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Going Nuclear: Notes from the officially unofficial book tour
I work in the analytical labs at one of Europe’s oldest and largest nuclear sites: Sellafield, in northwestern England. I spend my days at the fume hood front, pipette in one hand and radiation probe in the other (and dosimeter pinned to my chest, of course). Outside the lab, I have a second job: I moonlight as a writer and public speaker. My new popular science book—Going Nuclear: How the Atom Will Save the World—came out last summer, and it feels like my life has been running at full power ever since.
Farzad Rahnema, Dingkang Zhang
Nuclear Science and Engineering | Volume 200 | Number 4 | April 2026 | Pages 865-876
Research Article | doi.org/10.1080/00295639.2025.2460389
Articles are hosted by Taylor and Francis Online.
In this paper, a new high-order stochastic perturbation method is developed to update the COMET surface-to-surface and fission response functions due to any change in arbitrary magnitude in the density of materials or isotopic atom densities. The method is developed by deriving the relation between the weights of a particle making multiple collisions in the perturbed and unperturbed systems and tallying the Chebyshev expansion moments of the response functions. As a result, the response functions can be updated on the fly during COMET core calculations to account for any arbitrary change in the material density or isotopic atom density. The method is benchmarked in a full-length Advanced High-Temperature Reactor (AHTR) single-assembly problem.
A comparison between the COMET solution using the perturbation method and that using the response function library generated directly by Monte Carlo reveals excellent agreement between the two COMET solutions (i.e. the corresponding eigenvalues and fission density distributions). The difference in the eigenvalues is 2 pcm, which is less than one standard deviation (1 of the stochastic uncertainty in the COMET calculations (7 pcm), and the average relative difference in the stripewise fission densities is 0.12%, which is less than 3 . The perturbation method eliminates the need for precomputing the perturbed responses for the perturbed COMET calculation. This is a savings of the library precomputation time by a factor of 3.66.