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 EJ: Mini-Symposium on Fundamental Neutron Physics III |
Hide Abstracts |
Chair: Hirohiko Shimizu, Nagoya University Room: Hilton Kona 5 |
Thursday, October 25, 2018 7:00PM - 7:30PM |
EJ.00001: Symmetry Violation Searches with Neutrons Invited Speaker: Beatrice Franke Neutrons are a great tool for fundamental property investigations, such as symmetries. Within this context they are a complementary probe to the standard models of particle physics and cosmology as compared to the high energy frontier. Parity violation can well be studied in the weak interaction, for example through beta decay correlations and neutron lifetime. The free neutron lifetime on the other hand also affects bigbang nuclesynthesys. Additionally, time reversal symmetry violation (and thus CP symmetry by assuming CPT to be a good symmetry of nature) can be studied through the search for a permanent neutron electric dipole moment. Through this portal, neutrons also offer a handle on the Baryon Asymmetry of the Universe, and thus beyond standard model physics. Other high precision experiements with neutrons can also assess the strong CP problem by searching for beyond standard model interactions coupling through eg axions, axionlike particles, or other dark matter candidates. This presentation shall give an overview of the field and serve as introduction to the topics covered in this session. Different experimental techniques and their properties will briefly be presented, covering fundamental neutron physics as well as aspects from the hadronic sector. |
Thursday, October 25, 2018 7:30PM - 7:45PM |
EJ.00002: Progress towards a room temperature neutron electric dipole moment search at the Los Alamos Neutron Science Center Robert Pattie A discovery of the neutron's permanent electric dipole moment larger than the standard model prediction of dn≈10-31 e·cm would signal a new source of CP-violation and help explain the matter-antimatter asymmetry in the universe. Improving limits on dn constrain extensions to the standard model in a complementary fashion to the atomic and electron EDM searches. The recent upgrade of the Los Alamos ultracold neutron source makes it possible for a new room temperature search with the statistical reach to improve upon current limits by a factor of 10 or more. During the 2017 LANSCE cycle a prototype apparatus was used to demonstrate the capability to transport and manipulate polarized neutrons and perform Ramsey and Rabi sequence measurements. I will report on the measurements made over the last year, efforts underway to upgrade the prototype chamber, and possible future upgrades of the ultracold neutron source. |
Thursday, October 25, 2018 7:45PM - 8:00PM |
EJ.00003: Magnetic field apparatus for the neutron electric dipole moment search at Oak Ridge National Lab Simon Slutsky, Christopher M Swank, Wanchun Wei, Bradley Filippone, Charles Osthelder, Robert Carr A search for a neutron electric dipole moment (nEDM) will be carried out at the Oak Ridge National Laboratory's Spallation Neutron Source (SNS) with a sensitivity goal of < 3 × 10-28 e-cm. Polarized ultracold neutrons will precess in a constant magnetic holding field, B0, inside a ∼0.4 m long liquid helium cell, which will be doped with a minute amount of He-3 to measure the precession frequency. Magnetic field gradients in the cell must be reduced below 3 ppm/cm relative to B0 in order to mitigate the false nEDM signal due to the geometric phase effect and to increase the neutron and He-3 polarization lifetime. Superconducting magnetic coils ∼1.5-2 m in diameter will be operated inside a nearly-hermetic, superconducting lead shield to produce B0 and other required fields. I will discuss design efforts to meet the stringent magnetic requirement in ways that also meet the challenges of cryogenic operation, in particular the significant thermal contraction. I will also show ongoing work to prepare and validate the experiment's main aluminum cryostat for use. |
Thursday, October 25, 2018 8:00PM - 8:15PM |
EJ.00004: Measurement of Neutron Polarization and Transport for the nEDM@SNS Experiment. Syed 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. The experiment will measure the change in precession frequency of UCN and 3He via the scintillation light produced from the spin-dependent n-3He absorption. 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. |
Thursday, October 25, 2018 8:15PM - 8:30PM |
EJ.00005: Producing ultracold neutrons with a spallation source and superfluid helium Wolfgang Schreyer An electric dipole moment of the neutron large enough to detect with current techniques would be an indication of CP-violating processes beyond the standard model of particle physics and could explain the matter-antimatter asymmetry in the universe. |
Thursday, October 25, 2018 8:30PM - 8:45PM |
EJ.00006: Intense UCN production in He-II for nEDM Yasuhiro Masuda, Kensaku Matsuta, Mototsugu Mihara We have been developing a new UCN production method in a 0.8 K He-II, which is placed in a 20 kW spallation neutron source. We are aiming to obtain a UCN density of 800 UCN/cm3 in a nEDM measurement cell for a measurement of 10-27 e cm. We need to remove a γ heating of 5 W in the He-II at a proton beam power of 20 kW so that He-II temperature is kept below 0.8 K to suppress UCN loss in He-II. The heat conducts through the He-II to a 4He-3He heat exchanger, which is cooled down by a 3He cryostat. We have studied quantum effects at the heat conduction in He-II, phonons, potential flow and quantized vortices, and also an acoustic mismatch at the boundary between the He-II and the heat exchanger. We have constructed the second generation UCN source of He-II. Here, we will show how the heat in a UCN production volume is removed through a 85 mm diameter He-II by a 0.7 K 3He cryostat. Phonon heat conduction is enough to cool down the UCN production volume below 0.8 K. But, a TRIUMF-KEK group claims the quantum turbulence and the acoustic mismatch have serious effects on the heat conduction. Here, we will show we can control these effects to keep the He-II temperature below 0.8 K.
|
Thursday, October 25, 2018 8:45PM - 9:00PM |
EJ.00007: Pressure and temperature dependence of electrical breakdown in liquid helium Takeyasu Ito, Steven Clayton, Scott Currie, Nguyen Phan, John Ramsey, George M Seidel, Wanchun Wei The SNS nEDM collaboration is developing an experiment to search for the neutron’s electric dipole moment (EDM), using ultracold neutrons (UCNs) stored in superfluid liquid helium, to be run at the Spallation Neutron Source (SNS) at Oak Ridge National Laboratory. In this experiment, being able to achieve a strong and stable electric field in superfluid liquid helium in the region where UCNs are stored is of critical importance, because in EDM searches in general the sensitivity depends linearly on the strength of the applied electric field. The design goal is to stably apply a DC electric field exceeding 75 kV/cm inside measurement cells whose inner dimension is 40 cm x 7.62 cm x 10.16 cm. However, the phenomenon of electric breakdown in liquid helium is poorly understood, and as such a major R&D effort is under way. As part of this R&D effort, we measured the dependence of the breakdown field on the pressure and temperature of liquid helium using two apparatus, one with ~1cm size electrodes and the other with ~50 cm size electrodes. In this study, we present the results of these measurements and discuss their implications on the mechanism of electrical breakdown in liquid helium. |
Thursday, October 25, 2018 9:00PM - 9:15PM |
EJ.00008: 129Xe comagnetometer for neutron EDM experiment Mototsugu Mihara, Yasuhiro Masuda, Kensaku Matsuta The neutron electric dipole moment (nEDM) has been providing strict constraints on theories underlying the CP violation that predict larger nEDM than the standard model. In order to exceed the present upper limit on the nEDM of 3 × 10−26 ecm measured at Grenoble, several groups are now developing new methods of nEDM measurements to reduce systematic errors as well as new ultracold neutron (UCN) sources to achieve higher statistics. The systematic error at the Grenoble experiment was dominated by the the geometric phase effect (GPE) for the 199Hg comagnetometer. We have proposed a 129Xe comagnetometer which can possibly reduce the GPE to 4 × 10−28 ecm because of a buffer gas effect. Spin polarized 129Xe nuclei are used to monitor the static magnetic field in an nEDM cell where both spin polarized UCN and 129Xe are confined. Highly spin polarized 129Xe produced by means of the spin exchange optical pumping (SEOP) technique is accumulated in a cold trap, and then is introduced into the nEDM cell. The spin precession of 129Xe nuclei will be observed using two-photon excitation of Xe atoms. We have achieved 70% of 129Xe polarization in the SEOP cell and are now developing the cold trap. The progress of our development will be presented. |
Thursday, October 25, 2018 9:15PM - 9:30PM |
EJ.00009: Material Tests of Magnetic Instability in the Ultra-Cold Neutron EDM Apparatus at PSI Naoya Ozawa, Georg Bison, Klaus Kirch, Yasuhiro Sakemi Investigation is conducted for magnetic instability in the neutron electric dipole moment (EDM) experimental apparatus at the Paul Scherrer Institute (PSI) using optically pumped Cs magnetometers. The control of magnetic field is crucial for the measurement of EDM. Since it is probed using the energy shift induced by an applied electric field, any magnetic field fluctuation will induce a false signal of EDM due to the Zeeman effect. Therefore, the effect of magnetic fields on the energy shifts must be precisely monitored so that the real EDM effect could be precisely extracted. Metal shields cancel the magnetic fields entering the measurement region, but the material may possess an intrinsic fluctuation. Ideally, the region inside the magnetic shield must be zero-field, especially in the innermost area. During the measurement, there is a 1 μT field for spin-aligning the neutron samples, thus the magnetic field has a finite offset component. The Cs magnetometer is an excellent tool to measure such instabilities, since it can measure the magnetic fluctuations of either case using the same apparatus. This work is conducted with Georg Bison, Klaus Kirch, and Yasuhiro Sakemi for nEDM PSI Collaboration. |
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. |
© 2024 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