Bulletin of the American Physical Society
APS April Meeting 2019
Volume 64, Number 3
Saturday–Tuesday, April 13–16, 2019; Denver, Colorado
Session L14: Fundamental Neutron Physics |
Hide Abstracts |
Sponsoring Units: DNP Chair: Shannon Hoogerheide, National Institute of Standards and Technology Room: Sheraton Plaza Court 3 |
Sunday, April 14, 2019 3:30PM - 3:42PM |
L14.00001: The Nab Experiment: A Precision Measurement of Unpolarized Neutron Beta Decay Jason A Fry Neutron beta decay is one of the most fundamental processes in nuclear physics and provides means to uncover the details of the weak interaction. Neutron beta decay can evaluate the ratio of axial-vector to vector coupling constants in the standard model, $\lambda$ = $G_A$/$G_V$ , through multiple decay correlations. The Nab experiment will carry out measurements of the electron-neutrino correlation parameter $a$ with a precision of $\delta a/a$ = 10$\times 10^{-3}$ and the Fierz interference term $b$ to $\delta b$ = 3$\times 10^{-3}$ in unpolarized free neutron beta decay. These results aim to deliver an independent and competitive determination of $\lambda$ that will allow an evaluation of $V_{ud}$ and sensitively test CKM unitarity, independent of nuclear models. Nab utilizes a novel, long asymmetric spectrometer that guides the decay electron and proton to two large area silicon detectors in order to precisely determine the electron energy and proton momentum. The Nab apparatus is under installation on the Fundamental Neutron Physics Beamline at the Spallation Neutron Source at Oak Ridge National Lab. We present the motivation, goals, and principles of the Nab experiment. |
Sunday, April 14, 2019 3:42PM - 3:54PM |
L14.00002: Magnetometry for the Nab Experiment Elizabeth M Scott Nab uses an asymmetric magnetic spectrometer and two large-area segmented Si detectors to extract the neutron beta decay electron-neutrino correlation coefficient \textit{a} and the Fierz interference term \textit{b} from the proton momentum and electron energy spectrum. Nab was designed to achieve a $10^{-3}$ relative uncertainty in \textit{a}, and this requires a detailed characterization and analysis of the magnetic field in the spectrometer. This talk will cover the design and implementation of this field characterization scheme and the current analysis. |
(Author Not Attending)
|
L14.00003: Detector Systematics for the Nab Experiment Glenn Randall The Nab experiment at the Spallation Neutron Source (SNS) will make precision measurements of the electron-neutrino correlation coefficient and the Fierz interference term for neutron beta decay. The experiment will use a novel field expansion spectrometer to measure electron energy and proton momentum. Two important systematics are detector energy calibration and time of flight shift. Energy calibration is specified as \delta E < 200eV and time of flight shift is specified as \delta t < 0.3 ns. In situ radioactive sources will be heavily used in efforts to characterize both of these systematics. Characterizing the detectors’ energy response linearity will be done using a pulser. This talk will present these systematics, their importance to Nab, plans for measurement, as well as Geant4 simulation to show the plausibility of our plans. |
Sunday, April 14, 2019 4:06PM - 4:18PM |
L14.00004: Data Acquisition and Digital Signal Processing for the Nab Experiment Michelle H Gervais, Christopher B Crawford The goal of the Nab experiment is to measure the electron-neutrino correlation parameter (a) with an uncertainty of 0.001 and the Fierz interference term (b) with an uncertainty of 0.005 by measuring both the electron and proton energy in coincidence for full kinematic reconstruction of the electron neutrino angle. In order to reach this precision, a custom DAQ system with high noise tolerance, low trigger threshold, and high acceptance rates for the multi-pixel silicon detectors is required. We have developed a new DAQ architecture based on deep onboard memory buffers and high-speed field-programmable gate arrays to streamline global trigger logic. We will present this novel system and advanced DSP filters which allow us to detect protons accelerated to 30 kV in coincidence with electrons with high efficiency and event rate. |
Sunday, April 14, 2019 4:18PM - 4:30PM |
L14.00005: Progress on the Design, Construction and Test of the Full Size Magnet for the SNS Neutron Electric Dipole Moment Search Wanchun Wei, Simon A Slutsky, Christopher M Swank, Xuan Sun, Robert Carr, Charles Osthelder, John C. Ramsey, Christopher Daurer, Larry Bartoszek, Roy J Holt, Bradley Filippone The SNS nEDM project aims to search for a neutron electric dipole moment (nEDM) at a goal sensitivity of 3x10-28 e-cm at the Spallation Neutron Source (SNS) of Oak Ridge National Laboratory (ORNL). The nEDM signal will appear as a change of the procession frequency of polarized ultracold neutrons (UCN) induced by the application of a high electric field. A uniform magnetic field over the UCN storage volume of 0.4 m long with a gradient less than 3 ppm/cm is crucial to suppress the false nEDM signal due to the geometric phase effect, and the field strength will be monitored by comagnetometer He-3. The magnetic fields will be generated by superconducting cosine-theta coils of 1.5—2 m in diameter, enclosed in a nearly-hermetic superconducting lead shield. In this talk, we will present the progress of design, construction and tests of the full size magnets and magnetic shielding as well as the cryogenic systems. The challenges and solutions will be discussed. |
Sunday, April 14, 2019 4:30PM - 4:42PM |
L14.00006: 3He Spin Transport Magnet Development for the SNS nEDM Experiment Mark H McCrea Measurements of the neutron electric dipole moment (nEDM) are one of the most important tests of the parity and time reversal symmetries with implications both to baryogenesis in the early universe and fundamental physics. The SNS nEDM experiment aims to make a measurement to an accuracy of $3\times10^{-28}$ e-cm, 100 times better than previously existing measurements that have set an upper limit on the value of the nEDM. One of the methods to be used to meet the goal accuracy will be to use polarized helium-3 both as a co-magnetometer and as part of the neutron polarization measurement process. |
Sunday, April 14, 2019 4:42PM - 4:54PM |
L14.00007: Measurement of Neutron Polarization and Transport for the nEDM@SNS Experiment. Kavish Imam The existence and size of a neutron electric dipole moment (nEDM) remains an important question in particle and cosmological physics. The nEDM@SNS experiment proposes a new limit for nEDM search by using ultra-cold neutrons (UCN) in a bath of superfluid helium. The experiment uses polarized 8.9Å neutrons to create polarized UCN in situ in superfluid helium via superthermal downscattering. This process requires 8.9Å neutrons to retain their polarization as they pass through magnetic shielding and nEDM cryostat windows. This talk will describe a setup that will allow us to measure neutron polarization loss from the magnetic shielding and cryostat windows. |
Sunday, April 14, 2019 4:54PM - 5:06PM |
L14.00008: Scintillation from Charged Particles in Liquid Helium Nguyen Phan Studies of scintillation in liquid helium resulting from the passage of charged particles is of both practical and theoretical interests. Recently, a diverse range of experiments including the search for the neutron electric dipole moment (nEDM), the measurement of the neutron-decay lifetime, solar neutrino detection, and the search for dark matter have used or proposed the use of liquid helium scintillators. With such broad applications, many properties of the scintillation remain to be explored. I will discuss the ongoing R&D effort at Los Alamos National Laboratory to measure scintillation from liquid helium under conditions pertinent to the proposed nEDM experiment at the Spallation Neutron Source (SNS). Important to this effort is an understanding of the dependence of the scintillation light produced by different particles (alphas, electrons, protons, tritons) when the liquid is subjected to high electric fields (10’s of kV/cm) over a wide range of temperatures (0.5 K – 4K) and pressures. |
Sunday, April 14, 2019 5:06PM - 5:18PM |
L14.00009: Development of a Cryogenic High Voltage Multiplier Steven Clayton A classic electrostatic induction machine, Cavallo's multiplier, can be used for in situ production of very high voltage in cryogenic environments, starting with a much more modest high voltage fed in from outside the cryostat. The device is suitable for generating a large electrostatic field under conditions of very small load current. This talk will describe efforts to develop this device for a cryogenic neutron electric dipole moment experiment, in which a measurement cell filled with and surrounded by sub-1 Kelvin liquid helium is expected to withstand a working voltage of 650 kV across ≈8 cm. This talk will describe a cryogenic test apparatus, currently under construction at Los Alamos National Laboratory, to develop a Cavallo apparatus for the nEDM experiment and to test the effect of nearby sparks on SQUID magnetometers. |
Sunday, April 14, 2019 5:18PM - 5:30PM |
L14.00010: Progress toward a new room temperature neutron electric dipole moment search at the Los Alamos Neutron Science Center Robert W Pattie
|
Follow Us |
Engage
Become an APS Member |
My APS
Renew Membership |
Information for |
About APSThe American Physical Society (APS) is a non-profit membership organization working to advance the knowledge of physics. |
© 2025 American Physical Society
| All rights reserved | Terms of Use
| Contact Us
Headquarters
1 Physics Ellipse, College Park, MD 20740-3844
(301) 209-3200
Editorial Office
100 Motor Pkwy, Suite 110, Hauppauge, NY 11788
(631) 591-4000
Office of Public Affairs
529 14th St NW, Suite 1050, Washington, D.C. 20045-2001
(202) 662-8700