,. \tag{27.29} m ( μ 2 ) = [ α ( μ 1 ) α ( μ 2 ) ] c 1 / b 1 m ( μ 1 ) . ( 27.29 )
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