A = 8 Recoil Spectroscopy with the Beta Decay Paul Trap
ORAL · Invited
Abstract
The A = 8 system is a rich playground for probing science ranging from testing the nature of the weak interaction to understanding the physics of the Sun. Through careful study of the β-delayed α-particles following the decays of 8Li and 8B, the triple coincidence measurement of β-α-α can be used to determine the β-ν angular correlation coefficient aβν in these Gamow-Teller decays to place constraints on possible Tensor currents in the weak interaction. Additionally, an α-α coincidence measurement enables a determination of the of the 8B neutrino energy spectrum. An ideal tool to study the charged particles emitted during the β-decay process are linear Paul traps. These traps suspend a cloud of radioactive ions in a high vacuum environment using static and RF electric fields, confining the cloud to a region of ~1mm3 for extended periods of time, free from interactions with a substrate, and enabling a backing free measurement of the emitted radiation following β-decay. At ANL’s ATLAS facility, the Beta-decay Paul Trap (BPT) is dedicated to studying the β-delayed α emission of 8Li and 8B. The open geometry of the BPT allows for close packing of four 64x64 mm, 1 mm thick, 32-fold segmented DSSD Si detectors, backed by four plastic scintillators, providing ~25% solid angle coverage.
We will present an overview of the A=8 program with the BPT, including measurements of aβν in 8Li and 8B and a determination of the neutrino spectrum following β-decay of 8B. In particular, we will highlight the recent results from a high-statistics measurement of the 8B dataset to determine aβν and new constraints on CT and C’T in the decay of mirror systems.
We will present an overview of the A=8 program with the BPT, including measurements of aβν in 8Li and 8B and a determination of the neutrino spectrum following β-decay of 8B. In particular, we will highlight the recent results from a high-statistics measurement of the 8B dataset to determine aβν and new constraints on CT and C’T in the decay of mirror systems.
*We acknowledge the U.S. DOE Contract No. DE-AC02-06CH11357 [ANL] and DE- AC52-07NA27344 [LLNL], the Argonne National Laboratory ATLAS facility, which is a DOE Office of Science User Facility, and NSERC, Canada, Contract Nos. SAPPJ-2015- 00034 and SAPPJ-2018-00028.
–
Presenters
-
Aaron T Gallant
- Lawrence Livermore National Lab
- Lawrence Livermore National Laboratory
- Lawrence Livermore Natl Lab