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Measurement of the Positive Muon Lifetime and Determination of the Fermi Constant to Part-per-Million Precision

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arxiv 1010.0991 v2 pith:ZRFKVQO2 submitted 2010-10-05 hep-ex nucl-ex

classification hep-exnucl-ex
keywords lifetimemuonpreciseconstantexperimentfermimeasurementmulan
verification ladder T0 review T1 audit T2 compute T3 formal
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We report a measurement of the positive muon lifetime to a precision of 1.0 parts per million (ppm); it is the most precise particle lifetime ever measured. The experiment used a time-structured, low-energy muon beam and a segmented plastic scintillator array to record more than 2 x 10^{12} decays. Two different stopping target configurations were employed in independent data-taking periods. The combined results give tau_{mu^+}(MuLan) = 2196980.3(2.2) ps, more than 15 times as precise as any previous experiment. The muon lifetime gives the most precise value for the Fermi constant: G_F(MuLan) = 1.1663788 (7) x 10^-5 GeV^-2 (0.6 ppm). It is also used to extract the mu^-p singlet capture rate, which determines the proton's weak induced pseudoscalar coupling g_P.

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Cited by 4 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

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    Forward-region Bhabha ratios at Tera-Z could extract alpha_em(m_Z^2) with a projected statistical sensitivity of about 6e-6, below the current bottleneck.

  3. Neutrino Induced Charged Current Coherent Pion Production for Constraining the Muon Neutrino Flux at DUNE

    hep-ph 2025-02 conditional novelty 6.0 of 10

    Monte Carlo projections indicate that neutrino-induced coherent pion production can constrain the DUNE muon-neutrino flux normalization to about 1.5% (in-situ pion-argon measurement) or 2-5% (external pion-argon data)...

  4. Complete $\mathcal{O}(\alpha_s^2)$ Corrections to the Leptonic Invariant Mass Spectrum in $b\to X_c l\bar{\nu}_l$ Decay

    hep-ph 2024-11 accept novelty 6.0 of 10

    The authors complete the O(alpha_s^2) perturbative correction to the q^2 spectrum of b -> X_c l nu_l, adding the triple-charm channel, and confirm the existing single-charm result.

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