99 research outputs found
The Cosmic Ray Muon Flux at WIPP
In this work a measurement of the muon intensity at the Waste Isolation Pilot
Plant (WIPP) near Carlsbad, NM, USA is presented. WIPP is a salt mine with a
depth of 655 m. The vertical muon flux was measured with a two panels
scintillator coincidence setup to
Phi_{vert}=3.10(+0.05/-0.07)*10^(-7)s^(-1)cm^(-2)sr^(-1).Comment: 18 pages, p figure
A proposed measurement of the Ă asymmetry in neutron decay with the Los Alamos Ultra-Cold Neutron Source
This article reviews the status of an experiment to study the neutron spin-electron angular correlation with the Los Alamos Ultra-Cold Neutron (UCN) source. The experiment will generate UCNs from a novel solid deuterium, spallation source, and polarize them in a solenoid magnetic field. The experiment spectrometer will consist of a neutron decay region in a solenoid magnetic field combined with several different detector possibilities. An electron beam and a magnetic spectrometer will provide a precise, absolute calibration for these detectors. An A-correlation measurement with a relative precision of 0.2% is expected by the end of 2002
First Measurement of the Neutron -Asymmetry with Ultracold Neutrons
We report the first measurement of angular correlation parameters in neutron
-decay using polarized ultracold neutrons (UCN). We utilize UCN with
energies below about 200 neV, which we guide and store for s in a Cu
decay volume. The potential of a static 7 T field
external to the decay volume provides a 420 neV potential energy barrier to the
spin state parallel to the field, polarizing the UCN before they pass through
an adiabatic fast passage (AFP) spin-flipper and enter a decay volume, situated
within a 1 T, superconducting solenoidal spectrometer. We
determine a value for the -asymmetry parameter , proportional to
the angular correlation between the neutron polarization and the electron
momentum, of .Comment: 4 pages, 2 figures, 1 table, submitted to Phys. Rev. Let
Demonstration of a solid deuterium source of ultra-cold neutrons
Ultra-cold neutrons (UCN), neutrons with energies low enough to be confined
by the Fermi potential in material bottles, are playing an increasing role in
measurements of fundamental properties of the neutron. The ability to
manipulate UCN with material guides and bottles, magnetic fields, and gravity
can lead to experiments with lower systematic errors than have been obtained in
experiments with cold neutron beams. The UCN densities provided by existing
reactor sources limit these experiments. The promise of much higher densities
from solid deuterium sources has led to proposed facilities coupled to both
reactor and spallation neutron sources. In this paper we report on the
performance of a prototype spallation neutron-driven solid deuterium source.
This source produced bottled UCN densities of 145 +/-7 UCN/cm3, about three
times greater than the largest bottled UCN densities previously reported. These
results indicate that a production UCN source with substantially higher
densities should be possible
Final results for the neutron ÎČ-asymmetry parameter Aâ from the UCNA experiment
The UCNA experiment was designed to measure the neutron ÎČ-asymmetry parameter A0 using polarized ultracold neutrons (UCN). UCN produced via downscattering in solid deuterium were polarized via transport through a 7âT magnetic field, and then directed to a 1âT solenoidal electron spectrometer, where the decay electrons were detected in electron detector packages located on the two ends of the spectrometer. A value for A0 was then extracted from the asymmetry in the numbers of counts in the two detector packages. We summarize all of the results from the UCNA experiment, obtained during run periods in 2007, 2008â2009, 2010, and 2011â2013, which ultimately culminated in a 0.67% precision result for Aâ
Mechanistic insight into proton-coupled mixed valency
Stabilisation of the mixed-valence state in [Mo2(TiPB)3(HDOP)]2+ (HTiPB = 2,4,6-triisopropylbenzoic acid, H2DOP = 3,6-dihydroxypyridazine) by electron transfer (ET) is related to the proton coordinate of the bridging ligands. Spectroelectrochemical studies suggest that ET is slower than 109 sâ1. The mechanism has been probed using DFT calculations, which show that proton transfer induces a larger dipole in the molecule resulting in ET
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