Bulletin of the American Physical Society
5th Joint Meeting of the APS Division of Nuclear Physics and the Physical Society of Japan
Volume 63, Number 12
Tuesday–Saturday, October 23–27, 2018; Waikoloa, Hawaii
Session FD: Electroweak Experiment and Theory
9:00 AM–11:30 AM,
Friday, October 26, 2018
Hilton
Room: Kohala 3
Chair: Dinko Pocanic, University of Virginia
Abstract ID: BAPS.2018.HAW.FD.6
Abstract: FD.00006 : Precise Half-Life Measurement of 30S
10:15 AM–10:30 AM
Presenter:
V.E. Iacob
(Cyclotron Institute, Texas A&M University, College Station, Texas 77843, USA)
Authors:
V.E. Iacob
(Cyclotron Institute, Texas A&M University, College Station, Texas 77843, USA)
J.C. Hardy
(Cyclotron Institute, Texas A&M University, College Station, Texas 77843, USA)
L. Chen
(Cyclotron Institute, Texas A&M University, College Station, Texas 77843, USA)
V. Horvat
(Cyclotron Institute, Texas A&M University, College Station, Texas 77843, USA)
M. Bencomo
(Cyclotron Institute, Texas A&M University, College Station, Texas 77843, USA)
N. Nica
(Cyclotron Institute, Texas A&M University, College Station, Texas 77843, USA)
H.I. Park
(Cyclotron Institute, Texas A&M University, College Station, Texas 77843, USA)
B.T. Roeder
(Cyclotron Institute, Texas A&M University, College Station, Texas 77843, USA)
A. Saastamoinen
(Cyclotron Institute, Texas A&M University, College Station, Texas 77843, USA)
As part of our program to test the unitarity of the Cabibbo-Kobayashi-Maskawa (CKM) matrix via 0+→0+ superallowed β decays, we measured the half-life of 30S. The radioactive beam was produced by the 1H(31P, 2n)30S reaction, in which a 30A MeV primary 31P beam bombarded a hydrogen target held at liquid nitrogen temperature and a pressure of 2.0 atm. With the MARS spectrograph we selected a high-purity 30S beam from the recoils. The beam was then extracted in air, passed through a 0.3-mm-thick BC-404 plastic scintillator and a set of Al degraders, adjusted to stop the 30S nuclei in the center of the 76-μm-thick aluminized-mylar tape of our fast tape-transport system. We collected 30S nuclei for 2.4 s; then the beam was switched off and the activity was moved in less than 0.2 s to the center of a 4π proportional counter. The observed decays were then multi-scaled over 24 s. Such collect-move-detect cycles were repeated until a total of 1.4×108 decays were recorded. We split the experiment into 33 runs, each differing from the others in its discriminator threshold, detector bias or dominant dead-time. No systematic effects were identified in these parameters. We found the half-life of 30S to be 1.17992(34) s, a result that is 5 times more precise than any previous measurement.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.HAW.FD.6
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