2019
DOI: 10.1103/physrevc.100.015501
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Monte Carlo simulations of trapped ultracold neutrons in the UCNτ experiment

Abstract: In the UCNτ experiment, ultracold neutrons (UCN) are confined by magnetic fields and the Earth's gravitational field. Field-trapping mitigates the problem of UCN loss on material surfaces, which caused the largest correction in prior neutron experiments using material bottles. However, the neutron dynamics in field traps differ qualitatively from those in material bottles. In the latter case, neutrons bounce off material surfaces with significant diffusivity and the population quickly reaches a static spatial … Show more

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Cited by 6 publications
(3 citation statements)
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“…of UCN velocity-and-angle-averaged loss per bounce of ð2 AE 1Þ × 10 −4 for aluminum, leading to a 0.15 AE 0.07 s correction to this subset of data. The other analyses perform similar assessments, and independent checks using our Monte Carlo framework[42] are consistent with this estimate. Further, this is consistent with a comparison of paired τ n during this period to the rest of the paired τ n values.…”
supporting
confidence: 66%
“…of UCN velocity-and-angle-averaged loss per bounce of ð2 AE 1Þ × 10 −4 for aluminum, leading to a 0.15 AE 0.07 s correction to this subset of data. The other analyses perform similar assessments, and independent checks using our Monte Carlo framework[42] are consistent with this estimate. Further, this is consistent with a comparison of paired τ n during this period to the rest of the paired τ n values.…”
supporting
confidence: 66%
“…This provided a variable counting time of a few seconds, depending on the thickness of the 10 B coating, and minimized errors introduced by the coupling between the phase space of the UCN and the time at which the UCN are counted. A detailed discussion of Phase space evolution in this trap is given by Callahan et al [30] Here we report a set of measurements made using the same experimental apparatus with the same UCN loading procedures, but with the neutrons counted at the end of storage by unloading through the trap door into an external detector. The time constant for counting UCN in a dagger with a 20 nm 10 B coating lowered to the bottom of the trap is 7.1(2) s. The time constant for unloading UCN in this experiment is 26.8(8) s. Although these experiments share many sources of systematic uncertainties, the coupling between phase space evolution and counting could be much larger in this experiment, because of the longer unloading time.…”
Section: Methodsmentioning
confidence: 99%
“…[7,108] for reviews), also the difference between recent bottle measurements [8,109,110] currently leads to a non-negligible scale factor in the PDG average [3]. Fortunately, there are plans to probe τ n at a level down to hundreds of ms [111][112][113][114].…”
Section: Observablementioning
confidence: 99%