In muonic hydrogen

CHEMISTRY · Multi-part · CBSE · Chemistry · Structure of Atom · Structure of Atom

Problem

In muonic hydrogen, the electron is replaced by a negatively charged muon (μ−\mu^-) that has the same charge magnitude as the electron but a mass mμ=207 mem_{\mu}=207\,m_e. The muon orbits a proton in a circular stationary state described by a principal quantum number nn. Assume the proton is infinitely massive compared with the muon. Constants: • e=1.60×10−19 Ce = 1.60\times10^{-19}\,\text{C} • ε0=8.85×10−12 C2 N−1 m−2\varepsilon_0 = 8.85\times10^{-12}\,\text{C}^2\,\text{N}^{-1}\,\text{m}^{-2} • h=6.63×10−34 J sh = 6.63\times10^{-34}\,\text{J\,s} • me=9.11×10−31 kgm_e = 9.11\times10^{-31}\,\text{kg} (a) Derive a general expression for the allowed orbital radius rn(μ)r_n^{(\mu)} of the muon in terms of nn, mμm_{\mu}, and fundamental constants. Express your result as a multiple of the Bohr radius a0a_0. (b) Calculate the ground-state (n=1n=1) radius of muonic hydrogen and compare it quantitatively with the ground-state radius of ordinary hydrogen. (c) Determine the ground-state energy E1(μ)E_{1}^{(\mu)} of muonic hydrogen in electron-volts (eV). (d) Explain qualitatively how the smaller orbital radius affects the wavelengths of spectral lines in muonic hydrogen compared with ordinary hydrogen.

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