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This paper presents the beam dynamics systematic corrections and their uncertainties for the Run-1 dataset of the Fermilab Muong−2Experiment. Two corrections to the measured muon precession frequencyωamare associated with well-known effects owing to the use of electrostatic quadrupole (ESQ) vertical focusing in the storage ring. An average vertically oriented motional magnetic field is felt by relativistic muons passing transversely through the radial electric field components created by the ESQ system. The correction depends on the stored momentum distribution and the tunes of the ring, which has relatively weak vertical focusing. Vertical betatron motions imply that the muons do not orbit the ring in a plane exactly orthogonal to the vertical magnetic field direction. A correction is necessary to account for an average pitch angle associated with their trajectories. A third small correction is necessary, because muons that escape the ring during the storage time are slightly biased in initial spin phase compared to the parent distribution. Finally, because two high-voltage resistors in the ESQ network had longer than designedRCtime constants, the vertical and horizontal centroids and envelopes of the stored muon beam drifted slightly, but coherently, during each storage ring fill. This led to the discovery of an important phase-acceptance relationship that requires a correction. The sum of the corrections toωamis0.50±0.09ppm; the uncertainty is small compared to the 0.43 ppm statistical precision ofωam.

This pilot study examines Ohio’s licensed nursing home administrators and state tested nursing assistant’s perspectives about job satisfaction, future career and employment plans, potential beneficial changes to their organizations, and their thoughts on reducing turnover rates in their field. Ohio Board of Executives of Long-Term Services and Supports provided their contact list of all 1,969 licensed nursing home administrators in Ohio in the fall of 2023. Two surveys were created for licensed nursing home administrators and state tested nursing assistants. Results were analyzed for themes within the open-ended responses; 28 surveys were received from licensed nursing home administrators and 17 surveys were received from state tested nursing assistants. Residents and their families are among the top reasons for job satisfaction, many employees face symptoms of burnout, and wages are a concern among both state tested nursing assistants and licensed nursing home administrators. Future career plans differed between the two professions and had distinct driving factors. A discussion of licensed nursing home administrators’ opinions on improving retention and turnover rates should include more accountability, personal responsibility, and adding opportunities for professional growth and development.

The muon (g – 2) experiment E821 is currently in progress at Brookhaven National Laboratory. Four data-taking runs for positive muons and one run for negative muons were successfully accomplished in 1997–2000 and 2001, respectively. Results of the 1997–2000 runs have been published, thus completing our experiment for µ + . Data analysis for the 2001 run for µ – is currently in progress. To provide measurement of a µ – = ½(g – 2) µ – at the same level of accuracy as for a µ + = ½(g – 2) µ +, we would need one more data-taking run. PACS Nos.: 31.15Pf, 31.30Jv, 32.10Hq

We present a detailed report of the method, setup, analysis and results of a precision measurement of the positive muon lifetime. The experiment was conducted at the Paul Scherrer Institute using a time-structured, nearly 100%-polarized, surface muon beam and a segmented, fast-timing, plastic scintillator array. The measurement employed two target arrangements; a magnetized ferromagnetic target with a ~4 kG internal magnetic field and a crystal quartz target in a 130 G external magnetic field. Approximately 1.6 x 10^{12} positrons were accumulated and together the data yield a muon lifetime of tau_{mu}(MuLan) = 2196980.3(2.2) ps (1.0 ppm), thirty times more precise than previous generations of lifetime experiments. The lifetime measurement yields the most accurate value of the Fermi constant G_F (MuLan) = 1.1663787(6) x 10^{-5} GeV^{-2} (0.5 ppm). It also enables new precision studies of weak interactions via lifetime measurements of muonic atoms.

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.

The muon (g – 2) experiment E821 is currently in progress at Brookhaven National Laboratory. Four data-taking runs for positive muons and one run for negative muons were successfully accomplished in 1997–2000 and 2001, respectively. Results of the 1997–2000 runs have been published, thus completing our experiment for µ + . Data analysis for the 2001 run for µ – is currently in progress. To provide measurement of a µ – = ½(g – 2) µ – at the same level of accuracy as for a µ + = ½(g – 2) µ +, we would need one more data-taking run. PACS Nos.: 31.15Pf, 31.30Jv, 32.10Hq

Three independent searches for an electric dipole moment (EDM) of the positive and negative muons have been performed, using spin precession data from the muon g-2 storage ring at Brookhaven National Laboratory. Details on the experimental apparatus and the three analyses are presented. Since the individual results on the positive and negative muon, as well as the combined result, d=-0.1(0.9)E-19 e-cm, are all consistent with zero, we set a new muon EDM limit, |d| < 1.9E-19 e-cm (95% C.L.). This represents a factor of 5 improvement over the previous best limit on the muon EDM.

We present a new measurement of the positive muon magnetic anomaly, \\(a_\\mu \\equiv (g_\\mu - 2)/2\\), from the Fermilab Muon \\(g\\!-\\!2\\) Experiment using data collected in 2019 and 2020. We have analyzed more than 4 times the number of positrons from muon decay than in our previous result from 2018 data. The systematic error is reduced by more than a factor of 2 due to better running conditions, a more stable beam, and improved knowledge of the magnetic field weighted by the muon distribution, \\(\\tilde{\\omega}'^{}_p\\), and of the anomalous precession frequency corrected for beam dynamics effects, \\(\\omega_a\\). From the ratio \\(\\omega_a / \\tilde{\\omega}'^{}_p\\), together with precisely determined external parameters, we determine \\(a_\\mu = 116\\,592\\,057(25) \\times 10^{-11}\\) (0.21 ppm). Combining this result with our previous result from the 2018 data, we obtain \\(a_\\mu\\text{(FNAL)} = 116\\,592\\,055(24) \\times 10^{-11}\\) (0.20 ppm). The new experimental world average is \\(a_\\mu (\\text{Exp}) = 116\\,592\\,059(22)\\times 10^{-11}\\) (0.19 ppm), which represents a factor of 2 improvement in precision.

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.