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 DG: Mini-Symposium on Fundamental Symmetries (Many-body Systems) II |
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Chair: John Behr, TRIUMF Room: Hilton King's 3 |
Thursday, October 25, 2018 9:00AM - 9:15AM |
DG.00001: Searching for Tensor Currents in the Weak Interaction Using 8B β Decay Aaron Gallant, Ralph Segel, Nicholas David Scielzo, Peter Mueller, Fritz Buchinger, Barbra Alan, Mary Burkey, Jason A Clark, Tsviki Hirsh, Kyle G Leach, Karolina Kolos, Bernhard Maaß, Wilfried Nörtershäuser, Rodney Orford, Guy Savard, Kumar Sharma The β decays of the A = 8 system present a unique window to study several aspects of the electroweak interaction with unprecedented accuracy. Studying the β-α-ν correlation from the β decay of 8B tests the fundamental “vector minus axial vector” (V-A) nature of the weak interaction by searching for possible tensor couplings. Using the β-decay Paul Trap (BPT) at Argonne National Laboratory we report a limit on the tensor coupling in 8B. We will also discuss both improvements to the BPT system and to the production of 8B with the goal of collecting ~2·106 β-α-α coincidences. |
Thursday, October 25, 2018 9:15AM - 9:30AM |
DG.00002: Branching-Ratio Measurements for Superallowed β Emitters at NIRS-HIMAC Daiki Nishimura, Mitsunori Fukuda, Akira Honma, Yuichi Ichikawa, Atsushi Kitagawa, Kensaku Matsuta, Mototsugu Mihara, Takashi Ohtsubo, Masaomi Tanaka, Shinji Sato The ft values for the superallowed 0+ → 0+ Fermi β decays provide valuable information on the CVC hypothesis, the unitarity of CKM matrix, and the isospin-symmetry breaking. The ft values for the 13 superallowed β emitters have been already determined very precisely. However, the emitters of 18Ne and 30S have not been determined yet due to large uncertainties of the branching ratios. Because they have the β feeding to both of the excited states including the 0+ state and the ground state, we have to measure not relative gamma intensities but absolute ones. The new precise branching-ratio measurement system is being developed. Our test measurement was carried out at NIRS-HIMAC. The secondary beam including 18Ne(30S) was produced with the projectile fragmentation reaction of 20Ne(36Ar) on a polyethylene target. The beam was separated and identified by passing through the secondary beam line and was implanted in a 6-mm-thick GSO active stopper surrounded by four clover Ge detectors. The β particles and γ rays were detected by the GSO stopper and the Ge detectors, respectively. We will report the current status of our results and a future plan to improve performance with movable active stoppers. |
Thursday, October 25, 2018 9:30AM - 9:45AM |
DG.00003: Measurements of beta-energy spectra in nuclear beta decay with a calorimetric technique Oscar Naviliat-Cuncic, Elizabeth A George, Xueying Huyan, Maximilian N Hughes, Paul A Voytas Searches for exotic tensor interactions in beta decay have motivated new measurements of beta-energy spectra in allowed Gamow-Teller transitions. Such measurements enable the most direct access to the Fierz interference term which constitutes a very sensitive probe to the presence of exotic couplings. We have implemented a calorimetric technique which makes use of high energy beams produced at the National Superconducting Cyclotron Laboratory. The technique eliminates the major instrumental effect related to the back-scattering of beta particles in surrounding matter and detectors but poses other specific challenges. We have performed measurements in the decays of $^6$He and $^{20}$F. In this contribution we describe the status of the data analysis with emphasis on the discussion of specific systematic effects. |
Thursday, October 25, 2018 9:45AM - 10:00AM |
DG.00004: In Situ Characterization of Beta Scattering at TRINAT Dan Melconian, Benjamin B Fenker, Melissa J Anholm, Danny Ashery, John A Behr, Iuliana Cohen, Alexandre Gorelov, Gerald Gwinner, James C McNeil Recently, the TRINAT collaboration reported a 0.32\% measurement of the $\beta$ asymmetry parameter, $A_\beta$, in the isobaric analgue decay of polarized $^{37}$K [PRL {\bf 120} (2018)]. The statistical and systematic uncertainty components are equal at 0.23\%, with the largest systematic sources arising from backgrounds (0.14\%) and $\beta$ scattering (0.12\%). We are able to test our GEANT4 modelling of $\beta$ scattering using a small subset of the data which we veto in the main analysis: events in our $\beta$ telescopes which register two separate pixels in the double-sided Si-strip detector along with a signal in the plastic scinitillator are predominantly due to $\beta$s which backscatter out of the scintillator. |
Thursday, October 25, 2018 10:00AM - 10:15AM |
DG.00005: Analysis of MTV experiment at TRIUMF about electron spin correlations in polarized 8Li beta decay Fumiya Goto, Hidetada Baba, John A Behr, Takuma Kajihara, Hirokazu Kawamura, Masaaki Kitaguchi, Phil Levy, Hidetada Masuda, Jiro Murata, Yusuke Nakaya, Sachi Ozaki, Matthew Pearson, Yuko Sakamoto, Hirohiko M Shimizu, Yuta Shimizu, Rei Takenaka, Kotaro Tamura, Saki Tanaka, Yumi Totsuka, Etsuko Watanabe, Yuji Yamawaki, Mami Yokohashi A large CP-Violation (considering CPT theorem, that also means T-violation) is required to explain matter dominated universe. It implies an existence of large T-Vioalation. In nuclear beta decay, T-Violation effect caused by CKM theory is much smaller than experimental resolution. If significant T-violation signal would be observed in nuclear system, it could be an evidence of new physics. Beta decay rate function includes electron spin correlation coefficients. We are interested in R and N correlation. These correlations are related to electron transverse polarization. R-correlation is P- and T-ood term which is sensitive to T-Violation. N-correlation has not measured in nuclear beta decay yet. In addition, N-correlation can be used as reference of analyzing power S which is the measuring sensitivity. In MTV (Mott Polarimetry for T-Violation) experiment, Mott scattered electron’s tracks are detected with cylindrical drift chamber(CDC). We measured the electron scattering angle asymmetry caused from electron transverse polarization. We will discuss the result of our latest data acquisition and analysis. |
Thursday, October 25, 2018 10:15AM - 10:30AM |
DG.00006: TAMUTRAP facility: A Penning trap facility for weak interaction studies. Praveen D Shidling, Veli Kolhinen, Benjamin Schroeder, Nasser Morgan, Asim Ozmetin, Dan G. Melconian TAMUTRAP is Texas A&M University Penning trap facility (TAMUTRAP) that will be used to perform precision experiments with short lived radioactive isotopes. The initial experimental program at the TAMUTRAP facility will be to search for possible scalar currents by measuring the β-ν angular correlation parameter, aβν , for T = 2 super-allowed β-delayed proton emitters. The information about the angular correlation parameter (aβν) will be extracted by observing the proton energy distribution. The experiment will be centered around a unique, large bore cylindrical Penning trap with inner radius of 90 mm, which is larger than any existing trap. This large radius Penning trap will allow full radial containment of decay products (4π acceptance) of interest, for aβν studies. Recently, TAMUTRAP facility was commissioned and demonstrated the ability of performing high precision mass measurement using a unique, compensated cylindrical Penning trap that employs a specially optimized length/radius(l/r = 3.72) ratio in the electrode structure that is not used by any other facility. In this talk, an overview of the TAMUTRAP facility will be presented.
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Thursday, October 25, 2018 10:30AM - 10:45AM |
DG.00007: Deep Learning for Liquid Scintillator-Based Double-Beta Decay Searches Aobo Li, Christopher P Grant, Suzannah A Fraker, Lindley A Winslow, Andrey Elagin Liquid scintillator-based (LS) detectors are one of the leading technologies in the search for neutrinoless double-beta decay. They are currently limited by naturally occurring and spallation-induced backgrounds. In the future, they will be limited by the neutrino-electron scattering of Boron-8 solar neutrinos. Here we use a convolutional neural network, a common algorithm from computer vision, to distinguish between signal and background events that would have made it through existing cuts. The network was trained on the MC events for different levels of photocathode coverage and quantum efficiency to demonstrate its performance under these parameters. The ultimate goal is to apply sophisticated machine learning techniques to reject backgrounds in real detector data. |
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