A Precision Measurement of the Muon Decay Parameters Rho and Delta

A Precision Measurement of the Muon Decay Parameters Rho and Delta PDF Author: Robert Paul MacDonald
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ISBN:
Category : Muons
Languages : en
Pages : 340

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A Precision Measurement of the Muon Decay Parameters Rho and Delta

A Precision Measurement of the Muon Decay Parameters Rho and Delta PDF Author: Robert Paul MacDonald
Publisher:
ISBN:
Category : Muons
Languages : en
Pages : 340

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A Precision Measurement of the Muon Decay Parameter Delta

A Precision Measurement of the Muon Decay Parameter Delta PDF Author: Andrei Gaponenko
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ISBN:
Category : Muons
Languages : en
Pages : 202

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Measurement of the [delta] and [eta] Muon Decay Parameters

Measurement of the [delta] and [eta] Muon Decay Parameters PDF Author: Anthony Hillairet
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ISBN:
Category :
Languages : en
Pages :

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Muon decay is a unique process involving only the four leptons of the first two generations. This makes it an ideal framework to study the weak interaction. The momentum-angle spectrum of the decay positron can be studied using a general 4-fermion interaction model. Only four parameters are needed in this model to entirely describe the spectrum. The measurement of these four muon decay parameters, rho, eta, delta and Pmu xi, provide a direct test of the Standard Model and its extensions. This thesis presents the final results from the blind analysis of the decay parameter delta using the TWIST (TRIUMF Weak Interaction Symmetry Test) spectrometer. The new precision on the parameter delta is a factor of 11.5 better than the last experimental result prior to TWIST achieving the goal of the TWIST collaboration of an order of magnitude improvement. The challenging parameter eta is also measured from the momentum-angle spectrum for the first time since 1969 with a precision improved by a factor of 7.4. The results are included in a global analysis to obtain stringent limits on some of the coupling constants of the 4-fermion interaction. The result of the measurement of delta are used to evaluate the possibility for a non-local tensor interaction.

Measurement of the Delta and Eta Muon Decay Parameters

Measurement of the Delta and Eta Muon Decay Parameters PDF Author: Anthony Hillairet
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ISBN:
Category :
Languages : en
Pages :

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Measurement of the Delta and Eta Muon Decay Parameters

Measurement of the Delta and Eta Muon Decay Parameters PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

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Book Description
Muon decay is a unique process involving only the four leptons of the first two generations. This makes it an ideal framework to study the weak interaction. The momentum-angle spectrum of the decay positron can be studied using a general 4-fermion interaction model. Only four parameters are needed in this model to entirely describe the spectrum. The measurement of these four muon decay parameters, rho, eta, delta and Pmu xi, provide a direct test of the Standard Model and its extensions. This thesis presents the final results from the blind analysis of the decay parameter delta using the TWIST (TRIUMF Weak Interaction Symmetry Test) spectrometer. The new precision on the parameter delta is a factor of 11.5 better than the last experimental result prior to TWIST achieving the goal of the TWIST collaboration of an order of magnitude improvement. The challenging parameter eta is also measured from the momentum-angle spectrum for the first time since 1969 with a precision improved by a factor of 7.4. The results are included in a global analysis to obtain stringent limits on some of the coupling constants of the 4-fermion interaction. The result of the measurement of delta are used to evaluate the possibility for a non-local tensor interaction.

A Measurement of the Michel Parameter [rho] in Muon Decay

A Measurement of the Michel Parameter [rho] in Muon Decay PDF Author:
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Category :
Languages : en
Pages :

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An improved measurement of the Michel parameter [rho] in normal muon decay has been made using the MEGA positron spectrometer. Muons were stopped in the center of a large solenoid (1.5 T nominal field) and the momenta of positrons with energies over about 35 MeV were measured with a precision of about 0.6 MeV/c FWHM. There over 15 million events in each spectrum taken for three operating configurations. The previous result has a precision of [delta][rho]/[rho] = 0.003 based on a sample of about 1 million events in the positron energy spectrum. The present experiment expects to improve the precision by a factor of three to six, depending on the level of systematic uncertainties. The improved result is a precise test of the standard model of electroweak interactions for a purely leptonic process. It also provides a better constraint on the mixing angle in a left-right symmetric extension to the standard model.

Measurement of the Decay Parameter [rho] and a Search for Non-Standard Model Decays in the Muon Decay Spectrum

Measurement of the Decay Parameter [rho] and a Search for Non-Standard Model Decays in the Muon Decay Spectrum PDF Author: Ryan David Bayes
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ISBN:
Category :
Languages : en
Pages :

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The study of the muon decay process?+? e+?e??? is a powerful constraint on the behaviour of the weak interaction, without contamination of the other, stronger, fundamental interactions. The spectrum measured from the momentum and angles of the decay positrons is parametrized using a set of four decay parameters. The purpose of the TWIST experiment is to measure these decay parameters to an unprecedented precision; an order of magnitude improvement in the uncertainties over measurements completed before the TWIST experiment. Measurements of the muon decay parameters constrain the values of a series of 19 weak coupling constants. In the standard model, V-A weak interaction, 18 of these constants are 0, while the remaining constant describes interactions between left handed particles, gV_LL= 1. The decay parameter? quantifies the behaviour of the spectrum with respect to momentum. According to the standard model the value of this parameter is 3/4. TWIST measured a value of? = 0.74991?0.00009(stat)?0.00028(sys). The measurement is limited by its systematic uncertainty, so a large focus of the experiment was on the determination and control of these uncertainties. The systematic uncertainties are derived from uncertainties in the detector construction and uncertainties in the biases generated by differences between the data and a matching Monte Carlo. Muon decay also limits the possibility of family symmetry breaking interactions. TWIST can be used to search for the possibility of muons decaying into a positron and a single unidentified neutral particle?+? e+X0 that does not otherwise interact with normal matter. The large momentum and angle acceptance of the TWIST spectrometer allows for searches of two body decays for masses of the X0 boson mX0? [0,80] MeV/c, with a variety of behaviours with respect to the angle of the positron track. Upper limits on massive and mass-less X0 decays are set with a 90% confidence level separately at parts per million for massive decays and parts in 10000 for mass-less decays.

Measurement of the Decay Parameter Rho and a Search for Non-Standard Model Decays in the Muon Decay Spectrum

Measurement of the Decay Parameter Rho and a Search for Non-Standard Model Decays in the Muon Decay Spectrum PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

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Book Description
The study of the muon decay process + e+e is a powerful constraint on the behaviour of the weak interaction, without contamination of the other, stronger, fundamental interactions. The spectrum measured from the momentum and angles of the decay positrons is parametrized using a set of four decay parameters. The purpose of the TWIST experiment is to measure these decay parameters to an unprecedented precision; an order of magnitude improvement in the uncertainties over measurements completed before the TWIST experiment. Measurements of the muon decay parameters constrain the values of a series of 19 weak coupling constants. In the standard model, V-A weak interaction, 18 of these constants are 0, while the remaining constant describes interactions between left handed particles, gV_LL= 1. The decay parameter quantifies the behaviour of the spectrum with respect to momentum. According to the standard model the value of this parameter is 3/4. TWIST measured a value of = 0.749910.00009(stat)0.00028(sys). The measurement is limited by its systematic uncertainty, so a large focus of the experiment was on the determination and control of these uncertainties. The systematic uncertainties are derived from uncertainties in the detector construction and uncertainties in the biases generated by differences between the data and a matching Monte Carlo. Muon decay also limits the possibility of family symmetry breaking interactions. TWIST can be used to search for the possibility of muons decaying into a positron and a single unidentified neutral particle + e+X0 that does not otherwise interact with normal matter. The large momentum and angle acceptance of the TWIST spectrometer allows for searches of two body decays for masses of the X0 boson mX0 [0,80] MeV/c, with a variety of behaviours with respect to the angle of the positron track. Upper limits on massive and mass-less X0 decays are set with a 90% confidence level separately at parts per million for massive decays and parts in.

A Precision Measurement of the Michel Parameter Ξ" in Polarised Muon Decay

A Precision Measurement of the Michel Parameter Ξ Author: Xavier Morelle
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ISBN:
Category :
Languages : en
Pages : 127

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Measurement of the Michel Parameter [rho] in Muon Decay

Measurement of the Michel Parameter [rho] in Muon Decay PDF Author: James Raymond Musser
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ISBN:
Category :
Languages : en
Pages :

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The TWIST Collaboration has measured the Michel parameter [rho] in normal muon decay, [mu] --> [epsilon]v[subscript epsilon]v̄[subscript mu]. In the standard model of particle physics, [rho] = 3/4. Deviations from this value require mixing of left- and right-handed muon and electron couplings in the muon-decay Lagrangian. We find [rho] = 0.75080 "0.00032(stat.)"0.00097(syst.) "0.00023, where the last uncertainty represents the dependence of [rho] on the Michel parameter [eta]. This result sets new limits on the W[subscript]L - W[subscript]R mixing angle in left-right symmetric models.