86 research outputs found

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

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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.Comment: Accepted for publication in Phys. Rev. Let

    Measurement of the Rate of Muon Capture in Hydrogen Gas and Determination of the Proton's Pseudoscalar Coupling gPg_P

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    The rate of nuclear muon capture by the proton has been measured using a new experimental technique based on a time projection chamber operating in ultra-clean, deuterium-depleted hydrogen gas at 1 MPa pressure. The capture rate was obtained from the difference between the measured Ό−\mu^- disappearance rate in hydrogen and the world average for the ÎŒ+\mu^+ decay rate. The target's low gas density of 1% compared to liquid hydrogen is key to avoiding uncertainties that arise from the formation of muonic molecules. The capture rate from the hyperfine singlet ground state of the ÎŒp\mu p atom is measured to be ΛS=725.0±17.4s−1\Lambda_S=725.0 \pm 17.4 s^{-1}, from which the induced pseudoscalar coupling of the nucleon, gP(q2=−0.88mÎŒ2)=7.3±1.1g_P(q^2=-0.88 m_\mu^2)=7.3 \pm 1.1, is extracted. This result is consistent with theoretical predictions for gPg_P that are based on the approximate chiral symmetry of QCD.Comment: submitted to Phys.Rev.Let

    Improved Measurement of the Positive Muon Lifetime and Determination of the Fermi Constant

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    The mean life of the positive muon has been measured to a precision of 11 ppm using a low-energy, pulsed muon beam stopped in a ferromagnetic target, which was surrounded by a scintillator detector array. The result, tau_mu = 2.197013(24) us, is in excellent agreement with the previous world average. The new world average tau_mu = 2.197019(21) us determines the Fermi constant G_F = 1.166371(6) x 10^-5 GeV^-2 (5 ppm). Additionally, the precision measurement of the positive muon lifetime is needed to determine the nucleon pseudoscalar coupling g_P.Comment: As published version (PRL, July 2007

    The DEAR experiment on DAΊNE

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    DEAR is one of the first experiments at the new DAΊNE Ø-factory at the Laboratori Nazionali di Frascati dell'INFN. The objective of the DEAR experiment is to perform a precision measurement of the strong interaction shifts and widths of the K-series lines in kaonic hydrogen and the first observation of the same quantities in kaonic deuterium. The aim is to obtain a precise determination of the isospin-dependent kaon-nucleon scattering lengths which will represent a breakthrough in KN low-energy phenomenology and will allow us to determine the kaon-nucleon sigma terms. The sigma terms give a direct measurement of chiral symmetry breaking and are connected to the strangeness content of the proton. First results on background measurements with the DEAR NTP setup installed on DAΊNE are reported

    Measurement of Muon Capture on the Proton to 1% Precision and Determination of the Pseudoscalar Coupling g_P

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    The MuCap experiment at the Paul Scherrer Institute has measured the rate L_S of muon capture from the singlet state of the muonic hydrogen atom to a precision of 1%. A muon beam was stopped in a time projection chamber filled with 10-bar, ultra-pure hydrogen gas. Cylindrical wire chambers and a segmented scintillator barrel detected electrons from muon decay. L_S is determined from the difference between the mu- disappearance rate in hydrogen and the free muon decay rate. The result is based on the analysis of 1.2 10^10 mu- decays, from which we extract the capture rate L_S = (714.9 +- 5.4(stat) +- 5.1(syst)) s^-1 and derive the proton's pseudoscalar coupling g_P(q^2_0 = -0.88 m^2_mu) = 8.06 +- 0.55.Comment: Updated figure 1 and small changes in wording to match published versio

    A worldwide survey of neonicotinoids in honey

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    Resonant Formation of dÎŒtd\mu t Molecules in Deuterium: An Atomic Beam Measurement of Muon Catalyzed dt Fusion

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    Resonant formation of dÎŒtd\mu t molecules in collisions of muonic tritium (ÎŒt\mu t) on D2_2 was investigated using a beam of ÎŒt\mu t atoms, demonstrating a new direct approach in muon catalyzed fusion studies. Strong epithermal resonances in dÎŒtd\mu t formation were directly revealed for the first time. From the time-of-flight analysis of 2036±1162036\pm 116 dtdt fusion events, a formation rate consistent with 0.73±(0.16)meas±(0.09)model0.73\pm (0.16)_{meas} \pm (0.09)_{model} times the theoretical prediction was obtained. For the largest peak at a resonance energy of 0.423±0.0370.423 \pm 0.037 eV, this corresponds to a rate of (7.1±1.8)×109(7.1 \pm 1.8) \times 10^9 s−1^{-1}, more than an order of magnitude larger than those at low energies.Comment: To appear in Phys. Rev. Let

    Muonic hydrogen cascade time and lifetime of the short-lived 2S2S state

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    Metastable 2S{2S} muonic-hydrogen atoms undergo collisional 2S{2S}-quenching, with rates which depend strongly on whether the ÎŒp\mu p 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 ÎŒp(2S)\mu p ({2S}) component was measured at 0.6 hPa H2\mathrm{H}_2 room temperature gas pressure, with lifetime τ2Sshort=165−29+38\tau_{2S}^\mathrm{short} = 165 ^{+38}_{-29} ns (i.e., λ2Squench=7.9−1.6+1.8×1012s−1\lambda_{2S}^\mathrm{quench} = 7.9 ^{+1.8}_{-1.6} \times 10^{12} \mathrm{s}^{-1} at liquid-hydrogen density) and population Ï”2Sshort=1.70−0.56+0.80\epsilon_{2S}^\mathrm{short} = 1.70^{+0.80}_{-0.56} % (per ÎŒp\mu p atom). In addition, a value of the ÎŒp\mu p cascade time, TcasÎŒp=(37±5)T_\mathrm{cas}^{\mu p} = (37\pm5) ns, was found.Comment: 4 pages, 3 figure

    The proton radius puzzle

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    High-precision measurements of the proton radius from laser spectroscopy of muonic hydrogen demonstrated up to six standard deviations smaller values than obtained from electron-proton scattering and hydrogen spectroscopy. The status of this discrepancy, which is known as the proton radius puzzle will be discussed in this paper, complemented with the new insights obtained from spectroscopy of muonic deuterium.Comment: Moriond 2017 conference, 8 pages, 4 figure
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