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19 April 2024
 
  » arxiv » 1911.5829

 Article overview


Improved limits on Fierz Interference using asymmetry measurements from the UCNA experiment
Xuan Sun ; E. Adamek ; B. Allgeier ; Y. Bagdasarova ; D. B. Berguno ; M. Blatnik ; T. J. Bowles ; L. J. Broussard ; M. A.-P. Brown ; R. Carr ; S. Clayton ; C. Cude-Woods ; S. Currie ; E. B. Dees ; X. Ding ; B. W. Filippone ; A. García ; P. Geltenbort ; S. Hasan ; K. P. Hickerson ; J. Hoagland ; R. Hong ; A. T. Holley ; T. M. Ito ; A. Knecht ; C.-Y. Liu ; J. Liu ; M. Makela ; R. Mammei ; J. W. Martin ; D. Melconian ; M. P. Mendenhall ; S. D. Moore ; C. L. Morris ; S. Nepal ; N. Nouri ; R. W. Pattie Jr. ; A. Pérez Galván ; D. G. Phillips II ; R. Picker ; M. L. Pitt ; B. Plaster ; D. J. Salvat ; A. Saunders ; E. I. Sharapov ; S. Sjue ; S. Slutsky ; W. Sondheim ; C. Swank ; E. Tatar ; R. B. Vogelaar ; B. VornDick ; Z. Wang ; W. Wei ; J. W. Wexler ; T. Womack ; C. Wrede ; A. R. Young ; B. A. Zeck ;
Date 13 Nov 2019
AbstractThe Ultracold Neutron Asymmetry (UCNA) experiment was designed to measure the $eta$-decay asymmetry parameter, $A_0$, for free neutron decay. In the experiment, polarized ultracold neutrons are transported into a decay trap, and their $eta$-decay electrons are detected with $approx 4pi$ acceptance into two detector packages which provide position and energy reconstruction. The experiment also has sensitivity to $b_{n}$, the Fierz interference term in the neutron $eta$-decay rate. In this work, we determine $b_{n}$ from the energy dependence of $A_0$ using the data taken during the UCNA 2011-2013 run. In addition, we present the same type of analysis using the earlier 2010 $A$ dataset. Motivated by improved statistics and comparable systematic errors compared to the 2010 data-taking run, we present a new $b_{n}$ measurement using the weighted average of our asymmetry dataset fits, to obtain $b_{n} = 0.066 pm 0.041_{ ext{stat}} pm 0.024_{ ext{syst}}$ which corresponds to a limit of $-0.012 < b_{n} < 0.144$ at the 90% confidence level.
Source arXiv, 1911.5829
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