Simulating the thermodynamics of gas, radiation, and multispecies dust: Method and applications to protoplanetary disks
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Introduction to the show: ident: Astrophysics Radio. Generated commentary on the latest astrophysics papers.
Vera: Today's paper: "Simulating the thermodynamics of gas, radiation, and multispecies dust".
Jocelyn: The thermodynamics of protoplanetary disks, governed by a complex interplay between gas, dust, and radiation, exerts a strong influence on their morphology and dynamics at both large and small scales.
Vera: First, who's behind it and why it matters.
Title and authors: Vera: So Jocelyn, I was looking at the title of this paper, "Simulating the thermodynamics of gas, radiation, and multispecies dust: Method and applications to protoplanetary disks," and it sounds really comprehensive. It suggests they're tackling a lot of complexity in how gas, dust, and radiation all interact within these disks.
Jocelyn: I agree with you, Vera; the title immediately tells me this isn't just a simple hydrodynamical simulation anymore; they are focusing on the thermodynamics and the multispecies aspect. It implies they are looking at how things change based on energy exchange between all those components, which is what we always worry about in these simulations.
Subrahmanyan: From a theoretical perspective, that focus on thermodynamics is significant because it addresses a major limitation in previous modeling approaches where things were often simplified or treated separately. It suggests they are moving toward a more physically motivated description of the disk's state.
Vera: Exactly, Subrahmanyan; it sounds like they are taking existing simulations and adding a much richer layer of physical detail regarding how energy moves around the disk. It points to a deeper look at the physics governing the structure we observe in protoplanetary disks.
Jocelyn: I think for us listeners, it means we're getting a more detailed picture of what goes on inside these dusty environments, not just where the dust is located, but how hot or cold it is and how that affects everything else.
Subrahmanyan: It suggests a shift away from just tracking density and velocity toward understanding the energy balance that dictates those structures at both large and small scales. That's a big step in connecting theory to observation.
The paper's summary: Vera: What I see in the summary of this paper, "Simulating the thermodynamics of gas, radiation, and multispecies dust: Method and applications to protoplanetary disks," is that they are addressing the fact that older hydrodynamical simulations often used rough estimates like local isothermality or parametrized beta-cooling. This new approach aims for something more complete.
Jocelyn: Right, Vera; the summary points out that they are moving beyond those approximate methods and instead using a radiation-hydrodynamics scheme that includes energy exchange for gas, radiation, and multiple species of dust. That's a lot of physical processes being accounted for at once.
Subrahmanyan: The core idea seems to be that they've developed a method based on detailed calculations of equilibrium dust distribution, temperature structure, and collisional or radiative relaxation timescales to make the modeling more realistic. That foundation is crucial for connecting simulation output to real astrophysical conditions.
Vera: That makes sense; they are basing their thermodynamic prescriptions on actual calculations rather than just assuming simple exponential thermal relaxation to a fixed background as was often done before. It sounds like they are building a framework that allows the dust and gas temperatures to behave in a way that is physically expected, especially in upper layers.
Jocelyn: The summary highlights the introduction of a three-temperature or 3T scheme based on the M1 method for the PLUTO code, which lets them self-consistently evolve the separate energies of gas, dust, and radiation through things like thermal accommodation and stellar irradiation. That’s a sophisticated way to handle coupling.
Subrahmanyan: That three-temperature scheme is interesting because it allows dust and gas temperatures to decouple in upper layers while still being coupled in other ways through energy exchange mechanisms like absorption or emission of radiation. It shows they're capturing complexity without losing numerical tractability too quickly.
The paper's improvements: Vera: When we look at the suggested improvements, what stands out to me is how they compare modeling dust as superparticles with a pressureless-fluid approach, noting that the pressureless fluid method loses realism when the Stokes number St ts K one. That’s a key technical detail for accuracy.
Jocelyn: I see; so they are flagging that treating dust purely as a pressureless fluid isn't always realistic, especially when those grains are large enough that their inertia matters significantly in the dynamics. It suggests they recognize the limitations of that simplification in certain regimes.
Subrahmanyan: It confirms what we often see in theory—that approximations work best when the physical parameters allow them to be valid; so this paper is emphasizing the regime where those approximations start to fail, which is important for setting realistic simulation boundaries.
Vera: And they also mention that using local dust abundance just to compute opacities without considering collisional thermal relaxation rates isn't enough, because you need that thermal relaxation coupling too. It sounds like the improvement involves incorporating those detailed collisional and radiative relaxation timescales into the overall structure calculation.
Jocelyn: So, it’s not just about how much dust is there, but how fast that dust can exchange energy with its environment; that's a deeper level of interaction they are aiming for in their simulation.
Subrahmanyan: That level of detail is what allows them to move beyond simpler models and capture the intricate thermal structure of the disk more accurately. It moves the modeling from just describing where things are to describing how those things actually behave thermally over time.
Conclusion: Vera: So, wrapping up this discussion on "Simulating the thermodynamics of gas, radiation, and multispecies dust: Method and applications to protoplanetary disks," it seems the main implication is that we can now compute variables like temperatures, velocities, and densities self-consistently within a single simulation without making assumptions about local thermal equilibrium.
Jocelyn: That's right; the method allows them to reproduce that "twotemperature" limit seen in tightly coupled regimes while accurately modeling things like dust ring formation at pressure bumps and sublimation fronts. It’s a significant step forward because it means we can test those complex physical features without relying on pre-assumed equilibrium conditions.
Subrahmanyan: Theoretically, this capability to compute these variables self-consistently is valuable because it directly impacts how we model the physics of disk substructure driven by planets or shadows, as well as infalling streamers (Kuznetsova et al. two thousand twenty-two).
Vera: It really sets a new standard for how we can use these simulations to generate mock observational data, allowing us to test other models against high-fidelity results derived from this method. We're heading toward a time where we can use these simulations much more effectively for predictive modeling.
Jocelyn: I think the ability to generate synthetic data that reflects the true thermodynamic complexity is what really opens up new avenues for testing our understanding of disk evolution and planet formation processes.
Subrahmanyan: Indeed, by incorporating multiple species of dust with their individual self-consistent dynamics, this method builds upon its precursor which only used an explicit step, allowing us to define dust opacity as kappa d,j = S j(T d,j) kappa zero and consider a single dust species perfectly coupled to the gas. This makes it possible to reproduce spatial variations in grain opacity and size distributions by incorporating phenomena such as radial drift (e.g., Dullemond et al. two thousand eighteen) and dust settling (e.g., Bae et al. two thousand twenty-one).
Vera: So, the big picture here is that this paper gives us a powerful new tool to get closer to understanding how large-scale disk substructure is driven by planets or shadows or infalling streamers (Kuznetsova et al. two thousand twenty-two).
Jocelyn: It’s exciting because we can finally model things like dust ring formation at pressure bumps and sublimation fronts with the level of detail required to connect simulations to what we see in scattered light or continuum observations.
Subrahmanyan: That level of detail allows us to move from just theoretical concepts to simulating the actual dynamical processes that shape these regions.
Max-Planck-Institut für Astronomie · Max-Planck-Institut für Astrophysik
astro-ph.EP, astro-ph.IM
Submitted: 2026-09-24
Updated: 2026-09-24
Comments: 18 pages (+7 pages appendix), 13 figures. Accepted to Astronomy and Astrophysics; further comments and questions welcome
License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
Importance score: 80/100
The gist: The thermodynamics of protoplanetary disks, governed by a complex interplay between gas, dust, and radiation, exerts a strong influence on their morphology and dynamics at both large and small scales.
Key concepts
- Thermodynamics of Protoplanetary Disks
- This involves understanding the complex interplay between gas, dust, and radiation within protoplanetary disks. It dictates the disk's morphology and dynamics at various scales by focusing on how energy exchanges affect the physical state of these components.
- Three-Temperature (3T) Scheme
- This method used in the simulation allows gas and dust temperatures to evolve separately while still being coupled through energy exchange mechanisms like radiation absorption or emission. It captures complexity without losing numerical tractability.
- Dust Superparticles vs. Pressureless Fluid
- The paper notes that treating dust purely as a pressureless fluid is inaccurate when grain inertia matters, especially for larger grains. This highlights the need to use methods that account for the physical properties of dust particles in certain regimes.
- Collisional and Radiative Relaxation Timescales
- These timescales are incorporated into the modeling to ensure that dust energy exchange with its environment is accurately represented. This detail is crucial for capturing how dust interacts thermally with the surrounding gas.
Terminology
Summary
The thermodynamics of protoplanetary disks, governed by a complex interplay between gas, dust, and radiation, exerts a strong influence on their morphology and dynamics at both large and small scales. Historically, hydrodynamical simulations have treated thermodynamics with approximate prescriptions such as local isothermality or parametrized β-cooling. The authors devised a radiation-hydrodynamics scheme for the PLUTO code that includes energy exchange (via absorption, emission, and collisions) for gas, radiation, and multiple species of dust. Dust-gas dynamics are handled by treating each dust species as a pressureless, diffusive fluid to represent changes in disk illumination caused by grain settling and trapping.
The paper addresses the limitations of existing modeling approaches. Thermochemical models like ProDiMo or DALI are too computationally expensive to couple with gas dynamics because energy exchange must be recomputed at each timestep. Simulations have historically assumed locally isothermal equations of state or adiabatic equations with exponential thermal relaxation to a fixed background. In contrast, the authors advocate for physically-motivated thermodynamic prescriptions based on detailed calculations of equilibrium dust distribution, temperature structure, and collisional/radiative relaxation timescales. They introduce a three-temperature (3T) scheme based on the M1 method for the PLUTO code that self-consistently evolves the separate energies of gas, dust, and radiation via thermal accommodation, absorption/emission of radiation, and stellar irradiation to allow dust and gas temperatures to decouple in upper layers.
The authors compare modeling dust as superparticles (which suffers from Poisson noise) versus a pressureless-fluid approach (which loses realism when Stokes number St ≡ tsomegaK ≳ 1). They also note that using multiple pressureless fluids with collisional β-cooling rates, or local dust abundance to compute opacities without considering collisional thermal relaxation, are existing approaches.
The paper develops a numerical method to compute the dynamical and thermodynamical coupling between gas, radiation, and multiple species of dust within the grid-based PLUTO code. The solution strategy involves an implicit-explicit (IMEX) scheme (IMEX1) to combine implicitly integrated source terms with non-stiff explicit transport terms. The simulation timestep is determined by the CFL criterion. A Strang-split approach is used for radiation blocks, where energy and momentum exchange between gas, dust, and radiation are computed implicitly, while radiation transport is computed explicitly within substeps of length ∆trad to ensure numerical stability.
The energy and momentum updates are performed using a Newton-Raphson technique. The linearized energy update (Equation A.1a) shows the coupling between the radiation field, gas internal energy, and dust internal energy:
i+1 δXg /∆t = − δEgi+1 /∆t + cκi+1 − 4ar Tg3,i+1 Wgi+1 δEgi+1 g ρg (δEr −4ar Tgj=1
The momentum update involves solving a system of equations where the dust species do not directly interact with one another but influence each other through their effects on gas and dust energy and momenta. The resulting reduced Jacobian matrices allow for a significant reduction in computational complexity from O((nd + 2)3) to O(nd).
Conservation laws are verified, showing that the implicit step conserves the sum of all internal energies and momenta, modified only by the injection of energy to the system via stellar irradiation. The conservation law for total energy (Equation A.11) shows that the residuals cancel, and terms of the form Exi+1,∗k + δExi+1,∗k have been identified with the energy value at the next iteration.
The paper presents several test problems to verify functionality:
Energy and momentum coupling:
"In Figure 2, we plot the evolution of the temperatures and velocities of all species in the top and middle panels. Over the lifetime of the simulation, all species relax to the same temperature and velocity, at which point the energy and momentum exchange terms net to zero."
Ray-traced irradiation:
The authors test ray-traced starlight by assigning frequency-dependent absorption opacities (Equation 33) and initial fluxes based on a sum over frequency bands (Equation 34). They show that the resulting gas-pressure gradient drives motions, and the radiation flux couples to dust momentum.
Ray-traced force on dust:
They verify the radiative force by setting all stopping times to a large value and decoupling dynamics, showing that the velocity of each grain species would be expected to evolve as vd,j (t) = Fr σd,j t,
with relative deviation less than 10−3 at all times.
Multispecies dusty shock:
The method is tested in the presence of shocks, where analytical solutions for dust velocities are compared to numerical simulations, finding close agreement between simulation outputs (open circles, sampled every 5 grid cells) and analytical theory (solid curves).
Diffusion in a homogeneous medium:
For pure diffusion, the analytical evolution of dust density is solved using Equation (39), which yields the classical Gaussian vertical profile of protoplanetary disks. The numerical solution agrees well with this analytical form across many orders of magnitude in density.
Vertical dust settling:
The vertical structure is analyzed by balancing gravity and pressure support, leading to a characteristic dust scale height derived from Equations (40) and (42). They find that the dust scale height is Hd,j = p / (1 + Stj /α).
Radial drift:
The radial drift velocity is governed by Equation (45), which shows that for large bodies (St ≫ 1), angular momentum loss and thus radial drift are very slow. They verify the correct implementation of geometric source terms in curvilinear coordinates, finding that the numerical results agree with analytical predictions, with the error decreasing linearly with increasing Stokes number St.
Radial dust trapping:
They test a scenario where pressure bumps create a local maximum in radial drift velocity (Equation D.11). The equilibrium between dust-gas drag and diffusion sets the ring width, yielding a characteristic dust concentration width of wdg ≡ −α(St + St−1)/(p−1g ∂R pg)Rmax,
which shows that both small and large grains would not concentrate at the pressure bump.
Application: Dust drift and sublimation:
In the final application, they simulate dust drifting inward toward the star. They incorporate a novel numerical method where dust opacity and stopping time are functions of temperature (Equation 52), allowing for a phase transition from solid to gas at sublimation temperatures (e.g., Tsub ≈ 150 K for water ice). This treatment demonstrates that the simulation accurately reproduces the true steadystate solution even when local thermodynamic equilibrium (LTE) between gas, dust, and radiation cannot be assumed.
The authors conclude by summarizing their method as a novel numerical method that solves for thermodynamic coupling between gas, dust, and radiation. They state that this enables the computation of variables like temperatures, velocities, and densities self-consistently within a single simulation. This capability will significantly benefit investigations of how large-scale disk substructure is driven by planets or shadows. The methods presented are a starting point for future improvements, such as incorporating photoelectric heating or gas line transitions. Additionally, they suggest generalizing frictional heating to apply to each dust species separately and directly incorporating dynamical coupling into the solution of the Riemann problem.
The paper concludes with an extensive list of references covering topics from hydrodynamics and radiative transfer to specific dust dynamics applications. The simulations were carried out on VERA, FREYA, and ORION clusters at MPCDF in Germany. The authors acknowledge helpful discussions on scientific applications with various researchers and thank the anonymous referee for suggestions that improved the quality of the paper.
The final conclusion emphasizes that by incorporating multiple species of dust, their individual self-consistent dynamics (drag and diffusion), this method builds upon its precursor, which only used an explicit step in the temperature scheme. They can therefore define dust opacity as κd,j = Sj (Td,j)κ0 and consider a single dust species perfectly coupled to the gas. These changes make it possible to reproduce spa[cial] variations in grain opacity and size distributions by incorporating phenomena such as radial drift and dust settling. This reproduces more [realistic] observational features of protoplanetary disks. Monte Carlo radiative transfer (MCRT) tools can then be used to convert hydrodynamical simulations into multiwavelength mock images for comparison with observations, where the new method allows these variables to be computed self-consistently within a single simulation, greatly improving the predictive power of mock observations. This would significantly benefit investigations of how large-scale disk substructure, whether driven by planets (Speedie et al. 2022), shadows (Zhang & Zhu 2024), or infalling streamers (Kuznetsova et al. 2022), and their observational appearance in near-infrared scattered light (tracing small grains), millimeter/submillimeter continuum (tracing large grains), and various molecular lines (tracing the gas). Circumplanetary disks are also a potential application, where thermal relaxation timescales depend on the dynamically evolving size distribution of dust in the circumplanetary region. The opacities and stopping times which mediate thermal relaxation are, in turn, determined by the dynamically evolving size distribution and abundances of dust in the circumplanetary region."
The paper is structured with sections detailing equations (2) through (53), solution strategies (3), and test problems (6). Figures 1 through 13 provide graphical summaries of the simulation results. The Appendix details the linearized energy and momentum updates, including the full set of Jacobian matrices for each species. Appendix D provides derivations for key source terms like irradiation heating and ring-trapping tests. The overall structure is designed to demonstrate a comprehensive numerical method capable of handling the stiffness inherent in coupling gas, radiation, and multiple dust species across various physical regimes.
The authors explicitly state that the new method allows them to reproduce the twotemperature
limit used in most radiation-hydrodynamics schemes when dust and gas are tightly coupled. They also confirm that they have designed a novel numerical method where Tsub,j = 2000 K + j × (500 K) is a smooth planetary disks.
The final summary of the paper is:
"We have designed and implemented a novel numerical method that solves for thermodynamic coupling between gas, dust, and radiation, and in a number of test problems, where Tsub,j = 2000 K + j × (500 K) is the sublimation temperature. By incorporating multiple species of dust, our method builds upon its precursor [which only used an explicit step] to ensure numerical stability in the iterative each with its own self-consistent dynamics (drag and diffusion), and δsub = 10−10 is a small factor to pre-fusion), our method builds upon its precursor, which only used an explicit step. We can therefore define κd,j = Sj (Td,j)κ0 and consider a single dust species perfectly coupled to the gas. These changes make it possible to reproduce spa[cial] variations in grain opacity and size distributions by incorporating phenomena such as radial drift (e.g., Dullemond et al. 2018) and dust settling (e.g., Bae et al. 2021). These comprehensive treatments (e.g., Wang et al. 2023) in the set the local frequency-integrated opacities and gas-grain thermal accommodation timescales, and in turn the heating, cooling, and background temperature structure of the disk as a whole."
The paper is essentially a detailed description of a new radiation-hydrodynamics scheme for simulating protoplanetary disks that self-consistently couples gas dynamics with multiple species of dust by treating dust as pressureless fluids. It details the numerical implementation using an IMEX1 scheme and Newton-Raphson iterations to solve the coupled energy and momentum equations, ensuring conservation laws are satisfied in each iteration. The paper rigorously tests this method across various physical scenarios, including thermal relaxation times, radiative heating from starlight (ray-traced irradiation), collisional coupling, shocks, diffusion in homogeneous media (leading to Gaussian profiles), vertical settling of dust grains to the midplane, and radial drift toward pressure maxima or sublimation fronts. The key innovation lies in treating the dust energy and temperature evolution self-consistently with radiation and gas via coupled source terms derived from detailed physical processes like collisional coupling (Equation 8) and frictional heating (Equation 9), while also incorporating a gradient-diffusion prescription for dust transport (Equation 11). This allows for the computation of variables like temperatures, velocities, and densities self-consistently within a single simulation. The method is shown to be numerically stable and accurate across various resolutions, with errors decreasing as the timestep is refined. It successfully reproduces the twotemperature
limit in tightly coupled regimes and accurately models complex phenomena such as dust ring formation at pressure bumps and sublimation fronts, demonstrating its utility for understanding planet formation processes in protoplanetary disks."
The paper is essentially a detailed description of a new radiation-hydrodynamics scheme for simulating protoplanetary disks that self-consistently couples gas dynamics with multiple species of dust by treating dust as pressureless fluids. It details the numerical implementation using an IM
Improvements for AI systems
Based on this scientific paper, here are specific improvements that could be made to AI systems, categorized by the capabilities they would gain:
)AI System Improvement 1: Multiphysics Simulation Engine for Protoplanetary Disks (The Core Method)
This paper introduces a novel radiation-hydrodynamics scheme coupled with multiple pressureless dust fluids, treating gas, radiation, and multispecies dust self-consistently.
Improvements to the AI system would involve implementing this scheme as a core module within a general-purpose astrophysical simulation framework.
-
The AI system should be capable of solving complex conservation laws (Equations 1a-1d) incorporating:
-
A multi-fluid approach (gas + multiple pressureless dust species, treated as tracers/diffusive fluids).
-
Self-consistent energy exchange mechanisms including absorption, emission, and collisions between gas, radiation, and all dust species (Equations 7 through 9).
-
Dynamic radiation transport using a frequency-integrated moment method with the M1 closure (Equation 3), allowing for the evolution of background temperature profiles.
-
Explicit treatment of collisional coupling terms (momentum exchange and frictional heating) that depend on local dust abundance and grain size distribution (Equations 7-9).
-
Modeling dust advection and diffusion using a gradient-diffusion prescription, including the calculation of momentum transport due to this flux (Equations 11-12).
The improved AI system could:
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Accurately predict the morphology and dynamics of protoplanetary disks (e.g., spiral structures, gaps) under conditions where dust settling and trapping significantly alter radiation profiles.
-
Simulate the thermal decoupling between gas and dust in different disk regions (atmosphere vs. midplane) based on grain size distribution and stopping times.
-
Model the effects of planetary accretion or shadowing on radial temperature gradients by treating radiation transport dynamically rather than using fixed background profiles.
)AI System Improvement 2: Self-Consistent Thermodynamic Modeling for Chemical/Physical Properties
The paper demonstrates how dust properties (opacity, specific heat capacity, sublimation temperature) evolve based on their local thermodynamic state (temperature).
Improvements to the AI system would involve integrating this feedback loop into property calculation routines.
-
The AI system should incorporate a dynamic relationship where dust properties are functions of the local gas/dust temperature:
-
Dust opacity and specific heat capacity should be calculated using temperature-dependent functional forms (Equations 5, 33).
-
The sublimation front for various dust species must be dynamically determined based on their evolving temperature profile (Equation 52).
The improved AI system could:
-
Simulate the chemical evolution of disk material by tracking which dust species are sublimated and entrained in the gas due to local heating events (e.g., near a star or planet).
-
Predict the resulting changes in dust size distribution and abundance profiles as a function of disk evolution, crucial for understanding planetesimal formation pathways.
)AI System Improvement 3: Advanced Numerical Solver for Stiff Systems
The paper utilizes an Implicit-Explicit (IMEX) scheme combined with Newton-Raphson iteration and Jacobian matrix reduction to solve the coupled, potentially stiff equations efficiently.
Improvements to the AI system would involve optimizing its numerical backbone for long-term stability and speed.
-
The solver should employ an IMEX time integration scheme (Equation 16) where radiation/source terms are treated implicitly and hydrodynamical advection/diffusion is treated explicitly.
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It must utilize algebraic rowreduction of the Jacobian matrices for energy and momentum exchange to reduce computational complexity from cubic to quadratic in the number of unknowns (Equations 4.3, 4.4).
-
The system should be able to handle
stiff
dynamics where collisional coupling times are much shorter than hydrodynamic timescales (i.e., when dust and gas temperatures rapidly equilibrate) using appropriate implicit treatments for the source terms (Appendix A).
The improved AI system could:
-
Perform long-term, stable simulations of protoplanetary disks over many dynamical times without accumulating significant numerical errors in total energy or momentum conservation.
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Achieve high computational efficiency by solving the massive coupled system through reduced Jacobian methods, making complex multi-species simulations tractable for large grids.
)AI System Improvement 4: Predictive Modeling for Astrophysical Observables (Synthetic Data Generation)
The paper provides a framework to compute self-consistent thermodynamic variables (T, v, density) without relying on pre-assumptions like local thermal equilibrium (LTE).
Improvements to the AI system would involve using the simulation output as a high-fidelity data generator.
-
The AI system should be capable of running simulations that yield full spatio-temporal fields for gas temperature, dust temperature, and radiation energy density (Figures 2, 3).
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It must integrate these fields with Monte Carlo radiative transfer (MCRT) tools to generate synthetic observational data across various wavelengths (e.g., near-infrared scattered light for small grains, millimeter continuum for large grains).
The improved AI system could:
-
Generate realistic mock observational data sets that accurately reflect the complex interplay between gas, dust, and radiation in protoplanetary disks.
-
Test and validate other AI models or physical theories by comparing their predictions against these high-fidelity synthetic datasets, thereby accelerating discovery in astrophysical modeling.
Sources
- An analytical test case for dust dynamics during a shock-wave passage
- Vertical shear instability in two-moment radiation-hydrodynamical simulations of irradiated protoplanetary disks II. Secondary instabilities and stability regions
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