Location via proxy:   [ UP ]  
[Report a bug]   [Manage cookies]                
  • Editors' Suggestion

First Observation of P-odd γ Asymmetry in Polarized Neutron Capture on Hydrogen

D. Blyth et al. (NPDGamma Collaboration)
Phys. Rev. Lett. 121, 242002 – Published 13 December 2018

Abstract

We report the first observation of the parity-violating gamma-ray asymmetry Aγnp in neutron-proton capture using polarized cold neutrons incident on a liquid parahydrogen target at the Spallation Neutron Source at Oak Ridge National Laboratory. Aγnp isolates the ΔI=1, S31P31 component of the weak nucleon-nucleon interaction, which is dominated by pion exchange and can be directly related to a single coupling constant in either the DDH meson exchange model or pionless effective field theory. We measured Aγnp=[3.0±1.4(stat)±0.2(syst)]×108, which implies a DDH weak πNN coupling of hπ1=[2.6±1.2(stat)±0.2(syst)]×107 and a pionless EFT constant of CS31P31/C0=[7.4±3.5(stat)±0.5(syst)]×1011MeV1. We describe the experiment, data analysis, systematic uncertainties, and implications of the result.

  • Figure
  • Figure
  • Figure
  • Figure
  • Received 11 March 2018
  • Revised 22 October 2018

DOI:https://doi.org/10.1103/PhysRevLett.121.242002

© 2018 American Physical Society

Physics Subject Headings (PhySH)

Particles & Fields

Authors & Affiliations

Click to Expand

Article Text (Subscription Required)

Click to Expand

References (Subscription Required)

Click to Expand
Issue

Vol. 121, Iss. 24 — 14 December 2018

Reuse & Permissions
Access Options
CHORUS

Article Available via CHORUS

Download Accepted Manuscript
Author publication services for translation and copyediting assistance advertisement

Authorization Required


×

Images

  • Figure 1
    Figure 1

    A schematic vertical cut view of the NPDGamma experiment on the FnPB; for details see text.

    Reuse & Permissions
  • Figure 2
    Figure 2

    Plot of a typical detector voltage signal as a function of time bin for eight 60 Hz neutron pulses. The proton pulse was not delivered to the spallation target in the 2nd pulse resulting in a dropped pulse. The peak yield in the 3rd pulse is 1% low because the phosphorescence tail from the second pulse is missing. The rising (falling) edges of the pulses correspond to the choppers opening (closing). The pedestal from the β-delayed γ’s of Al28 is shown. Finally, the fiducial time interval (27 time bins wide) is shown in pulse seven (time bins 253 to 279).

    Reuse & Permissions
  • Figure 3
    Figure 3

    Histogram of hydrogen asymmetries (1/30 of all the data) for a typical detector before (left) and after (right) the cuts described in the text have been applied. Note the different x-axis scale on the right panel. The distinct side lobes in the uncut data correspond to SS in which one or more dropped pulses occurred.

    Reuse & Permissions
  • Figure 4
    Figure 4

    hπ1 from theoretical estimates or calculations (blue) and this work (red).

    Reuse & Permissions
×

Sign up to receive regular email alerts from Physical Review Letters

Log In

Cancel
×

Search


Article Lookup

Paste a citation or DOI

Enter a citation
×