Daniel Salvat
Los Alamos National Laboratory
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by Daniel Salvat.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2015
Zhehui Wang; Mark A. Hoffbauer; C. L. Morris; Nathan Callahan; E. R. Adamek; Jeffrey Bacon; M. Blatnik; Aaron Brandt; L. J. Broussard; Steven Clayton; C. Cude-Woods; S. Currie; E. B. Dees; X. Ding; J. Gao; F. Gray; K. P. Hickerson; A. T. Holley; Takeyasu M. Ito; Ching Liu; M. Makela; J. C. Ramsey; Robert Pattie; Daniel Salvat; A. Saunders; D. W. Schmidt; R. K. Schulze; S. J. Seestrom; E. I. Sharapov; A. Sprow
Abstract A multilayer surface detector for ultracold neutrons (UCNs) is described. The top 10 B layer is exposed to vacuum and directly captures UCNs. The ZnS:Ag layer beneath the 10 B layer is a few microns thick, which is sufficient to detect the charged particles from the 10 B(n,α) 7 Li neutron-capture reaction, while thin enough that ample light due to α and 7 Li escapes for detection by photomultiplier tubes. A 100-nm thick 10 B layer gives high UCN detection efficiency, as determined by the mean UCN kinetic energy, detector materials, and other parameters. Low background, including negligible sensitivity to ambient neutrons, has also been verified through pulse-shape analysis and comparison with other existing 3 He and 10 B detectors. This type of detector has been configured in different ways for UCN flux monitoring, development of UCN guides and neutron lifetime research.
Physical Review C | 2018
M. A. P. Brown; E. B. Dees; E. R. Adamek; B. Allgeier; M. Blatnik; T. J. Bowles; L. J. Broussard; R. Carr; Steven Clayton; C. Cude-Woods; S. Currie; X. Ding; B. W. Filippone; A. García; P. Geltenbort; S. Hasan; K. P. Hickerson; J. Hoagland; R. Hong; G. E. Hogan; A. T. Holley; Takeyasu M. Ito; A. Knecht; Ching Liu; J. Liu; M. Makela; J. W. Martin; D. Melconian; M. P. Mendenhall; S. D. Moore
Background: The neutron β-decay asymmetry parameter A_0 defines the angular correlation between the spin of the neutron and the momentum of the emitted electron. Values for A_0 permit an extraction of the ratio of the weak axial-vector to vector coupling constants, λ≡gA/gV, which under assumption of the conserved vector current hypothesis (gV=1) determines gA. Precise values for gA are important as a benchmark for lattice QCD calculations and as a test of the standard model. Purpose: The UCNA experiment, carried out at the Ultracold Neutron (UCN) source at the Los Alamos Neutron Science Center, was the first measurement of any neutron β-decay angular correlation performed with UCN. This article reports the most precise result for A_0 obtained to date from the UCNA experiment, as a result of higher statistics and reduced key systematic uncertainties, including from the neutron polarization and the characterization of the electron detector response. Methods: UCN produced via the downscattering of moderated spallation neutrons in a solid deuterium crystal were polarized via transport through a 7 T polarizing magnet and a spin flipper, which permitted selection of either spin state. The UCN were then contained within a 3-m long cylindrical decay volume, situated along the central axis of a superconducting 1 T solenoidal spectrometer. With the neutron spins then oriented parallel or anti-parallel to the solenoidal field, an asymmetry in the numbers of emitted decay electrons detected in two electron detector packages located on both ends of the spectrometer permitted an extraction of A_0. Results: The UCNA experiment reports a new 0.67% precision result for A_0 of A_0=−0.12054(44)_(stat)(68)_(syst), which yields λ=gA/gV=−1.2783(22). Combination with the previous UCNA result and accounting for correlated systematic uncertainties produces A0=−0.12015(34)stat(63)syst and λ=gA/gV=−1.2772(20). Conclusions: This new result for A0 and gA/gV from the UCNA experiment has provided confirmation of the shift in values for gA/gV that has emerged in the published results from more recent experiments, which are in striking disagreement with the results from older experiments. Individual systematic corrections to the asymmetries in older experiments (published prior to 2002) were >10%, whereas those in the more recent ones (published after 2002) have been of the scale of <2%. The impact of these older results on the global average will be minimized should future measurements of A0 reach the 0.1% level of precision with central values near the most recent results.
Physical Review C | 2013
E. I. Sharapov; C. L. Morris; M. Makela; A. Saunders; E. R. Adamek; Yelena Bagdasarova; L. J. Broussard; C. Cude-Woods; Deon E Fellers; P. Geltenbort; Syed Hasan; K. P. Hickerson; Gary E. Hogan; A. T. Holley; Chen-Yu Liu; M. P. Mendenhall; J. Ortiz; Robert Pattie; D. G. Phillips; J. C. Ramsey; Daniel Salvat; S. J. Seestrom; E. Shaw; Sky Sjue; W. E. Sondheim; B. VornDick; Zhehui Wang; T. L. Womack; A. R. Young; B. A. Zeck
The study of neutron cross sections for elements used as efficient “absorbers” of ultracold neutrons (UCN) is crucial for many precision experiments in nuclear and particle physics, cosmology and gravity. In this context, “absorption” includes both the capture and upscattering of neutrons to the energies above the UCN energy region. The available data, especially for hydrogen, do not agree between themselves or with the theory. In this report we describe measurements performed at the Los Alamos National Laboratory UCN facility of the UCN upscattering cross sections for vanadium and for hydrogen in CH_2 using simultaneous measurements of the radiative capture cross sections for these elements. We measured σ_(up)=1972±130 b for hydrogen in CH_2, which is below theoretical expectations, and σ_(up)=25±9 b for vanadium, in agreement with the expectation for the neutron heating by thermal excitations in solids.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2017
L. J. Broussard; B. A. Zeck; E. R. Adamek; S. Baeßler; N. Birge; M. Blatnik; J. D. Bowman; Aaron Brandt; M. A. P. Brown; J. Burkhart; Nathan Callahan; Steven Clayton; C. Crawford; C. Cude-Woods; S. Currie; E. B. Dees; X. Ding; N. Fomin; E. Frlez; J. Fry; F. Gray; S. Hasan; K. P. Hickerson; J. Hoagland; A. T. Holley; Takeyasu M. Ito; Andreas Klein; Hengne Li; Ching Liu; M. Makela
We describe a detection system designed for precise measurements of angular correlations in neutron β decay. The system is based on thick, large area, highly segmented silicon detectors developed in collaboration with Micron Semiconductor, Ltd. The prototype system meets specifications for β electron detection with energy thresholds below 10 keV, energy resolution of ∼3 keV FWHM, and rise time of ∼50 ns with 19 of the 127 detector pixels instrumented. Using ultracold neutrons at the Los Alamos Neutron Science Center, we have demonstrated the coincident detection of β particles and recoil protons from neutron β decay. The fully instrumented detection system will be implemented in the UCNB and Nab experiments to determine the neutron β decay parameters B, a, and b.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2017
Robert Pattie; E. R. Adamek; Thomas Brenner; Aaron Brandt; L. J. Broussard; Nathan Callahan; Steven Clayton; C. Cude-Woods; S. Currie; P. Geltenbort; Takeyasu M. Ito; Thorsten Lauer; Chen-Yu Liu; Jaroslaw Majewski; M. Makela; Yasohira Masuda; C. L. Morris; J. C. Ramsey; Daniel Salvat; A. Saunders; Juri Schroffenegger; Zhaowen Tang; W. Wei; Zhehui Wang; Erik B. Watkins; A. R. Young; B. A. Zeck
Abstract We report on the evaluation of commercial electroless nickel phosphorus (NiP) coatings for ultracold neutron (UCN) transport and storage. The material potential of 50 μ m thick NiP coatings on stainless steel and aluminum substrates was measured to be V F = 213 ( 5 . 2 ) neV using the time-of-flight spectrometer ASTERIX at the Lujan Center. The loss per bounce probability was measured in pinhole bottling experiments carried out at ultracold neutron sources at Los Alamos Neutron Science Center and the Institut Laue-Langevin. For these tests a new guide coupling design was used to minimize gaps between the guide sections. The observed UCN loss in the bottle was interpreted in terms of an energy independent effective loss per bounce, which is the appropriate model when gaps in the system and upscattering are the dominate loss mechanisms, yielding a loss per bounce of 1 . 3 ( 1 ) × 1 0 − 4 . We also present a detailed discussion of the pinhole bottling methodology and an energy dependent analysis of the experimental results.
Physical Review C | 2013
E. I. Sharapov; C. L. Morris; M. Makela; A. Saunders; E. R. Adamek; L. J. Broussard; C. Cude-Woods; Deion E Fellers; P. Geltenbort; M. Hartl; Syed Hasan; K. P. Hickerson; Gary E. Hogan; A. T. Holley; C. M. Lavelle; Chen-Yu Liu; M. P. Mendenhall; J. Ortiz; Robert Pattie; D. G. Phillips; J. C. Ramsey; Daniel Salvat; S. J. Seestrom; E. Shaw; Sky Sjue; W. E. Sondheim; B. VornDick; Zhehui Wang; T. L. Womack; A. R. Young
It is generally accepted that the main cause of ultracold neutron (UCN) losses in storage traps is upscattering to the thermal energy range by hydrogen adsorbed on the surface of the trap walls. However, the data on which this conclusion is based are poor and contradictory. Here we report a measurement, performed at the Los Alamos National Laboratory UCN source, of the average energy of the flux of upscattered neutrons after the interaction of UCN with hydrogen bound in the semicrystalline polymer PMP (trade name TPX), [C_6H_(12)]_n. Our analysis, performed with the mcnp code which applies the neutron-scattering law to UCN upscattered by bound hydrogen in semicrystalline polyethylene, [C_2H_4]_n, leads us to a flux average energy value of 26±3 meV, in contradiction to previously reported experimental values of 10 to 13 meV and in agreement with the theoretical models of neutron heating implemented in MCNP.
arXiv: Nuclear Experiment | 2018
X. Sun; E. R. Adamek; B. Allgeier; M. Blatnik; T. J. Bowles; L. J. Broussard; M. A. P. Brown; R. Carr; Steven Clayton; C. Cude-Woods; S. Currie; E. B. Dees; X. Ding; B. W. Filippone; A. García; P. Geltenbort; S. Hasan; K. P. Hickerson; J. Hoagland; R. Hong; G. E. Hogan; A. T. Holley; Takeyasu M. Ito; A. Knecht; Ching Liu; J. Liu; M. Makela; R. Mammei; J. W. Martin; D. Melconian
It has been proposed recently that a previously unobserved neutron decay branch to a dark matter particle (χ) could account for the discrepancy in the neutron lifetime observed in experiments that use two different measurement techniques. One of the possible final states discussed includes a single χ along with an e^+e^− pair. We use data from the UCNA (Ultracold Neutron Asymmetry) experiment to set limits on this decay channel. Coincident electron-like events are detected with ∼4π acceptance using a pair of detectors that observe a volume of stored Ultracold Neutrons (UCNs). The summed kinetic energy (E_(e^+e^−)) from such events is used to set limits, as a function of the χ mass, on the branching fraction for this decay channel. For χ masses consistent with resolving the neutron lifetime discrepancy, we exclude this as the dominant dark matter decay channel at ≫ 5σlevel for 100 keV 90% confidence level.
Next Generation Experiments to Measure the Neutron Lifetime | 2014
Alexander Saunders; Daniel Salvat; E. R. Adamek; David Bowman; Steven Clayton; C. Cude; W. Fox; Gary E. Hogan; K. P. Hickerson; A. T. Holley; Ching Liu; M. Makela; G. Manus; C. L. Morris; S. Penttila; J. C. Ramsey; S. Sawtelle; K. Solberg; John Vanderwerp; B. VornDick; Peter Walstrom; Zhehui Wang; A. R. Young
The UCNtau project is intended to develop a new measurement of the neutron lifetime using ultra-cold neutrons (UCNs) stored in a magneto-gravitational trap. In this article, we will describe the development of the experiment so far, including the trap itself, the UCN transport and monitoring system, the neutron detection methods, and the Monte Carlo simulations that have been used to model these elements. Finally, we will describe the first systematic effects that we plan to study using this apparatus.
Physical Review C | 2018
Takeyasu M. Ito; E. R. Adamek; Nathan Callahan; J. H. Choi; Steven Clayton; C. Cude-Woods; S. Currie; X. Ding; D. E. Fellers; P. Geltenbort; S. K. Lamoreaux; Ching Liu; S. MacDonald; M. Makela; C. L. Morris; Robert Pattie; J. C. Ramsey; Daniel Salvat; A. Saunders; E. I. Sharapov; Sky Sjue; A. P. Sprow; Z. Tang; H. L. Weaver; W. Wei; A. R. Young
Physical Review C | 2017
S. J. Seestrom; E. R. Adamek; Dave Barlow; Marie Blatnik; L. J. Broussard; Nathan Callahan; Steven Clayton; C. Cude-Woods; S. Currie; Eric B. Dees; Walt Fox; Mark A. Hoffbauer; K. P. Hickerson; Adam Holley; Chen-Yu Liu; M. Makela; Jason Medina; Deborah Jean Morley; C. L. Morris; Robert Pattie; J. C. Ramsey; A. Roberts; Daniel Salvat; A. Saunders; Eduard I. Sharapov; Sky Sjue; Brad A. Slaughter; Peter Walstrom; Zhehui Wang; Jonathon Wexler