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A Robust Star Removal Algorithm for the Neutron Imaging System Diagnostic University of California, Santa Cruz 1 ; NIF, Lawrence Livermore National Laboratory 2 ; Los Alamos National Laboratory 3 The Neutron Imaging System (NIS) diagnostic is an important tool for measuring the size and shape of the burning deuterium-tritium plasma during the ignition stage of inertial confinement fusion implosions. The NIS uses a pinhole neutron aperture array with penumbral apertures which is placed between the neutron source and a neutron detector. An iterative maximum likelihood algorithm reconstructs the neutron source from the observed image. However, during image collection, some neutrons scatter from the flight path and interact directly with the CCD elements, producing bright pixels called “stars,” which could negatively impact the reconstruction. An automated algorithm has been developed to remove these stars and is in the process of being integrated in the NIF automated analysis framework. Introduction Star Removal Algorithm George Labaria 1,2 , Abbie Warrick 2 , David Fittinghoff 2 , and Petr Volegov 3 The National Ignition Facility (NIF) utilizes the Neutron Imaging System diagnostic to provide data on the size and shape of the fusion hotspot and surrounding cold fuel during the ignition stage of the inertial confinement fusion implosions. LLNL-POST-735383 National Ignition Facility Lawrence Livermore National Laboratory Operated by the US Department of Energy This work performed under the auspices of the U.S. Department of Energy and an appointment to the Office of Science, Science Undergraduate Laboratory Internship (SULI) Program at the Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344. Some neutrons scatter from the flight path and interact directly with the CCD, producing bright pixels called “stars” (figure 3). These stars negatively impact noise modeling and pinhole extraction algorithms. The star removal algorithm is a small but critical component in the NIS image pre- processing. The previous version of the star removal algorithm lacked the ability to correct stars that were greater than a pixel in size. Examination of the data suggests that stars greater than a pixel do exist. Figure 4. Active and star region pixels. Figure 5. Active region pixel intensity profile. Let 77 () be the 7x7 set of pixels centered around (figure 6). Let = 77 77 Pixel is flagged as a star if ≥6. If pixel is a star, then the eight adjacent pixels are considered and flagged as part of the star if ≥ _ℎ where 33 ()\{}. The threshold _ℎ is typically set to 3 or 1.5, determined by the data in 77 . Flagged star pixels are replaced by the median 77 . 7x7 active region 3x3 star region star Figure 6. Schematic of 77 . Results and Concluding Remarks The star removal algorithm is a critical component to the image-preprocessing component for the NIS diagnostic. The algorithm provides a plausible replacement for the star pixels based on the surrounding data, which ultimately improves noise modeling and the centering of the pinhole extraction algorithm. star Figure 3. A typical example of a star in the pinhole region. Raw shot data Background correction Flat field correction Sat. pixel correction Warp correction MCP gain correction Pen. ID and Orient Image Rebin image Penumbral ID Long-range blur corr. Source recon. Raw pre-shot data Star removal
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A Robust Star Removal Algorithm for the Neutron Imaging ......A Robust Star Removal Algorithm for the Neutron Imaging System Diagnostic University of California, Santa Cruz 1 ; NIF,

Sep 13, 2020

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Page 1: A Robust Star Removal Algorithm for the Neutron Imaging ......A Robust Star Removal Algorithm for the Neutron Imaging System Diagnostic University of California, Santa Cruz 1 ; NIF,

A Robust Star Removal Algorithm for the Neutron Imaging System Diagnostic

University of California, Santa Cruz1; NIF, Lawrence Livermore National Laboratory2; Los Alamos National Laboratory3

The Neutron Imaging System (NIS) diagnostic is an important tool for measuring the size and shape of the burning deuterium-tritium plasma during the ignition stage of

inertial confinement fusion implosions. The NIS uses a pinhole neutron aperture array with penumbral apertures which is placed between the neutron source and a neutron

detector. An iterative maximum likelihood algorithm reconstructs the neutron source from the observed image. However, during image collection, some neutrons scatter

from the flight path and interact directly with the CCD elements, producing bright pixels called “stars,” which could negatively impact the reconstruction. An automated

algorithm has been developed to remove these stars and is in the process of being integrated in the NIF automated analysis framework.

Introduction Star Removal Algorithm

George Labaria1,2, Abbie Warrick2, David Fittinghoff2, and Petr Volegov3

The National Ignition Facility (NIF) utilizes the Neutron Imaging System diagnostic to

provide data on the size and shape of the fusion hotspot and surrounding cold fuel

during the ignition stage of the inertial confinement fusion implosions.

LLNL-POST-735383National Ignition Facility • Lawrence Livermore National Laboratory • Operated by the US Department of Energy

This work performed under the auspices of the U.S. Department of Energy and an appointment to the Office of Science, Science Undergraduate Laboratory Internship (SULI)

Program at the Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344.

• Some neutrons scatter from the flight path and interact directly with the CCD,

producing bright pixels called “stars” (figure 3).

• These stars negatively impact noise modeling and pinhole extraction algorithms.

• The star removal algorithm is a small but critical component in the NIS image pre-

processing.

• The previous version of the star removal algorithm lacked the ability to correct stars

that were greater than a pixel in size.

• Examination of the data suggests that stars greater than a pixel do exist.

Figure 4. Active and star region pixels. Figure 5. Active region pixel intensity profile.

• Let 𝑁7𝑥7(𝑖) be the 7x7 set of pixels centered around 𝑖 (figure 6).

• Let

𝑟𝑒𝑙𝑑𝑖𝑓𝑓 𝑖 =𝑖 − 𝑚𝑒𝑑 𝑁7𝑥7 𝑖

𝑠𝑡𝑑 𝑁7𝑥7 𝑖

• Pixel 𝑖 is flagged as a star if 𝑟𝑒𝑙𝑑𝑖𝑓𝑓 𝑖 ≥ 6.

• If pixel 𝑖 is a star, then the eight adjacent pixels are considered and

flagged as part of the star if 𝑟𝑒𝑙𝑑𝑖𝑓𝑓 𝑗 ≥ 𝑙𝑜𝑤_𝑡ℎ𝑟𝑒𝑠 where 𝑗 ∈𝑁3𝑥3(𝑖)\{𝑖}. The threshold 𝑙𝑜𝑤_𝑡ℎ𝑟𝑒𝑠 is typically set to 3 or 1.5,

determined by the data in 𝑁7𝑥7 𝑖 .

• Flagged star pixels 𝑖 are replaced by the median 𝑚𝑒𝑑 𝑁7𝑥7 𝑖 .

7x7 active region

3x3 star region

star

𝑖

Figure 6. Schematic of 𝑁7𝑥7 𝑖 .

Results and Concluding RemarksThe star removal algorithm is a critical

component to the image-preprocessing

component for the NIS diagnostic. The

algorithm provides a plausible replacement for

the star pixels based on the surrounding data,

which ultimately improves noise modeling and

the centering of the pinhole extraction

algorithm.

star

Figure 3. A typical example of a star in the pinhole region.

Raw shot data

Background correction

Flat field correction

Sat. pixel correction

Warp correction

MCP gain correction

Pen. ID and Orient Image

Rebin imagePenumbral

IDLong-range blur corr.

Source recon.

Raw pre-shot data

Star removal