Abstract

The aim of this research is to produce double differential thick target yields, angular distributions and integrated yields for the inclusive production of neutrons, protons, deuterons, tritons, 3 He, and 4 He from intermediate heavy-ion interactions on thick targets of aluminium, polyethylene and other targets of interest to the radiation shielding program as specified by the National Aeronautics and Space Administration (NASA). In tandem with the experimental research, transport model calculations of these thick target yields were also performed. The first such experimental run was conducted in May 2015, with the expectation of improved experimental results at a following March 2016 run at the NASA Space Radiation Laboratory (NSRL) on the campus of Brookhaven National Laboratory (BNL). The May 2015 commissioning run served to test the electronics of the experimental setup, as well as the various detectors and other equipment under the conditions in which the following measurements will be run. The series of future accelerator-based experiments will rely on the inclusion of two separate upstream and downstream targets. Analysis of the data from both sets of detectors – liquid scintillator and sodium iodide – using both pulse height and time-of-flight methods will allow NASA to perform uncertainty quantification and sensitivity analysis on their transport codes and future shielding studies.

Highlights

  • Depending on the experimental setup, different particles could be identified at the various detectors

  • Additional plots from the proton runs will be presented to show the angular dependence on the data

  • A series of thick-target experiments has been designed to aid National Aeronautics and Space Administration (NASA) interests in deep-space manned missions by providing experimental data to assist with improving the transport models via uncertainty quantification

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Summary

Introduction

For the heavier ions (Z > 8) and heavy ion fragments (2 < Z < 8), there are reasonable levels of agreement on dose contributions. As such, this experiment is designed to study the Z = 1 & 2 particles - their production, their various energy- and spatial-based fluxes, and their dose contributions inside the target area

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