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Criteria for projected discovery and exclusion sensitivities of counting experiments
Abstract The projected discovery and exclusion capabilities of particle physics and astrophysics/cosmology experiments are often quantified using the median expected p-value or its corresponding significance. We argue that this criterion leads to flawed results, which for example can counterintuitively project lessened sensitivities if the experiment takes more data or reduces its background. We discuss the merits of several alternatives to the median expected significance, both when the background is known and when it is subject to some uncertainty. We advocate for standard use of the “exact Asimov significance” $$Z^\mathrm{A}$$ Z A detailed in this paper.
Enhancing Adaptive Physics Refinement Simulations Through the Addition of Realistic Red Blood Cell Counts
Simulations of cancer cell transport require accurately modeling mm-scale and longer trajectories through a circulatory system containing trillions of deformable red blood cells, whose intercellular interactions require submicron fidelity. Using a hybrid CPU-GPU approach, we extend the advanced physics refinement (APR) method to couple a finely-resolved region of explicitly-modeled red blood cells to a coarsely-resolved bulk fluid domain. We further develop algorithms that: capture the dynamics at the interface of differing viscosities, maintain hematocrit within the cell-filled volume, and move the finely-resolved region and encapsulated cells while tracking an individual cancer cell. Comparison to a fully-resolved fluid-structure interaction model is presented for verification. Finally, we use the advanced APR method to simulate cancer cell transport over a mm-scale distance while maintaining a local region of RBCs, using a fraction of the computational power required to run a fully-resolved model.
Quantum-enhanced phase imaging without coincidence counting
Quantitative phase imaging provides a way to image transparent objects, such as biological cells, and measure their thickness. We report on a phase-imaging method that achieves twice the phase shift and approximately 1.7 times the spatial resolution of an equivalent spatially and temporally coherent classical quantitative phase-imaging system by using quantum interference between successive spontaneous parametric downconversion events in a nonlinear crystal. Furthermore, our method is approximately 1000 times faster than imaging the parametric downconversion photons in coincidence, which requires measurement times on the order of tens of hours. Our method may be useful for imaging sensitive transparent objects that require low illumination intensities at near-infrared and longer illumination wavelengths, such as photosensitive biological samples.
Fast-neutron multiplicity counting for nuclear safeguards and nonproliferation applications [Slides]
Abstract not provided.
NEGATIVE MUON COUNT FOR THE MUON g-2 EXPERIMENT
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Negative Muon Count for the FNAL Muon g-2 Experiment
The primary goal of the FNAL Muon g-2 Experiment, located in Batavia, IL, USA, is to measure the anomalous magnetic dipole moment, a μ = (g-2)/2, of a muon to a precision of 0.14 ppm. Initial results from the experiment confirm a discrepancy between the experimental value of the muon anomaly compared with the theoretical value first discovered by the Brookhaven Muon g-2 Experiment in 2001. This discrepancy hints at new physics. However, running the experiment with negative muons is essential in order to verify the experimental value of the muon anomaly. As neither experiments nor simulation studies pertaining to the muon anomaly have been performed with negative muons, the goal of this work is to estimate the rates of negative muons arriving at the FNAL Muon g-2 experiment so that scientists can estimate the time required to run the experiment with negative muons. In order to do this, we performed several simulations of the Muon Campus, which delivers muons to the FNAL Muon g-2 Experiment, using the G4Beamline v. 3.06 at the National Energy Research Computing Center. We performed separate simulations for different sections of the muon campus, and simulations were repeated twice, once for negative muons and once for positive muons. An initial 10 9 protons were shot on target for both the negative and positive muon simulations. We found that the rate of negative muons arriving at the experiment was 0.549 times the rate of positive muons arriving at the experiment.
Low-level beta counting: technical foundation and blind validation experiments [Slides]
Abstract not provided.
Counting Abelian Squares More Efficiently
I present a recursive formula for calculating the number of abelian squares of length n+n over an alphabet of size d. The presented formula is similar to a previously known formula but has substantially lower complexity when d >> n.
Single Photon Counting Scintillation Detectors with Analog Silicon Photomultipliers.
Abstract not provided.
In-Situ Ion Counting for Deterministic Placement of Single Photon Emitters.
Abstract not provided.
Overview of MUSiC and Neutron Multiplicity Counting Analysis with the NoMAD Detector [Slides]
Rocky Flats are hemisphere shells of bare HEU. Planet is a vertical lift assembly at the DAF. MUSiC is a set of experiments using the Rocky Flats hemisphere shells and the Planet lift assembly.
From count rates to quantifying isotopic activities: Field analysis of radiation monitoring data
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Focused Ion Beam Implantation for the Fabrication of Single Defect Centers in Wide Bandgap Substrates using in-situ Counting and Photoluminescence .
Abstract not provided.
Implementing auto-loading germanium counting systems for neutron activation measurements at Sandia?s Z-Facility.
Abstract not provided.