Reuse & Permissions

It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4.0 International license. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author(s) and the published article's title, journal citation, and DOI are maintained. Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures.

Export citation

Export citation

Choose format for download:

Download Citation
  • Editors' Suggestion
  • Letter
  • Open Access

N-dimensional maximum-entropy tomography via particle sampling

Austin Hoover*

  • *Contact author: hooveram@ornl.gov

Phys. Rev. Accel. Beams 28, L084601 – Published 7 August, 2025

DOI: https://doi.org/10.1103/zl2h-3v32

Abstract

We propose a modified maximum-entropy (MENT) algorithm for six-dimensional phase space tomography. The algorithm uses particle sampling and low-dimensional density estimation to approximate large sets of high-dimensional integrals in the original MENT formulation. We implement this approach using Markov Chain Monte Carlo (MCMC) sampling techniques and demonstrate convergence of six-dimensional MENT on both synthetic and measured data.

View figure in article

Physics Subject Headings (PhySH)

Article Text

Supplemental Material

References (28)

  1. C. McKee, P. O’Shea, and J. Madey, Phase space tomography of relativistic electron beams, Nucl. Instrum. Methods Phys. Res., Sect. A 358, 264 (1995).
  2. A. Wolski, D. C. Christie, B. L. Militsyn, D. J. Scott, and H. Kockelbergh, Transverse phase space characterization in an accelerator test facility, Phys. Rev. Accel. Beams 23, 032804 (2020).
  3. A. Wolski, M. A. Johnson, M. King, B. L. Militsyn, and P. H. Williams, Transverse phase space tomography in an accelerator test facility using image compression and machine learning, Phys. Rev. Accel. Beams 25, 122803 (2022).
  4. R. Roussel, J. P. Gonzalez-Aguilera, A. Edelen, E. Wisniewski, A. Ody, W. Liu, Y.-K. Kim, and J. Power, Efficient six-dimensional phase space reconstructions from experimental measurements using generative machine learning, Phys. Rev. Accel. Beams 27, 094601 (2024).
  5. A. Hoover and J. C. Wong, High-dimensional maximum-entropy phase space tomography using normalizing flows, Phys. Rev. Res. 6, 033163 (2024).
  6. A. Caticha and R. Preuss, Maximum entropy and Bayesian data analysis: Entropic prior distributions, Phys. Rev. E 70, 046127 (2004).
  7. S. Pressé, K. Ghosh, J. Lee, and K. A. Dill, Principles of maximum entropy and maximum caliber in statistical physics, Rev. Mod. Phys. 85, 1115 (2013).
  8. G. Minerbo, MENT: A maximum entropy algorithm for reconstructing a source from projection data, Comput. Graphics Image Process. 10, 48 (1979).
  9. N. J. Dusaussoy and I. E. Abdou, The extended MENT algorithm: A maximum entropy type algorithm using prior knowledge for computerized tomography, IEEE Trans. Signal Process. 39, 1164 (1991).
  10. C. T. Mottershead, Maximum entropy tomography, in Maximum Entropy and Bayesian Methods, edited by K. M. Hanson and R. N. Silver, Fundamental Theories of Physics Vol. 79 (Springer, Dordrecht, 1996), pp. 425–430, 10.1007/978-94-011-5430-7_54.
  11. G. N. Minerbo, O. R. Sander, and R. A. Jameson, Four-dimensional beam tomography, IEEE Trans. Nucl. Sci. 28, 2231 (1981).
  12. J. C. Wong, A. Shishlo, A. Aleksandrov, Y. Liu, and C. Long, 4D transverse phase space tomography of an operational hydrogen ion beam via noninvasive 2D measurements using laser wires, Phys. Rev. Accel. Beams 25, 042801 (2022).
  13. A. Hoover, Four-dimensional phase space tomography from one-dimensional measurements of a hadron beam, Phys. Rev. Accel. Beams 27, 122802 (2024).
  14. This principle of minimal updating is enforced via two axioms, which we paraphrase from [15]: (i) Subset independence: Probabilities conditioned on one domain should not be affected by information about a different, nonoverlapping domain. Consequently, nonoverlapping domains contribute additively to the entropy. (ii) Subsystem independence: If we assume two variables are unrelated, and if we receive information about each variable separately, then we should not infer any relationship between the variables on the basis of this information. In other words, if we measure the marginal distributions {ρ(v),ρ(w)}, and if the prior does not encode any relationship between v and w, then the posterior should be the product of the marginals: ρ(v,w)=ρ(v)ρ(w).

  15. A. Caticha, Entropy, information, and the updating of probabilities, Entropy 23, 895 (2021).
  16. A. Gelman, J. B. Carlin, H. S. Stern, and D. B. Rubin, Bayesian Data Analysis (Chapman and Hall/CRC, 1995).
  17. N. Metropolis, A. W. Rosenbluth, M. N. Rosenbluth, A. H. Teller, and E. Teller, Equation of state calculations by fast computing machines, J.Chem. Phys. 21, 1087 (1953).
  18. One way to fit the 4D or 6D covariance matrix to all measured projections is to leverage the Cholesky decomposition Σ=LLT, where L is a lower-diagonal matrix with positive diagonal elements, which ensures the covariance matrix is positive semidefinite. Alternatively, the diagonal or block-diagonal elements of the covariance matrix are typically available from faster measurements of the 2D phase space distributions {ρ(x,x′),ρ(y,y′),ρ(z,z′)}. Cross-plane correlations ignored in this scenario are typically much weaker than within-plane correlations, such as quadrupole focusing. If 2D measurements are unavailable, one may estimate the beam size by sampling from a uniform MENT prior and refining until the beam size can be estimated. (The prior is nonzero only in the regions allowed by the measurements).

  19. For a fixed number of measurements K=N(N−1)/2 of a distribution without linear correlations between planes, we hypothesize that the ideal set of measurements is the set of K two-dimensional marginals.

  20. In this case, we extracted the covariance matrix elements from the previous GPSR fit.

  21. See Supplemental Material at http://link.aps.org/supplemental/10.1103/zl2h-3v32 for 1D and 2D projections of the reconstructed 6D phase space distribution.
  22. C. Durkan, A. Bekasov, I. Murray, and G. Papamakarios, Neural spline flows, in Advances in Neural Information Processing Systems (Curran Associates, Inc., 2019), Vol. 32, https://proceedings.neurips.cc/paper_files/paper/2019/file/7ac71d433f282034e088473244df8c02-Paper.pdf.
  23. A. Hoover, K. Ruisard, A. Aleksandrov, A. Zhukov, and S. Cousineau, Analysis of a hadron beam in five-dimensional phase space, Phys. Rev. Accel. Beams 26, 064202 (2023).
  24. The distribution exhibits some fluctuations during training, which may indicate that the sampling chains have not fully converged to the target distribution. However, the final distribution seems fairly stable with respect to random number generator seed. Additional convergence diagnostics (beyond visual checks) should be used in future studies to resolve this issue.

  25. E. Higson, W. Handley, M. Hobson, and A. Lasenby, Dynamic nested sampling: An improved algorithm for parameter estimation and evidence calculation, Stat. Comput. 29, 891 (2019).
  26. L. I. Midgley, V. Stimper, G. N. C. Simm, B. Schölkopf, and J. M. Hernández-Lobato, Flow annealed importance sampling bootstrap, in Proceedings of the 11th International Conference on Learning Representations (2023), https://openreview.net/forum?id=XCTVFJwS9LJ.
  27. http://energy.gov/downloads/doe-public-access-plan
  28. A. Hoover, N-dimensional maximum-entropy tomography via particle sampling, Zenodo (v0.1) (2025), 10.5281/zenodo.15412851

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation