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Abstract

A negative muon, captured in a mixture of natural hydrogen with a small amount of another gas of atomic number Z, forms a muonic hydrogen or a muonic Z atom in an excited state. In the deexcitation process, muonic X rays are emitted. Because the cascade time is very short (of the order of 10–12 s at 10 bar), they appear promptly with regard to the incoming muon. After deexcitation of the (μp)* system (in about 10–10s), which occurs essentially by collisions, 1 the (up) is atom can then disappear by muon decay with an associated rate λ0, by formation of a pup mesomolecule (λpp), or by transferring the muon to deuterium (λd) or to the Z element (λpz). The total disappearance rate of the up atom, λ is then:

$$\lambda = {\lambda _{0}} + {\lambda _{{pp}}} + {\lambda _{d}} + {\lambda _{{pZ}}}$$
((1))

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Jacot-Guillarmod, R., Mulhauser, F., Piller, C., Schaller, L.A., Schellenberg, L., Schneuwly, H. (1990). Muon Transfer to Low Z Elements. In: Simons, L.M., Horváth, D., Torelli, G. (eds) Electromagnetic Cascade and Chemistry of Exotic Atoms. Ettore Majorana International Science Series, vol 52. Springer, Boston, MA. https://doi.org/10.1007/978-1-4899-3701-8_21

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  • DOI: https://doi.org/10.1007/978-1-4899-3701-8_21

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