This program is a collaborative effort between NIST and NC State. It is designed to measure the neutron beta-decay lifetime n using a substantially new technique. Our method confines Ultra Cold Neutrons (UCN) within a three-dimensional magnetic trap. Cooling of the neutrons occurs within the conservative trap when 12 K neutrons (0.89 nm) down-scatter in superfluid 4He to near rest via single phonon emission (superthermal production). The UCN then interact only with the magnetic field via their magnetic moment and when the spin is anti-parallel to the magnetic field, they will seek to minimize their potential energy by moving towards low field regions. By cooling the trap to temperatures of approximately 100 mK, the population of UCN becomes thermally detached from the helium bath allowing accumulation of UCN to a density as high as P, where P is the superthermal production rate and  is the UCN lifetime in the source. Neutron decay is detected by turning off the cold neutron beam and observing the scintillation light resulting from the beta-decay electrons. When an electron moves through liquid helium, it ionizes helium atoms along its track. These helium ions quickly recombine into metastable He*2 molecules. About 35 % of the initial electron energy goes into the production of extreme ultraviolet (EUV) photons from singlet decays, corresponding to approximately 22 photons/keV. These EUV photons are frequency down-converted to blue photons using the organic fluor tetraphenyl butadiene (TPB) coated onto a diffuse reflector surrounding the trapping region. This light is transported via non-imaging optics to room temperature and detected by two photomultiplier tube (PMT)s operating in coincidence. This unique trapping and detection method allows us to observe neutron decay events in situ, and therefore directly measure the decay curve.
Data analysis is currently ongoing with preliminary results expected early this year. In parallel, we are constructing a new helium purifier to address helium contamination issues uncovered with AMS. The purifier is expected to be complete by summer, and should allow us to demonstrate that our unique technique holds the potential to reach sensitivities significantly beyond what has currently been achieved by other techniques.
Figure: Lifetime corrected and background sbtracted data from 17 run pairs, showing the decay curve associated with the trap lifetime.