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Dive into the research topics where M. P. Mendenhall is active.

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Featured researches published by M. P. Mendenhall.


Physical Review Letters | 2010

Determination of the axial-vector weak coupling constant with ultracold neutrons.

J. Liu; M. P. Mendenhall; Adam Holley; H. O. Back; T. J. Bowles; L. J. Broussard; R. Carr; S. Clayton; S. Currie; B. W. Filippone; Alejandro García; P. Geltenbort; K. P. Hickerson; J. Hoagland; Gary E. Hogan; B. Hona; T. M. Ito; C.-Y. Liu; M. Makela; R. R. Mammei; J. W. Martin; D. Melconian; C. L. Morris; R. W. Pattie; A. Pérez Galván; M. L. Pitt; B. Plaster; J. C. Ramsey; R. Rios; R. Russell

A precise measurement of the neutron decay β asymmetry A₀ has been carried out using polarized ultracold neutrons from the pulsed spallation ultracold neutron source at the Los Alamos Neutron Science Center. Combining data obtained in 2008 and 2009, we report A₀ = -0.119 66±0.000 89{-0.001 40}{+0.001 23}, from which we determine the ratio of the axial-vector to vector weak coupling of the nucleon g{A}/g{V}=-1.275 90{-0.004 45}{+0.004 09}.


Physical Review C | 2012

Measurement of the neutron β -asymmetry parameter A 0 with ultracold neutrons

B. Plaster; R. Carr; B. W. Filippone; K. P. Hickerson; T. M. Ito; Jianbei Liu; J. W. Martin; M. P. Mendenhall; A. Pérez Galván; R. Russell; R. Schmid; B. Tipton; Junhua Yuan

We present a detailed report of a measurement of the neutron β-asymmetry parameter A_0, the parity-violating angular correlation between the neutron spin and the decay electron momentum, performed with polarized ultracold neutrons (UCN). UCN were extracted from a pulsed spallation solid deuterium source and polarized via transport through a 7-T magnetic field. The polarized UCN were then transported through an adiabatic-fast-passage spin-flipper field region, prior to storage in a cylindrical decay volume situated within a 1-T 2×2π solenoidal spectrometer. The asymmetry was extracted from measurements of the decay electrons in multiwire proportional chamber and plastic scintillator detector packages located on both ends of the spectrometer. From an analysis of data acquired during runs in 2008 and 2009, we report A_0=−0.11966±0.00089_(−0.00140)^(+0.00123), from which we extract a value for the ratio of the weak axial-vector and vector coupling constants of the nucleon, λ=g_A/g_V=−1.27590±0.00239_(−0.00377)^(+0.00331). Complete details of the analysis are presented.


Physical Review C | 2013

Precision measurement of the neutron β-decay asymmetry

M. P. Mendenhall; R. Carr; B. W. Filippone; K. P. Hickerson; J. L. Liu; A. Pérez Galván; R. Picker

A new measurement of the neutron β-decay asymmetry A_0 has been carried out by the UCNA Collaboration using polarized ultracold neutrons (UCNs) from the solid deuterium UCN source at the Los Alamos Neutron Science Center. Improvements in the experiment have led to reductions in both statistical and systematic uncertainties leading to A_0=−0.11954(55)_(stat)(98)_(syst), corresponding to the ratio of axial-vector to vector coupling λ ≡ g_A/g_V = −1.2756(30).


Physical Review C | 2013

Precision Measurement of the Neutron Beta-Decay Asymmetry

M. P. Mendenhall; R. W. Pattie; Y. Bagdasarova; D. B. Berguno; L. J. Broussard; R. Carr; S. Currie; X. Ding; B. W. Filippone; A. Garc; P. Geltenbort; K. P. Hickerson; J. Hoagland; Adam Holley; R. Hong; Takeyasu M. Ito; A. Knecht; Y. Liu; J. Liu; M. Makela; R. R. Mammei; J. W. Martin; Dan Melconian; S. D. Moore; C. L. Morris; M. L. Pitt; B. Plaster; J. C. Ramsey; R. Rios; A. Saunders

A new measurement of the neutron β-decay asymmetry A_0 has been carried out by the UCNA Collaboration using polarized ultracold neutrons (UCNs) from the solid deuterium UCN source at the Los Alamos Neutron Science Center. Improvements in the experiment have led to reductions in both statistical and systematic uncertainties leading to A_0=−0.11954(55)_(stat)(98)_(syst), corresponding to the ratio of axial-vector to vector coupling λ ≡ g_A/g_V = −1.2756(30).


Physical Review C | 2012

Measurement of the neutron

B. Plaster; J. Hoagland; R. W. Pattie; S. Clayton; P. Geltenbort; R. Mortensen; C. Wrede; A. García; H. Yan; T. J. Bowles; A. Saunders; B. W. Filippone; R. Rios; Dan Melconian; R. R. Mammei; R. Carr; Jianbei Liu; B. Hona; B. VornDick; M. Makela; A. R. Young; K. P. Hickerson; H. O. Back; M. P. Mendenhall; R. B. Vogelaar; T. M. Ito; S. J. Seestrom; J. C. Ramsey; Gary E. Hogan; W. E. Sondheim

We present a detailed report of a measurement of the neutron β-asymmetry parameter A_0, the parity-violating angular correlation between the neutron spin and the decay electron momentum, performed with polarized ultracold neutrons (UCN). UCN were extracted from a pulsed spallation solid deuterium source and polarized via transport through a 7-T magnetic field. The polarized UCN were then transported through an adiabatic-fast-passage spin-flipper field region, prior to storage in a cylindrical decay volume situated within a 1-T 2×2π solenoidal spectrometer. The asymmetry was extracted from measurements of the decay electrons in multiwire proportional chamber and plastic scintillator detector packages located on both ends of the spectrometer. From an analysis of data acquired during runs in 2008 and 2009, we report A_0=−0.11966±0.00089_(−0.00140)^(+0.00123), from which we extract a value for the ratio of the weak axial-vector and vector coupling constants of the nucleon, λ=g_A/g_V=−1.27590±0.00239_(−0.00377)^(+0.00331). Complete details of the analysis are presented.


Physical Review C | 2017

\beta

K. P. Hickerson; X. Sun; R. Carr; B. W. Filippone; J. Liu; M. P. Mendenhall; A. Pérez Galván; R. Picker

Precision measurements of free-neutron β decay have been used to precisely constrain our understanding of the weak interaction. However, the neutron Fierz interference term b_n, which is particularly sensitive to beyond-standard-model tensor currents at the TeV scale, has thus far eluded measurement. Here we report the first direct constraints on this term, finding b_n=0.067±0.005_(stat)^(+0.090)_(−0.061)_(sys), consistent with the standard model. The uncertainty is dominated by absolute energy reconstruction and the linearity of the β spectrometer energy response.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2017

-asymmetry parameter

S. Slutsky; C.M. Swank; A. Biswas; R. Carr; J. Escribano; B. W. Filippone; W. C. Griffith; M. P. Mendenhall; N. Nouri; C. Osthelder; A. Pérez Galván; R. Picker; B. Plaster

A magnetic coil operated at cryogenic temperatures is used to produce spatial, relative field gradients below 6 ppm/cm, stable for several hours. The apparatus is a prototype of the magnetic components for a neutron electric dipole moment (nEDM) search, which will take place at the Spallation Neutron Source (SNS) at Oak Ridge National Laboratory using ultra-cold neutrons (UCN). That search requires a uniform magnetic field to mitigate systematic effects and obtain long polarization lifetimes for neutron spin precession measurements. This paper details upgrades to a previously described apparatus [1], particularly the introduction of super-conducting magnetic shielding and the associated cryogenic apparatus. The magnetic gradients observed are sufficiently low for the nEDM search at SNS.


Physical Review C | 2013

A_0

M. P. Mendenhall; R. W. Pattie; Y. Bagdasarova; D. B. Berguno; L. J. Broussard; R. Carr; S. Currie; X. Ding; B. W. Filippone; A. García; P. Geltenbort; K. P. Hickerson; J. Hoagland; Adam Holley; R. Hong; T. M. Ito; A. Knecht; C.-Y. Liu; J. Liu; M. Makela; R. R. Mammei; J. W. Martin; Dan Melconian; S. D. Moore; C. L. Morris; A. Pérez Galván; R. Picker; M. L. Pitt; B. Plaster; J. C. Ramsey

A new measurement of the neutron β-decay asymmetry A_0 has been carried out by the UCNA Collaboration using polarized ultracold neutrons (UCNs) from the solid deuterium UCN source at the Los Alamos Neutron Science Center. Improvements in the experiment have led to reductions in both statistical and systematic uncertainties leading to A_0=−0.11954(55)_(stat)(98)_(syst), corresponding to the ratio of axial-vector to vector coupling λ ≡ g_A/g_V = −1.2756(30).


Physical Review C | 2012

with ultracold neutrons

B. Plaster; R. Rios; H. O. Back; T. J. Bowles; L. J. Broussard; R. Carr; S. Clayton; S. Currie; B. W. Filippone; A. García; P. Geltenbort; K. P. Hickerson; J. Hoagland; Gary E. Hogan; B. Hona; Adam Holley; T. M. Ito; C.-Y. Liu; Jianbei Liu; M. Makela; R. R. Mammei; J. W. Martin; Dan Melconian; M. P. Mendenhall; C. L. Morris; R. Mortensen; R. W. Pattie; A. Pérez Galván; M. L. Pitt; J. C. Ramsey

We present a detailed report of a measurement of the neutron β-asymmetry parameter A_0, the parity-violating angular correlation between the neutron spin and the decay electron momentum, performed with polarized ultracold neutrons (UCN). UCN were extracted from a pulsed spallation solid deuterium source and polarized via transport through a 7-T magnetic field. The polarized UCN were then transported through an adiabatic-fast-passage spin-flipper field region, prior to storage in a cylindrical decay volume situated within a 1-T 2×2π solenoidal spectrometer. The asymmetry was extracted from measurements of the decay electrons in multiwire proportional chamber and plastic scintillator detector packages located on both ends of the spectrometer. From an analysis of data acquired during runs in 2008 and 2009, we report A_0=−0.11966±0.00089_(−0.00140)^(+0.00123), from which we extract a value for the ratio of the weak axial-vector and vector coupling constants of the nucleon, λ=g_A/g_V=−1.27590±0.00239_(−0.00377)^(+0.00331). Complete details of the analysis are presented.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2011

First direct constraints on Fierz interference in free-neutron β decay

A. Pérez Galván; B. Plaster; J. Boissevain; R. Carr; B. W. Filippone; M. P. Mendenhall; R. Schmid; R. Alarcon; S. Balascuta

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B. W. Filippone

California Institute of Technology

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K. P. Hickerson

California Institute of Technology

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R. Carr

California Institute of Technology

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B. Plaster

California Institute of Technology

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M. Makela

Los Alamos National Laboratory

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A. Pérez Galván

California Institute of Technology

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Adam Holley

North Carolina State University

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C. L. Morris

Los Alamos National Laboratory

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