Abstract

Metastable 2S{2S} muonic-hydrogen atoms undergo collisional 2S{2S}-quenching, with rates which depend strongly on whether the μpμp kinetic energy is above or below the 2S→2P{2S}\to {2P} energy threshold. Above threshold, collisional 2S→2P{2S} \to {2P} excitation followed by fast radiative 2P→1S{2P} \to {1S} deexcitation is allowed. The corresponding short-lived μp(2S)μp ({2S}) component was measured at 0.6 hPa H2\mathrm{H}_2 room temperature gas pressure, with lifetime τ2Sshort=165−29+38τ_{2S}^\mathrm{short} = 165 ^{+38}_{-29} ns (i.e., λ2Squench=7.9−1.6+1.8×1012s−1λ_{2S}^\mathrm{quench} = 7.9 ^{+1.8}_{-1.6} \times 10^{12} \mathrm{s}^{-1} at liquid-hydrogen density) and population ε2Sshort=1.70−0.56+0.80ε_{2S}^\mathrm{short} = 1.70^{+0.80}_{-0.56} % (per μpμp atom). In addition, a value of the μpμp cascade time, Tcasμp=(37±5)T_\mathrm{cas}^{μp} = (37\pm5) ns, was found.

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