Time-of-flight vs time-of-arrival in neutron spectroscopic measurements for high energy density plasmas

Author:

Grim G. P.1ORCID,Mitrani J. M.1ORCID,Chandler G. A.2ORCID,Hahn K. D.1ORCID,Jones M. C.2ORCID,Mannion O. M.2ORCID

Affiliation:

1. Lawrence Livermore National Laboratory 1 , 7000 East Rd., Livermore, California 94551, USA

2. Sandia National Laboratories 2 , 1515 Eubank SE, Albuquerque, New Mexico 87185, USA

Abstract

The neutron time-of-flight (nToF) diagnostic technique has a lengthy history in Inertial Confinement Fusion (ICF) and High Energy Density (HED) Science experiments. Its initial utility resulted from the simple relationship between the full width half maximum of the fusion peak signal in a distant detector and the burn averaged conditions of an ideal plasma producing the flux [Lehner and Pohl, Z. Phys. 207, 83–104 (1967)]. More recent precision measurements [Gatu-Johnson et al., Phys. Rev. E 94(8), 021202 (2016)] and theoretical studies [Munro, Nucl. Fusion 56, 035001 (2016)] have shown the spectrum to be more subtle and complicated, driving the desire for an absolute calibration of the spectrum to disambiguate plasma dynamics from the conditions producing thermonuclear reactions. In experiments where the neutron production history is not well measured, but the neutron signal is preceded by a concomitant flux of photons, the spectrum can be in situ calibrated using a set of collinear detectors to obtain a true “time-of-flight” measurement. This article presents the motivation and overview of this technique along with estimates of the experimental precision needed to make useful measurements in existing and future nToF systems such as the pulsed power Z-machine located in Albuquerque, NM, at Sandia National Laboratories.

Funder

Lawrence Livermore National Laboratory

Sandia National Laboratories

Publisher

AIP Publishing

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