A knock-on deuteron imager for measurements of fuel and hotspot asymmetry in direct-drive inertial confinement fusion implosions (invited).

A knock-on deuteron imager (KoDI) has been implemented to measure the fuel and hotspot asymmetry of cryogenic inertial confinement fusion implosions on OMEGA. Energetic neutrons produced by D-T fusion elastically scatter ("knock on") deuterons from the fuel layer with a probability that depends on ρR. Deuterons above 10 MeV are produced by near-forward scattering, and imaging them is equivalent to time-integrated neutron imaging of the hotspot. Deuterons below 6 MeV are produced by a combination of side scattering and ranging in the fuel, and encode information about the spatial distribution of the dense fuel. The KoDI instrument consists of a multi-penumbral aperture positioned 10-20 cm from the implosion using a ten-inch manipulator and a detector pack at 350 cm from the implosion to record penumbral images with magnification of up to 35×. Range filters and the intrinsic properties of CR-39 are used to distinguish different charged-particle images by energy along the same line of sight. Image plates fielded behind the CR-39 record a 10 keV x-ray image using the same aperture. A maximum-likelihood reconstruction algorithm has been implemented to infer the source from the projected penumbral images. The effects of scattering and aperture charging on the instrument point-spread function are assessed. Synthetic data are used to validate the reconstruction algorithm and assess an appropriate termination criterion. Significant aperture charging has been observed in the initial experimental dataset, and increases with aperture distance from the implosion, consistent with a simple model of charging by laser-driven EMP.

[1]  J. Knauer,et al.  Knock-on deuteron imaging for diagnosing the morphology of an ICF implosion at OMEGA , 2022, Physics of Plasmas.

[2]  O. Landen,et al.  Extensions of a classical mechanics “piston-model” for understanding the impact of asymmetry on ICF implosions: The cases of mode 2, mode 2/1 coupling, time-dependent asymmetry, and the relationship to coast-time , 2022, Physics of Plasmas.

[3]  J. Frenje,et al.  An x-ray penumbral imager for measurements of electron-temperature profiles in inertial confinement fusion implosions at OMEGA. , 2021, The Review of scientific instruments.

[4]  J. Kwiatkowski,et al.  Mitigation of mode-one asymmetry in laser-direct-drive inertial confinement fusion implosions , 2021, Physics of Plasmas.

[5]  J. Frenje,et al.  CR-39 nuclear track detector response to inertial confinement fusion relevant ions. , 2020, The Review of scientific instruments.

[6]  N. Woolsey,et al.  EMP control and characterization on high-power laser systems , 2018, High Power Laser Science and Engineering.

[7]  O. Landen,et al.  Fluence-compensated down-scattered neutron imaging using the neutron imaging system at the National Ignition Facility. , 2016, The Review of scientific instruments.

[8]  O. Landen,et al.  Spatial resolution measurements of the advanced radiographic capability x-ray imaging system at energies relevant to Compton radiography. , 2016, The Review of scientific instruments.

[9]  T. C. Sangster,et al.  Effects of fuel-capsule shimming and drive asymmetry on inertial-confinement-fusion symmetry and yield , 2016 .

[10]  J. Frenje,et al.  A new model to account for track overlap in CR-39 data , 2012 .

[11]  N. M. Larson,et al.  ENDF/B-VII.1 Nuclear Data for Science and Technology: Cross Sections, Covariances, Fission Product Yields and Decay Data , 2011 .

[12]  J. Frenje,et al.  The response of CR-39 nuclear track detector to 1-9 MeV protons. , 2011, The Review of scientific instruments.

[13]  J. Ziegler,et al.  SRIM – The stopping and range of ions in matter (2010) , 2010 .

[14]  Barry E. Schwartz,et al.  Proton core imaging of the nuclear burn in inertial confinement fusion implosions , 2006 .

[15]  C. Deutsch,et al.  Hierarchy of beam plasma instabilities up to high beam densities for fast ignition scenario , 2005 .

[16]  P. W. McKenty,et al.  D3He-proton emission imaging for inertial-confinement-fusion experiments (invited) , 2004 .

[17]  Barry E. Schwartz,et al.  Spectrometry of charged particles from inertial-confinement-fusion plasmas , 2003 .

[18]  E. R. Podolyak,et al.  Programs for signal recovery from noisy data using the maximum likelihood principle I. General description , 1993 .

[19]  S. S. Wilks The Large-Sample Distribution of the Likelihood Ratio for Testing Composite Hypotheses , 1938 .