Abstract

Neutron bang times ${t}_{\text{bang}}$ and mean neutron speeds $\overline{u}$ have been measured at the $Z$ facility for a series of ${D}_{2}$-filled targets, in magnetized liner inertial fusion experiments. Measurements were made by a novel neutron time-of-flight (nTOF) diagnostic, adapted for use at this facility, and consisted of detecting the neutron times in flight at seven independent scintillator--photomultiplier tube detectors (channels), located on three noncoplanar lines of sight, with distances to the neutron source varying between 690 and 2510 cm. The nTOF signals were analyzed by identifying fiducials on the detector traces to quantify the time in flight to each distance, using a nonrelativistic model for a uniformly thermalized, Maxwellian plasma distribution. The measured neutron arrival times were then linearly regressed on distance with the bang time and mean speed estimated from the fit parameters. A particular shot, 2584, is analyzed here to illustrate the method and the issues encountered in these measurements. On this particular shot, six usable channel traces were obtained. The standard errors of the parameter fits were as follows: ${t}_{\text{bang}}=3102.95\ifmmode\pm\else\textpm\fi{}0.97\text{ }\text{ }\mathrm{ns}$ (standard error) with six nTOF traces on the system clock and $\overline{u}=2.1524\ifmmode\pm\else\textpm\fi{}0.0032\text{ }\text{ }\mathrm{cm}/\mathrm{ns}$ (standard error), from which the mean, nonrelativistic, kinetic energy $\overline{E}$ of the neutrons was $2.4216\ifmmode\pm\else\textpm\fi{}0.0144\text{ }\text{ }\mathrm{MeV}$ (standard error). The estimates of $\overline{u}$ and $\overline{E}$ here agree within 1% of the published values for the $D{(d,n)}^{3}\mathrm{He}$ reaction. Hence, these measurements are consistent with the production of a thermalized, Maxwellian D-D fusion plasma in this experiment. The source duration was estimated to be $3.25\ifmmode\pm\else\textpm\fi{}0.84\text{ }\text{ }\mathrm{ns}$ (standard error) from six pulse-width measurements.

Highlights

  • Inertial confinement fusion (ICF) experiments on various fusion targets have been conducted at the Z accelerator (Z) [1,2] (Sandia National Laboratories, New Mexico) for over 20 years

  • The purpose of this article is to evaluate a novel neutron time-of-flight technique at Z for measuring (a) the bang time tbang of neutron emission on a system clock and (b) the mean speed uof the emergent neutrons, which can be compared to the published value for a thermalized

  • Plasma driven by the Dðd; nÞ3He reaction

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Summary

Introduction

Inertial confinement fusion (ICF) experiments on various fusion targets have been conducted at the Z accelerator (Z) [1,2] (Sandia National Laboratories, New Mexico) for over 20 years. Of particular recent interest has been the magnetic liner inertial fusion (MagLIF) approach [3]. The attainment of a pulsed plasma source of thermonuclear DD neutrons (with a mean neutron energy of 2.45 MeV, ion temperature of 2–3 keV, duration of ∼2 ns, and yield into 4π sr of ∼1012 neutrons) has been reported for D2-filled targets [4,5,6,7]. The purpose of this article is to evaluate a novel neutron time-of-flight (nTOF) technique at Z for measuring (a) the bang time tbang of neutron emission on a system clock and (b) the mean speed uof the emergent neutrons, which can be compared to the published value for a thermalized. This article focuses more on the nTOF technique—as modified for use at the Z accelerator—than on interpreting the internal plasma dynamics of a given MagLIF target

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