muon lifetime
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Author(s):  
Rebecca Carey ◽  
Tim Gorringe ◽  
David Hertzog

The part-per-million measurement of the positive muon lifetime and determination of the Fermi constant by the MuLan experiment at the Paul Scherrer Institute is reviewed. The experiment used an innovative, time-structured, surface muon beam and a near-4\piπ, finely-segmented, plastic scintillator positron detector. Two in-vacuum muon stopping targets were used: a ferromagnetic foil with a large internal magnetic field, and a quartz crystal in a moderate external magnetic field. The experiment acquired a dataset of 1.6 \times 10^{12}1.6×1012 positive muon decays and obtained a muon lifetime \tau_{\mu} = 2\, 196\, 980.3(2.2)τμ=2196980.3(2.2)~ps (1.0~ppm) and Fermi constant G_F = 1.166\, 378\, 7(6) \times 10^{-5}F=1.1663787(6)×10−5 GeV^{-2}−2 (0.5~ppm). The thirty-fold improvement in \tau_{\mu}τμ has proven valuable for precision measurements in nuclear muon capture and the commensurate improvement in G_FF has proven valuable for precision tests of the standard model.


2021 ◽  
Vol 103 (10) ◽  
Author(s):  
Iarley P. Lobo ◽  
Christian Pfeifer

2019 ◽  
Vol 794 ◽  
pp. 41-44
Author(s):  
Michele Arzano ◽  
Jerzy Kowalski-Glikman ◽  
Wojciech Wiślicki
Keyword(s):  

2018 ◽  
Vol 39 (4) ◽  
pp. 045801
Author(s):  
D Bosnar ◽  
Z Matić ◽  
I Friščić ◽  
P Žugec ◽  
H Janči

2018 ◽  
Vol 181 ◽  
pp. 01017 ◽  
Author(s):  
Thomas J. Phillips

A direct measurement of the gravitational acceleration of antimatter has the potential to show that we live in a “Dirac-Milne” Universe, which could explain cosmological observations without the need for dark matter, dark energy, inflation, or missing antimatter. Such a measurement would also be sensitive to the possible existence of a fifth force. Cooling antimatter to temperatures where gravitational energies are comparable to thermal energies is challenging for most forms of antimatter, which annihilate upon contact with matter. The exception is the antimuon (μ+), which is easily cooled by stopping in cold matter, but the short muon lifetime poses challenges. Positive muons that stop in material will combine with free electrons to form muonium, a neutral leptonic atom with most of its mass derived from the 2nd-generation antimuon. We are developing the Muonium Antimatter Gravity Experiment (MAGE) to measure the gravitational force on muonium using a novel, monoenergetic, low-velocity, horizontal muonium beam directed at an ultra-precise atom interferometer. If successful, MAGE will measure for the first time the gravitational coupling to a 2nd-generation particle in a system whose antimatter-dominated mass is not predominantly strong-interaction binding energy. The novel MAGE beam production approach could also have important applications to other muonium experiments as well as to the measurement ofg– 2.


2017 ◽  
Vol 866 ◽  
pp. 012011
Author(s):  
Luis Rodolfo Pérez Sánchez ◽  
Federico Izraelevitch

Author(s):  
Feng Zhang ◽  
Boyuan Li ◽  
Lianqiang Shan ◽  
Bo Zhang ◽  
Wei Hong ◽  
...  

Muons produced by a short pulse laser can serve as a new type of muon source having potential advantages of high intensity, small source emittance, short pulse duration and low cost. To validate it in experiments, a suitable muon diagnostics system is needed since high muon flux generated by a short pulse laser shot is always accompanied by high radiation background, which is quite different from cases in general muon researches. A detection system is proposed to distinguish muon signals from radiation background by measuring the muon lifetime. It is based on the scintillator detector with water and lead shields, in which water is used to adjust energies of muons stopped in the scintillator and lead to against radiation background. A Geant4 simulation on the performance of the detection system shows that efficiency up to 52% could be arrived for low-energy muons around 200 MeV and this efficiency decreases to 14% for high-energy muons above 1000 MeV. The simulation also shows that the muon lifetime can be derived properly by measuring attenuation of the scintilla light of electrons from muon decays inside the scintillator detector.


2013 ◽  
Vol 87 (5) ◽  
Author(s):  
V. Tishchenko ◽  
S. Battu ◽  
R. M. Carey ◽  
D. B. Chitwood ◽  
J. Crnkovic ◽  
...  

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