Srednicki — Quantum Field Theory · Problem 83.6

Canonical Quantization of Scalar Fields — Mark Srednicki

Physics — QFT · chiral-symmetry-breaking

Problem

Consider the case of three light quark flavors, with masses mum_u, mdm_d, and msm_s. a) Find the masses-squared of the eight pseudogoldstone bosons. Take the limit mu,d≪msm_{u,d} \ll m_s, and drop terms that are of order mu,d2/msm_{u,d}^2/m_s. b) Assume that mπ±2m^2_{\pi^\pm} and mK±2m^2_{K^\pm} each receive an electromagnetic contribution; to zeroth order in the quark masses, this contribution is the same for both, but the comparatively large strange quark mass results in an electromagnetic contribution to mK±2m^2_{K^\pm} that is roughly twice as large as the electromagnetic contribution ΔmEM2\Delta m^2_{\mathrm{EM}} to mπ±2m^2_{\pi^\pm}. Use the observed masses of the π±\pi^\pm, π0\pi^0, K±K^\pm, and K0K^0 to compute muv3/fπ2m_u v^3/f_\pi^2, mdv3/fπ2m_d v^3/f_\pi^2, msv3/fπ2m_s v^3/f_\pi^2, and ΔmEM2\Delta m^2_{\mathrm{EM}}. c) Compute the quark mass ratios mu/mdm_u/m_d and ms/mdm_s/m_d. d) Use your results from part (b) to predict the η\eta mass. How good is your prediction?

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