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arxiv: 2602.21375 · v1 · submitted 2026-02-24 · ⚛️ physics.plasm-ph · physics.flu-dyn

Passive freeze-out of the Richtmyer-Meshkov instability

J. Strucka , D. M. Sterbentz , B. Lukic , K. Mughal , Y. Yao , K. Marrow , W. J. Schill , C. F. Jekel
show 11 more authors
D. A. White N. Asmedianov R. Grikshtas O. Belozerov S. Efimov J. Skidmore A. Rack Ya. E. Krasik J. L. Belof J. P. Chittenden S. N. Bland
This is my paper

Pith reviewed 2026-05-15 19:33 UTC · model grok-4.3

classification ⚛️ physics.plasm-ph physics.flu-dyn
keywords Richtmyer-Meshkov instabilitypassive freeze-outinertial confinement fusionsub-surface voidsshock shapinghydrodynamic instabilitieshigh energy density physicsadditive manufacturing
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The pith

Sub-surface voids in sinusoidal targets suppress Richtmyer-Meshkov instability growth by over 70 percent through passive shock sequencing.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

This paper demonstrates that embedding additively manufactured sub-surface voids in a sinusoidal interface can induce passive freeze-out of the Richtmyer-Meshkov instability. The voids convert a single incoming shock into a train of weaker successive shocks that stagnate instability growth upstream of the surface without any alteration to the driving pressure pulse or the target geometry itself. High-speed X-ray imaging in a low-pressure surrogate regime records suppression exceeding 70 percent, while hydrodynamic simulations identify temporal shock shaping as the main cause with smaller contributions from curvature and weakening. The result supplies a driver-independent route to controlling shock-driven mixing in inertial confinement fusion and other high-energy-density flows.

Core claim

The central discovery is the first experimental observation of passive freeze-out of the Richtmyer-Meshkov instability. Additively manufactured sub-surface voids placed beneath a sinusoidal interface reshape an incident single shock into a sequence of weaker shocks. This temporal sequencing produces stagnation of the instability amplitude, yielding more than 70 percent suppression as recorded by X-ray imaging. Simulations confirm that the dominant mechanism is the altered pressure history at the interface rather than geometric curvature or net shock weakening.

What carries the argument

Additively manufactured sub-surface voids that convert a single shock into a sequence of weaker successive shocks, thereby imposing temporal pressure shaping at the interface.

If this is right

  • Instability control is achieved without any modification to the external driver pulse or the perturbed surface geometry.
  • Reduced mixing and improved performance become possible in inertial confinement fusion targets through this passive internal modification.
  • The same void-based shock sequencing can be applied to other high-energy-density systems limited by Richtmyer-Meshkov or related instabilities.
  • Additive manufacturing provides a practical route to placing voids at chosen depths and spacings for tailored shock trains.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • This passive method could lessen the need for intricate active pulse shaping in future driver designs.
  • Void patterns might be tuned to suppress specific wavelengths or mode numbers that dominate in a given target.
  • The approach could transfer to laboratory astrophysics experiments that simulate supernova remnant shocks.
  • Combining internal voids with surface or drive modifications may produce hybrid stabilization strategies.

Load-bearing premise

The measured suppression arises primarily from the temporal sequencing of shocks created by the voids rather than from spatial curvature or overall shock weakening.

What would settle it

An experiment that fills the voids with solid material of identical density and measures instability growth returning to the level seen in the no-void control case while every other parameter remains fixed.

Figures

Figures reproduced from arXiv: 2602.21375 by A. Rack, B. Lukic, C. F. Jekel, D. A. White, D. M. Sterbentz, J. L. Belof, J. P. Chittenden, J. Skidmore, J. Strucka, K. Marrow, K. Mughal, N. Asmedianov, O. Belozerov, R. Grikshtas, S. Efimov, S. N. Bland, W. J. Schill, Ya. E. Krasik, Y. Yao.

Figure 1
Figure 1. Figure 1: FIG. 1. (a) Side-on and isometric view of the experimental setup showing the exploding copper foil, direction of the current [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. (a) X-ray radiographs of our baseline experiment [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. (a) Jet tip position (red) and mean interface position (blue) vs. time for the baseline geometry. (b) Same as (a), for [PITH_FULL_IMAGE:figures/full_fig_p004_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. Mass modulation [PITH_FULL_IMAGE:figures/full_fig_p005_5.png] view at source ↗
read the original abstract

The Richtmyer-Meshkov instability (RMI) poses a major challenge in inertial confinement fusion (ICF) due to its role in mixing and performance degradation. We report the first experimental observation of passive freeze-out of RMI in a low-pressure surrogate regime; an instability stagnation effect induced without modifying the driving pressure pulse or the target surface geometry. Using additively manufactured sub-surface voids in a sinusoidal target, we convert a single shock into a sequence of weaker shocks that suppress instability growth upstream of the surface by over 70%. High-speed X-ray imaging and hydrodynamic simulations suggest that this suppression arises primarily from temporal shaping, with lesser contributions from spatial curvature and shock weakening. Our results demonstrate a driver-independent pathway for controlling shock-driven hydrodynamic instabilities relevant to ICF and other high energy density systems.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 1 minor

Summary. The paper reports the first experimental observation of passive freeze-out of the Richtmyer-Meshkov instability (RMI) in a low-pressure surrogate regime. Using additively manufactured sub-surface voids in a sinusoidal target, a single shock is converted into a sequence of weaker shocks that suppress instability growth upstream of the surface by over 70%, without modifying the driving pressure pulse or target surface geometry. High-speed X-ray imaging and hydrodynamic simulations suggest the suppression arises primarily from temporal shock shaping, with lesser contributions from spatial curvature and shock weakening.

Significance. If the central observation holds, the work demonstrates a novel driver-independent pathway for controlling shock-driven hydrodynamic instabilities relevant to inertial confinement fusion (ICF) and high-energy-density systems. The passive approach via sub-surface voids could simplify target design by avoiding changes to the drive or surface geometry. The experimental demonstration in a surrogate regime is a useful proof-of-concept, though its broader impact would be strengthened by quantitative error analysis and extension to relevant ICF conditions.

major comments (2)
  1. [Abstract] Abstract: The claim of 'over 70%' suppression is presented without quantitative error bars, baseline controls, or details on the extraction method from X-ray imaging data. This figure is load-bearing for the central claim of significant passive freeze-out and requires explicit support in the results section.
  2. [Simulations] Hydrodynamic simulations discussion: The attribution that temporal shaping dominates over curvature and weakening is based on simulation outputs, but no explicit decomposition (e.g., controlled runs holding curvature fixed while varying shock timing) is described. This apportionment is load-bearing for the proposed mechanism and remains an unverified modeling result.
minor comments (1)
  1. [Abstract] The abstract would benefit from a brief statement of the surrogate regime pressure range and target parameters to provide immediate context for the low-pressure claim.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their constructive review and for highlighting areas where additional quantitative support would strengthen the central claims. We address each major comment below and have revised the manuscript accordingly to incorporate the requested details and analyses.

read point-by-point responses

  1. Referee: [Abstract] Abstract: The claim of 'over 70%' suppression is presented without quantitative error bars, baseline controls, or details on the extraction method from X-ray imaging data. This figure is load-bearing for the central claim of significant passive freeze-out and requires explicit support in the results section.

    Authors: We agree that the 'over 70%' suppression value requires explicit quantitative backing. In the revised manuscript we have expanded the results section with error bars derived from the standard deviation across repeated shots, direct comparison to baseline targets lacking sub-surface voids, and a detailed description of the amplitude extraction procedure from the high-speed X-ray radiographs. These additions are now cross-referenced in the abstract. revision: yes

  2. Referee: [Simulations] Hydrodynamic simulations discussion: The attribution that temporal shaping dominates over curvature and weakening is based on simulation outputs, but no explicit decomposition (e.g., controlled runs holding curvature fixed while varying shock timing) is described. This apportionment is load-bearing for the proposed mechanism and remains an unverified modeling result.

    Authors: The referee is correct that the original text did not present an explicit decomposition isolating each contribution. We have performed additional controlled hydrodynamic runs: one series holding shock timing fixed while varying interface curvature, and a second holding curvature fixed while varying the temporal shock profile. The new results, included as a supplementary figure and accompanying discussion, confirm that temporal shaping accounts for the majority of the observed suppression while curvature and weakening each contribute less than 20%. We have also added a brief statement on the modeling assumptions and limitations. revision: yes

Circularity Check

0 steps flagged

No significant circularity; experimental observation with standard simulation support

full rationale

The paper reports a direct experimental observation of >70% RMI suppression via X-ray imaging of additively manufactured targets with sub-surface voids. The central result is the measured stagnation effect itself, obtained without modifying the driving pulse or surface geometry. Hydrodynamic simulations are invoked only to apportion contributions from temporal shaping, curvature, and weakening, but no equations, fitted parameters, or derivations are shown that reduce the observed suppression to a quantity defined by the same data or by self-citation chains. No self-definitional steps, uniqueness theorems, or ansatzes imported from prior author work appear in the provided text. The finding is therefore self-contained as an empirical result interpreted with conventional hydrodynamics.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on standard hydrodynamic equations for shock propagation and interface evolution plus experimental measurement; no free parameters are introduced or fitted in the reported result, and no new physical entities are postulated.

axioms (1)
  • standard math Standard inviscid compressible hydrodynamic equations govern shock propagation and Richtmyer-Meshkov growth in the surrogate regime
    Invoked to interpret both the X-ray images and the supporting simulations

pith-pipeline@v0.9.0 · 5536 in / 1306 out tokens · 24786 ms · 2026-05-15T19:33:38.903051+00:00 · methodology

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Reference graph

Works this paper leans on

47 extracted references · 47 canonical work pages

  1. [1]

    The Lawrence Livermore National Laboratory journal number is LLNL-JRNL-2010870. 7 Appendix A: Dynamic compression experiment The dynamic compression experiment was performed at the European Synchrotron using the “Grengen” pulsed power generator charged to +45 kV [34]. In the experi- ment, the generator delivered a current pulse of∼110 kA in∼600 ns into a ...

    work page 2010

  2. [2]

    Zhou, Rayleigh–taylor and richtmyer–meshkov insta- bility induced flow, turbulence, and mixing

    Y. Zhou, Rayleigh–taylor and richtmyer–meshkov insta- bility induced flow, turbulence, and mixing. i, Physics Reports720–722, 1–136 (2017)

    work page 2017

  3. [3]

    Zhou, Rayleigh–taylor and richtmyer–meshkov insta- bility induced flow, turbulence, and mixing

    Y. Zhou, Rayleigh–taylor and richtmyer–meshkov insta- bility induced flow, turbulence, and mixing. ii, Physics Reports723–725, 1–160 (2017)

    work page 2017

  4. [4]

    A. B. Zylstra, O. A. Hurricane, D. A. Callahan, A. L. Kritcher, J. E. Ralph, H. F. Robey, J. S. Ross, C. V. Young, K. L. Baker, D. T. Casey, T. D¨ oppner, L. Di- vol, M. Hohenberger, S. Le Pape, A. Pak, P. K. Patel, R. Tommasini, S. J. Ali, P. A. Amendt, L. J. Atherton, B. Bachmann, D. Bailey, L. R. Benedetti, L. Berzak Hop- kins, R. Betti, S. D. Bhandark...

    work page 2022

  5. [5]

    B. D. Keenan, W. T. Taitano, A. N. Simakov, L. Chac´ on, and B. J. Albright, Shock-driven kinetic and diffusive mix in high-z pusher icf designs, Physics of Plasmas27, 10.1063/1.5140361 (2020)

    work page doi:10.1063/1.5140361 2020

  6. [6]

    D. S. Clark, A. Allen, S. H. Baxamusa, J. Biener, M. M. Biener, T. Braun, S. Davidovits, L. Divol, W. A. Farmer, T. Fehrenbach, C. Kong, M. Millot, J. Milovich, A. Nikroo, R. C. Nora, A. E. Pak, M. S. Rubery, M. Sta- dermann, P. Sterne, C. R. Weber, and C. Wild, Modeling ablator defects as a source of mix in high-performance im- plosions at the national i...

    work page doi:10.1063/5.0200730 2024

  7. [7]

    K. O. Mikaelian, Richtmyer-meshkov instabilities in stratified fluids, Phys. Rev. A31, 410 (1985)

    work page 1985

  8. [8]

    T. Sano, K. Ishigure, and F. Cobos-Campos, Suppres- sion of the richtmyer-meshkov instability due to a density transition layer at the interface, Physical Review E102, 10.1103/physreve.102.013203 (2020)

    work page doi:10.1103/physreve.102.013203 2020

  9. [9]

    Liang and X

    Y. Liang and X. Luo, Shock-induced dual-layer evolution, Journal of Fluid Mechanics929, 10.1017/jfm.2021.903 (2021)

    work page doi:10.1017/jfm.2021.903 2021

  10. [10]

    W. J. Schill, M. R. Armstrong, J. H. Nguyen, D. M. Sterbentz, D. A. White, L. X. Benedict, R. N. Rieben, A. Hoff, H. E. Lorenzana, J. L. Belof, B. M. La Lone, and M. D. Staska, Suppression of richtmyer-meshkov in- stability via special pairs of shocks and phase transitions, Phys. Rev. Lett.132, 024001 (2024)

    work page 2024

  11. [11]

    Samtaney, Suppression of the richtmyer–meshkov in- stability in the presence of a magnetic field, Physics of Fluids15, L53–L56 (2003)

    R. Samtaney, Suppression of the richtmyer–meshkov in- stability in the presence of a magnetic field, Physics of Fluids15, L53–L56 (2003)

    work page 2003

  12. [12]

    T. Sano, T. Inoue, and K. Nishihara, Critical magnetic field strength for suppression of the richtmyer-meshkov instability in plasmas, Physical Review Letters111, 10.1103/physrevlett.111.205001 (2013)

    work page doi:10.1103/physrevlett.111.205001 2013

  13. [13]

    C. M. Huntington, A. Shimony, M. Trantham, C. C. Kuranz, D. Shvarts, C. A. Di Stefano, F. W. Doss, R. P. Drake, K. A. Flippo, D. H. Kalantar, S. R. Klein, J. L. Kline, S. A. MacLaren, G. Malamud, A. R. Miles, S. T. Prisbrey, K. S. Raman, B. A. Remington, H. F. Robey, W. C. Wan, and H.-S. Park, Ablative sta- bilization of rayleigh-taylor instabilities resu...

    work page doi:10.1063/1.5022179 2018

  14. [14]

    S. W. Haan, J. D. Lindl, D. A. Callahan, D. S. Clark, J. D. Salmonson, B. A. Hammel, L. J. Atherton, R. C. Cook, M. J. Edwards, S. Glenzer, A. V. Hamza, S. P. Hatchett, M. C. Herrmann, D. E. Hinkel, D. D. Ho, H. Huang, O. S. Jones, J. Kline, G. Kyrala, O. L. Lan- den, B. J. MacGowan, M. M. Marinak, D. D. Meyerhofer, J. L. Milovich, K. A. Moreno, E. I. Mos...

    work page doi:10.1063/1.3592169 2010

  15. [15]

    R. B. Randolph, J. A. Oertel, D. W. Schmidt, M. N. Lee, B. M. Patterson, K. C. Henderson, and C. E. Hamil- ton, Process development and micro-machining of marble foam-cored rexolite hemi-shell ablator capsules, Fusion Science and Technology70, 230–236 (2016)

    work page 2016

  16. [16]

    R. E. Olson, T. J. Murphy, B. M. Haines, M. R. Douglas, B. J. Albright, M. A. Gunderson, Y. Kim, T. Cardenas, C. E. Hamilton, and R. B. Randolph, Development of the marble experimental platform at the national igni- tion facility, Physics of Plasmas27, 10.1063/5.0018819 (2020)

    work page doi:10.1063/5.0018819 2020

  17. [17]

    N. N. Vazirani, R. Sacks, B. M. Haines, M. J. Grosskopf, D. J. Stark, and P. A. Bradley, Bayesian batch optimiza- tion for molybdenum versus tungsten inertial confine- ment fusion double shell target design, Statistical Anal- ysis and Data Mining: The ASA Data Science Journal 17, 10.1002/sam.11698 (2024)

    work page doi:10.1002/sam.11698 2024

  18. [18]

    J. J. Kuczek and B. M. Haines, Simulated impact of fill tube geometry on recent high-yield implosions at the national ignition facility, Physics of Plasmas30, 10.1063/5.0156346 (2023)

    work page doi:10.1063/5.0156346 2023

  19. [19]

    B. M. Haines, W. S. Daughton, E. N. Loomis, E. C. Mer- ritt, D. S. Montgomery, J. P. Sauppe, and J. L. Kline, Computational study of instability and fill tube miti- gation strategies for double shell implosions, Physics of Plasmas26, 10.1063/1.5115031 (2019)

    work page doi:10.1063/1.5115031 2019

  20. [20]

    K. L. Baker, C. A. Thomas, T. R. Dittrich, O. Landen, G. Kyrala, D. T. Casey, C. R. Weber, J. Milovich, D. T. Woods, M. Schneider, S. F. Khan, B. K. Spears, A. Zyl- stra, C. Kong, J. Crippen, N. Alfonso, C. B. Yeamans, J. D. Moody, A. S. Moore, N. B. Meezan, A. Pak, D. N. Fittinghoff, P. L. Volegov, O. Hurricane, D. Callahan, P. Patel, and P. Amendt, Fill...

    work page doi:10.1063/5.0011385 2020

  21. [21]

    C. R. Weber, D. S. Clark, A. Pak, N. Alfonso, B. Bach- mann, L. F. Berzak Hopkins, T. Bunn, J. Crippen, L. Di- vol, T. Dittrich, A. L. Kritcher, O. L. Landen, S. Le Pape, A. G. MacPhee, E. Marley, L. P. Masse, J. L. Milovich, A. Nikroo, P. K. Patel, L. A. Pickworth, N. Rice, V. A. Smalyuk, and M. Stadermann, Mixing in icf implosions on the national igniti...

    work page doi:10.1063/1.5125599 2020

  22. [22]

    Zulick, Y

    C. Zulick, Y. Aglitskiy, M. Karasik, A. J. Schmitt, A. L. Velikovich, and S. P. Obenschain, Multimode hydrody- namic instability growth of preimposed isolated defects in ablatively driven foils, Phys. Rev. Lett.125, 055001 (2020)

    work page 2020

  23. [23]

    I. V. Igumenshchev, V. N. Goncharov, W. T. Shmayda, D. R. Harding, T. C. Sangster, and D. D. Meyerhofer, Ef- fects of local defect growth in direct-drive cryogenic im- plosions on omega, Physics of Plasmas20, 082703 (2013)

    work page 2013

  24. [24]

    Gardner, Ryan Turner, and Matthias Poloczek

    D. Eriksson, M. Pearce, J. R. Gardner, R. D. Turner, and M. Poloczek, Scalable global optimiza- tion via local bayesian optimization, arXiv e-prints 10.48550/arXiv.1910.01739 (2019), arXiv:1910.01739 [cs.LG]

    work page doi:10.48550/arxiv.1910.01739 1910

  25. [25]

    D. M. Sterbentz, C. F. Jekel, D. A. White, S. Aubry, H. E. Lorenzana, and J. L. Belof, Design optimization for richtmyer–meshkov instability suppression at shock- compressed material interfaces, Physics of Fluids34, 10 10.1063/5.0100100 (2022)

    work page doi:10.1063/5.0100100 2022

  26. [26]

    Aglitskiy, M

    Y. Aglitskiy, M. Karasik, A. L. Velikovich, V. Serlin, J. L. Weaver, T. J. Kessler, S. P. Nikitin, A. J. Schmitt, S. P. Obenschain, N. Metzler, and J. Oh, Observed transition from richtmyer-meshkov jet formation through feedout oscillations to rayleigh-taylor instability in a laser target, Physics of Plasmas19, 102707 (2012)

    work page 2012

  27. [27]

    Aglitskiy, A

    Y. Aglitskiy, A. L. Velikovich, M. Karasik, V. Serlin, C. J. Pawley, A. J. Schmitt, S. P. Obenschain, A. N. Mostovych, J. H. Gardner, and N. Metzler, Direct ob- servation of mass oscillations due to ablative richtmyer- meshkov instability in plastic targets, Phys. Rev. Lett. 87, 265001 (2001)

    work page 2001

  28. [28]

    Aglitskiy, A

    Y. Aglitskiy, A. L. Velikovich, M. Karasik, V. Ser- lin, C. J. Pawley, A. J. Schmitt, S. P. Obenschain, A. N. Mostovych, J. H. Gardner, and N. Metzler, Di- rect observation of mass oscillations due to ablative richt- myer–meshkov instability and feedout in planar plastic targets, Physics of Plasmas9, 2264 (2002)

    work page 2002

  29. [29]

    Christ, G

    F. Christ, G. Schaumann, N. Schott, J. Vetter, A. Blaeser, and M. Roth, Two-photon polymerization for inertial fusion energy target fabrication, Applied Physics A131, 10.1007/s00339-025-08657-x (2025)

    work page doi:10.1007/s00339-025-08657-x 2025

  30. [30]

    Pandolfi, T

    S. Pandolfi, T. Carver, D. Hodge, A. F. T. Leong, K. Kurzer-Ogul, P. Hart, E. Galtier, D. Khaghani, E. Cunningham, B. Nagler, H. J. Lee, C. Bolme, K. Ramos, K. Li, Y. Liu, A. Sakdinawat, S. Marchesini, P. M. Kozlowski, C. B. Curry, F.-J. Decker, S. Vetter, J. Shang, H. Aluie, M. Dayton, D. S. Montgomery, R. L. Sandberg, and A. E. Gleason, Novel fabricatio...

    work page 2022

  31. [31]

    Parisua˜ na, M

    C. Parisua˜ na, M. P. Valdivia, V. Bouffetier, K. Kurzer- Ogul, G. P´ erez-Callejo, S. Bott-Suzuki, A. Casner, N. S. Christiansen, N. Czapla, D. Eder, E. Galtier, S. H. Glen- zer, T. Goudal, B. M. Haines, D. Hodge, M. Ikeya, L. Izquierdo, D. Khaghani, Y. Kim, S. Klein, A. Koniges, H. J. Lee, M. Leininger, A. F. T. Leong, R. S. Lester, M. Makita, D. Mancel...

    work page 2025

  32. [32]

    D. S. Hodge, A. F. T. Leong, K. Kurzer-Ogul, S. Pandolfi, D. S. Montgomery, J. Shang, H. Aluie, S. Marchesini, Y. Liu, K. Li, A. Sakdinawat, E. C. Galtier, B. Nagler, H. J. Lee, E. F. Cunningham, T. E. Carver, C. A. Bolme, K. J. Ramos, D. Khaghani, P. M. Kozlowski, A. E. Glea- son, and R. L. Sandberg, Single-shot in-line x-ray phase- contrast imaging of v...

    work page 2025

  33. [33]

    E. M. Escauriza, J. P. Duarte, D. J. Chapman, M. E. Rutherford, L. Farbaniec, J. C. Jonsson, L. C. Smith, M. P. Olbinado, J. Skidmore, P. Foster, T. Ringrose, A. Rack, and D. E. Eakins, Collapse dynamics of spheri- cal cavities in a solid under shock loading, Scientific Re- ports10, 10.1038/s41598-020-64669-y (2020)

    work page doi:10.1038/s41598-020-64669-y 2020

  34. [34]

    Ranjan, J

    D. Ranjan, J. Oakley, and R. Bonazza, Shock-bubble interactions, Annual Review of Fluid Mechanics43, 117–140 (2011)

    work page 2011

  35. [35]

    Maler, O

    D. Maler, O. Belozerov, A. Godinger, S. Efimov, J. Strucka, Y. Yao, K. Mughal, B. Lukic, A. Rack, S. N. Bland, and Y. E. Krasik, Multi frame radiography of su- personic water jets interacting with a foil target, Journal of Applied Physics135, 10.1063/5.0186659 (2024)

    work page doi:10.1063/5.0186659 2024

  36. [36]

    V. I. Oreshkin and R. B. Baksht, Wire explosion in vacuum, IEEE Transactions on Plasma Science48, 1214–1248 (2020)

    work page 2020

  37. [37]

    G. T. Bokman, S. Fiorini, J. Strucka, B. Luki´ c, S. N. Bland, K. Mughal, S. Liu, A. Rack, and O. Supponen, Planar shock-induced bubble collapse and jetting in wa- ter captured via x-ray phase contrast imaging, Applied Physics Letters127, 014102 (2025)

    work page 2025

  38. [38]

    Strucka, B

    J. Strucka, B. Lukic, M. Koerner, J. W. D. Halliday, Y. Yao, K. Mughal, D. Maler, S. Efimov, J. Skidmore, A. Rack, Y. Krasik, J. Chittenden, and S. N. Bland, Synchrotron radiography of richtmyer–meshkov instabil- ity driven by exploding wire arrays, Physics of Fluids35, 10.1063/5.0144839 (2023)

    work page doi:10.1063/5.0144839 2023

  39. [39]

    M. P. Olbinado, X. Just, J.-L. Gelet, P. Lhuissier, M. Scheel, P. Vagovic, T. Sato, R. Graceffa, J. Schulz, A. Mancuso, J. Morse, and A. Rack, MHz frame rate hard x-ray phase-contrast imaging using synchrotron ra- diation, Optics Express25, 13857 (2017)

    work page 2017

  40. [40]

    M. P. Olbinado, V. Cantelli, O. Mathon, S. Pascarelli, J. Grenzer, A. Pelka, M. Roedel, I. Prencipe, A. L. Garcia, U. Helbig, D. Kraus, U. Schramm, T. Cowan, M. Scheel, P. Pradel, T. D. Resseguier, and A. Rack, Ul- tra high-speed x-ray imaging of laser-driven shock com- pression using synchrotron light, Journal of Physics D: Applied Physics51, 055601 (2018)

    work page 2018

  41. [41]

    Bakhrakh, O

    S. Bakhrakh, O. Drennov, and N. Kovalev,Hydrodynamic instability in strong media(1997)

    work page 1997

  42. [42]

    Anderson, A

    R. Anderson, A. Black, B. Blakeley, R. Bleile, J.-S. Camier, J. Ciurej, A. Cook, V. Dobrev, N. Elliott, J. Grondalski, C. Harrison, R. Hornung, T. Kolev, M. Legendre, W. Liu, W. Nissen, B. Olson, M. Osawe, G. Papadimitriou, O. Pearce, R. Pember, A. Skinner, D. Stevens, T. Stitt, L. Taylor, V. Tomov, R. Rieben, A. Vargas, K. Weiss, D. White, and L. Busby,T...

    work page 2020

  43. [43]

    Rieben, Poster: The MARBL multi-physics code, in Exascale Computing Project Annual Meeting(2020)

    R. Rieben, Poster: The MARBL multi-physics code, in Exascale Computing Project Annual Meeting(2020)

    work page 2020

  44. [44]

    R. W. Anderson, V. A. Dobrev, T. V. Kolev, R. N. Rieben, and V. Z. Tomov, High-order multi-material ALE hydrodynamics, SIAM J. Sci. Comput.40, B32 (2018)

    work page 2018

  45. [45]

    Dimonte, G

    G. Dimonte, G. Terrones, F. J. Cherne, T. C. Germann, V. Dupont, K. Kadau, W. T. Buttler, D. M. Oro, C. Mor- ris, and D. L. Preston, Use of the Richtmyer–Meshkov instability to infer yield stress at high-energy densities, Phys. Rev. Lett.107, 264502 (2011)

    work page 2011

  46. [46]

    D. M. Sterbentz, C. F. Jekel, D. A. White, R. N. Rieben, and J. L. Belof, Linear shaped-charge jet optimization using machine learning methods, Journal of Applied Physics134, 10.1063/5.0156373 (2023)

    work page doi:10.1063/5.0156373 2023

  47. [47]

    M. B. Prime, S. J. Fensin, D. R. Jones, J. W. Dyer, and D. T. Martinez, Multiscale richtmyer-meshkov in- stability experiments to isolate the strain rate depen- dence of strength, Physical Review E109, 10.1103/phys- reve.109.015002 (2024)

    work page doi:10.1103/phys- 2024