Josh Borrow’s research while affiliated with Massachusetts Institute of Technology and other places

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Publications (66)


The impact of galaxy selection on the splashback boundaries of galaxy clusters
  • Article

March 2022

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13 Reads

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14 Citations

Monthly Notices of the Royal Astronomical Society

Stephanie O’Neil

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Josh Borrow

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Benedikt Diemer

We explore how the splashback radius (Rsp) of galaxy clusters, measured using the number density of the subhalo population, changes based on various selection criteria using the IllustrisTNG cosmological galaxy formation simulation. We identify Rsp by extracting the steepest radial gradient in a stacked set of clusters in 0.5 dex wide mass bins, with our clusters having halo masses 1013 ≤ M200, mean/M⊙ ≤ 1015. We apply cuts in subhalo mass, galaxy stellar mass, i-band absolute magnitude and specific star formation rate. We find that, generally, galaxies of increasing mass and luminosity trace smaller measured splashback radii relative to the intrinsic dark matter radius. We also show that quenched galaxies may be used to reliably reconstruct the dark matter splashback radius. This trend is likely due to changes in the galaxy population. Additionally, we are able to reconcile different observational predictions that Rsp based upon galaxy number counts and dark matter may either align or show significant offset (e.g. those using optically- or SZ-selected clusters) through the selection functions that these studies employ. Finally, we demonstrate that changes in Rsp measured through number counts are not due to a simple change in galaxy abundance inside and outside of the cluster.


Figure 1. Density slices through the midplane of the simulation box at í µí±¡ ≈ 5í µí±¡ cc , for initial density contrasts í µí¼’ = 10 (left) and í µí¼’ = 100 (right), at the highest resolution (í µí±› = 128 3 ). Large morphological differences can be observed.
Figure 6. Projection of the mass at intermediate temperatures for initial density contrast í µí¼’ = 100 at time í µí±¡ ≈ 5t cc . Very different morphologies are apparent, even among those methods for which the covering fractions are similar (e.g. compare and ). The grid-like artifacts from the method are clearly visible.
Figure 7. Evolution of the mass of dense gas (top) and intermediate-temperature gas (bottom) for the SSSSSSS hydrodynamics method. Initial density contrasts are í µí¼’ = 10 (left) and í µí¼’ = 100 (right). The black lines show the evolution of the different gas phases after coarse-graining to the common resolution of 32 3 grid-cells.
Sensitivity of non-radiative cloud-wind interactions to the hydrodynamics solver
  • Preprint
  • File available

March 2022

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36 Reads

Cloud-wind interactions are common in the interstellar and circumgalactic media. Many studies have used simulations of such interactions to investigate the effect of particular physical processes, but the impact of the choice of hydrodynamics solver has largely been overlooked. Here we study the cloud-wind interaction, also known as the "blob test", using seven different hydrodynamics solvers: Three flavours of SPH, a moving mesh, adaptive mesh refinement and two meshless schemes. The evolution of masses in dense gas and intermediate-temperature gas, as well as the covering fraction of intermediate-temperature gas, are systematically compared for initial density contrasts of 10 and 100, and four numerical resolutions. To isolate the differences due to the hydrodynamics solvers, we use non-radiative simulations without physical conduction. We find large differences between these methods. SPH methods show slower dispersal of the cloud, particularly for the higher density contrast, but faster convergence, especially for the lower density contrast. Predictions for the intermediate-temperature gas differ particularly strongly, also between non-SPH codes, and converge most slowly. We conclude that the hydrodynamical interaction between a dense cloud and a supersonic wind remains an unsolved problem. Studies aiming to understand the physics or observational signatures of cloud-wind interactions should test the robustness of their results by comparing different hydrodynamics solvers.

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The impact of galaxy selection on the splashback boundaries of galaxy clusters

February 2022

·

14 Reads

We explore how the splashback radius (RspR_{\rm sp}) of galaxy clusters, measured using the number density of the subhalo population, changes based on various selection criteria using the IllustrisTNG cosmological galaxy formation simulation. We identify RspR_{\rm sp} by extracting the steepest radial gradient in a stacked set of clusters in 0.5 dex wide mass bins, with our clusters having halo masses 1013M200,mean/M101510^{13} \leq M_{\rm 200, mean} / {\rm M}_\odot \leq 10^{15}. We apply cuts in subhalo mass, galaxy stellar mass, i-band absolute magnitude and specific star formation rate. We find that, generally, galaxies of increasing mass and luminosity trace smaller measured splashback radii relative to the intrinsic dark matter radius. We also show that quenched galaxies may be used to reliably reconstruct the dark matter splashback radius. This trend is likely due to changes in the galaxy population. Additionally, we are able to reconcile different observational predictions that RspR_{\rm sp} based upon galaxy number counts and dark matter may either align or show significant offset (e.g. those using optically- or SZ-selected clusters) through the selection functions that these studies employ. Finally, we demonstrate that changes in RspR_{\rm sp} measured through number counts are not due to a simple change in galaxy abundance inside and outside of the cluster.


Sphenix : Smoothed Particle Hydrodynamics for the next generation of galaxy formation simulations

November 2021

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39 Reads

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75 Citations

Monthly Notices of the Royal Astronomical Society

Smoothed Particle Hydrodynamics (SPH) is a ubiquitous numerical method for solving the fluid equations, and is prized for its conservation properties, natural adaptivity, and simplicity. We introduce the Sphenix SPH scheme, which was designed with three key goals in mind: to work well with sub-grid physics modules that inject energy, be highly computationally efficient (both in terms of compute and memory), and to be Lagrangian. Sphenix uses a Density-Energy equation of motion, along with variable artificial viscosity and conduction, including limiters designed to work with common sub-grid models of galaxy formation. In particular, we present and test a novel limiter that prevents conduction across shocks, preventing spurious radiative losses in feedback events. Sphenix is shown to solve many difficult test problems for traditional SPH, including fluid mixing and vorticity conservation, and it is shown to produce convergent behaviour in all tests where this is appropriate. Crucially, we use the same parameters within Sphenix for the various switches throughout, to demonstrate the performance of the scheme as it would be used in production simulations. Sphenix is the new default scheme in the Swift cosmological simulation code and is available open-source.


Sígame v3: Gas Fragmentation in Postprocessing of Cosmological Simulations for More Accurate Infrared Line Emission Modeling

November 2021

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13 Reads

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17 Citations

The Astrophysical Journal

Karen Pardos Olsen

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Mordecai-Mark Mac Low

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[...]

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Desika Narayanan

We present an update to the framework called Simulator of Galaxy Millimeter/submillimeter Emission ( sígame ). sígame derives line emission in the far-infrared (FIR) for galaxies in particle-based cosmological hydrodynamics simulations by applying radiative transfer and physics recipes via a postprocessing step after completion of the simulation. In this version, a new technique is developed to model higher gas densities by parameterizing the probability distribution function (PDF) of the gas density in higher-resolution simulations run with the pseudo-Lagrangian, Voronoi mesh code arepo . The parameterized PDFs are used as a look-up table, and reach higher densities than in previous work. sígame v3 is tested on redshift z = 0 galaxies drawn from the simba cosmological simulation for eight FIR emission lines tracing vastly different phases of the interstellar medium. This version of sígame includes dust radiative transfer with S kirt and high-resolution photoionization models with C loudy , the latter sampled according to the density PDF of the arepo simulations to augment the densities in the cosmological simulation. The quartile distributions of the predicted line luminosities overlap with the observed range for nearby galaxies of similar star formation rate (SFR) for all but two emission lines: [O i ]63 and CO(3–2), which are overestimated by median factors of 1.3 and 1.0 dex, respectively, compared to the observed line–SFR relation of mixed-type galaxies. We attribute the remaining disagreement with observations to the lack of precise attenuation of the interstellar light on sub-grid scales (≲200 pc) and differences in sample selection.


The importance of black hole repositioning for galaxy formation simulations

September 2021

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11 Reads

Active galactic nucleus (AGN) feedback from accreting supermassive black holes (SMBHs) is an essential ingredient of galaxy formation simulations. The orbital evolution of SMBHs is affected by dynamical friction that cannot be predicted self-consistently by contemporary simulations of galaxy formation in representative volumes. Instead, such simulations typically use a simple "repositioning" of SMBHs, but the effects of this approach on SMBH and galaxy properties have not yet been investigated systematically. Based on a suite of smoothed particle hydrodynamics simulations with the SWIFT code and a Bondi-Hoyle-Lyttleton subgrid gas accretion model, we investigate the impact of repositioning on SMBH growth and on other baryonic components through AGN feedback. Across at least a factor ~1000 in mass resolution, SMBH repositioning (or an equivalent approach) is a necessary prerequisite for AGN feedback; without it, black hole growth is negligible. Limiting the effective repositioning speed to \lesssim 10 km/s delays the onset of AGN feedback and severely limits its impact on stellar mass growth in the centre of massive galaxies. Repositioning has three direct physical consequences. It promotes SMBH mergers and thus accelerates their initial growth. In addition, it raises the peak density of the ambient gas and reduces the SMBH velocity relative to it, giving a combined boost to the accretion rate that can reach many orders of magnitude. Our results suggest that a more sophisticated and/or better calibrated treatment of SMBH repositioning is a critical step towards more predictive galaxy formation simulations.


Projecting SPH Particles in Adaptive Environments

June 2021

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10 Reads

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3 Citations

The reconstruction of a smooth field onto a fixed grid is a necessary step for direct comparisons to various real-world observations. Projecting SPH data onto a fixed grid becomes challenging in adaptive environments, where some particles may have smoothing lengths far below the grid size, whilst others are resolved by thousands of pixels. In this paper we show how the common approach of treating particles below the grid size as Monte Carlo tracers of the field leads to significant reconstruction errors, and despite good convergence properties is unacceptable for use in synthetic observations in astrophysics. We propose a new method, where particles smaller than the grid size are `blitted' onto the grid using a high-resolution pre-calculated kernel, and those close to the grid size are subsampled, that allows for converged predictions for projected quantities at all grid sizes.


Figure 3. The same as Fig. 2, however this time using an approximate algorithm that only updates the self-contribution of the heated particle. This version of the algorithm shows non-convergent behaviour at low-energy injection values, but is significantly computationally cheaper than solutions that require neighbour loops during the iteration procedure.
Figure 4. Comparison between the simple energy injection procedure (Fig. 3, solid lines) against the method including a neighbour loop each iteration (Fig. 2, dashed lines) for various energy injection values. The vertical axis here shows the energy offset from the true requested energy (in absolute arbitrary code units). The neighbour loop approach allows for the injected energy error to decrease with each iteration, where the simple procedure has a fixed (injection dependent) energy error that is reached rapidly at low values of energy injection where the entropies of neighbouring particles remain dominant.
Figure 7. The same lines as Fig. 6, except now showing the 'error' as a function of time relative to the single-dt case (blue dashed line) of the pressurêpressurê P of the nearest neighbour to the 'hot' particle. Here the fractional error is defined asˆPasˆ asˆP (t) − ˆ P single-dt / ˆ P single-dt . The orange line showing the drifting using equation (35) shows that the pressure rapidly drops to zero after around four steps. The red dotted line (equation 36) shows the offset in pressure that is maintained even after the central 'hot' particle cools.
Inconsistencies arising from the coupling of galaxy formation sub-grid models to pressure-smoothed particle hydrodynamics

June 2021

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49 Reads

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16 Citations

Monthly Notices of the Royal Astronomical Society

Smoothed particle hydrodynamics (SPH) is a Lagrangian method for solving the fluid equations that is commonplace in astrophysics, prized for its natural adaptivity and stability. The choice of variable to smooth in SPH has been the topic of contention, with smoothed pressure (P-SPH) being introduced to reduce errors at contact discontinuities relative to smoothed density schemes. Smoothed pressure schemes produce excellent results in isolated hydrodynamics tests; in more complex situations however, especially when coupling to the ‘sub-grid’ physics and multiple time-stepping used in many state-of-the-art astrophysics simulations, these schemes produce large force errors that can easily evade detection as they do not manifest as energy non-conservation. Here, two scenarios are evaluated: the injection of energy into the fluid (common for stellar feedback) and radiative cooling. In the former scenario, force and energy conservation errors manifest (of the same order as the injected energy), and in the latter large force errors that change rapidly over a few time-steps lead to instability in the fluid (of the same order as the energy lost to cooling). Potential ways to remedy these issues are explored with solutions generally leading to large increases in computational cost. Schemes using a density-based formulation do not create these instabilities and as such it is recommended that they are preferred over pressure-based solutions when combined with an energy diffusion term to reduce errors at contact discontinuities.


SIGAME v3: Gas Fragmentation in Post-processing of Cosmological Simulations for More Accurate Infrared Line Emission Modeling

February 2021

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66 Reads

We present an update to the framework called SImulator of GAlaxy Millimeter/submillimeter Emission (S\'IGAME). S\'IGAME derives line emission in the far-infrared (FIR) for galaxies in particle-based cosmological hydrodynamics simulations by applying radiative transfer and physics recipes via a post-processing step after completion of the simulation. In this version, a new technique is developed to model higher gas densities by parametrizing the gas density probability distribution function (PDF) in higher resolution simulations for use as a look-up table, allowing for more adaptive PDFs than in previous work. S\'IGAME v3 is tested on redshift z = 0 galaxies drawn from the SIMBA cosmological simulation for eight FIR emission lines tracing vastly different interstellar medium phases. Including dust radiative transfer with SKIRT and high resolution photo-ionization models with Cloudy, this new method is able to self-consistently reproduce observed relations between line luminosity and star formation rate in all cases, except for [NII]122, [NII]205 and [OI]63, the luminosities of which are overestimated by median factors of 1.6, 1.2 and 1.2 dex, respectively. We attribute the remaining disagreement with observations to the lack of precise attenuation of the interstellar light on subgrid scales (<200 pc).


Sphenix: Smoothed Particle Hydrodynamics for the next generation of galaxy formation simulations

December 2020

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21 Reads

Smoothed Particle Hydrodynamics (SPH) is a ubiquitous numerical method for solving the fluid equations, and is prized for its conservation properties, natural adaptivity, and simplicity. We introduce the Sphenix SPH scheme, which was designed with three key goals in mind: to work well with sub-grid physics modules that inject energy, be highly computationally efficient (both in terms of compute and memory), and to be Lagrangian. Sphenix uses a Density-Energy equation of motion, along with variable artificial viscosity and conduction, including limiters designed to work with common sub-grid models of galaxy formation. In particular, we present and test a novel limiter that prevents conduction across shocks, preventing spurious radiative losses in feedback events. Sphenix is shown to solve many difficult test problems for traditional SPH, including fluid mixing and vorticity conservation, and it is shown to produce convergent behaviour in all tests where this is appropriate. Crucially, we use the same parameters within Sphenix for the various switches throughout, to demonstrate the performance of the scheme as it would be used in production simulations.


Citations (38)


... If inside-out growth has occurred, where star formation begins at the centre of a galaxy and over time moves outwards, we expect an older population of stars in the centre of that galaxy and a young population of stars on the outskirts (e.g., Muñoz-Mateos et al. 2007;Pezzulli et al. 2015;Lian et al. 2017;Frankel et al. 2019;Lyu et al. 2025). This would produce a more extended light profile in shorter wavelengths than longer wavelengths; hence, the rest-optical size will be larger than the rest-NIR size, and R F150W /R F444W > 1. If, however, a galaxy underwent a central starburst, the centre of that galaxy would be populated with young stars, and the outskirts would have older stars, which could potentially be caused by mergers (e.g., Tacchella et al. 2016a;McClymont et al. 2025b). This would lead to the light profile being more extended in the longer wavelengths than the shorter wavelengths, and the size in the rest-optical will be more compact than the size in the rest-NIR, therefore R F150W /R F444W < 1. ...

Reference:

Big, Dusty Galaxies in Blue Jay: Insights into the Relationship Between Morphology and Dust Attenuation at Cosmic Noon
The THESAN-ZOOM project: central starbursts and inside-out quenching govern galaxy sizes in the early Universe

... The stellar mass and SFR are, however, not independent quantities, with a plethora of works studying the observed relationship between the SFR and stellar mass, or the star-forming main sequence (e.g., Brinchmann et al. 2004;Nelson et al. 2016b;Lin et al. 2019;Nelson et al. 2021;Leja et al. 2022;Alsing et al. 2024;McClymont et al. 2025a). Therefore, cross-correlations may elevate the correlation between the dust attenuation and the stellar mass or SFR. ...

The THESAN-ZOOM project: Burst, quench, repeat -- unveiling the evolution of high-redshift galaxies along the star-forming main sequence

... This will enabled rapid copying of the data via the Librarian to NERSC. For more details on the Librarian see Borrow et al. 2024. 19 We deploy several separate JupyterHub installations, split across three KVM guests running on two servers, to enable user interactive data exploration. ...

Making Research Data Flow With Python
  • Citing Conference Paper
  • July 2024

... The Thesan simulation suite (Kannan et al. 2021;Garaldi et al. 2022;Smith et al. 2022) is based on the widely used IllustrisTNG simulations (Nelson et al. 2017(Nelson et al. , 2019Pillepich et al. 2017;Springel et al. 2017;Marinacci et al. 2018;Naiman et al. 2018); however, Thesan runs Arepo-RT (Kannan et al. 2019): a modified version of IllustrisTNG's magnetohydrodynamical model Arepo (Weinberger et al. 2020), differing primarily in the implementation of radiative hydrodynamics, aimed at modelling the interactions of radiation with gas cells, thereby advocating the direct computation of phenomena such as radiative feedback from young stars and active galactic nuclei (AGN). At Thesan's final redshift of z = 5.5, approximately 1.04 gigayears after the Big Bang, we find a sample of nine central galaxies with a stellar mass above 10 10 M ⊙ and instantaneous specific star formation rate below 1Gyr −1 ; four of which have maintained this low star formation for the past 100 Myr, have grown their stellar mass in close relation to their AGN growth, and exhibit a stellar half-mass radius below 4 comoving kiloparsecs (ckpc) at the final snapshot (Shen et al. 2024b); similar to the five massive galaxies found to be quenched at this time in Carnall et al. (2024). We show a summary of the key properties of these galaxies in table 1. ...

The thesan project: galaxy sizes during the epoch of reionization
  • Citing Article
  • September 2024

Monthly Notices of the Royal Astronomical Society

... Despite the general enhancement of SMBH synthesis resulting from this inhomogeneous and self-consistent radiation background, the tight concentration of ionising sources in the environments of MQGs contribute significantly to galaxy-black hole coevolution. Conaboy et al. (2025) show that the most massive haloes and dense environments in the Sherwood-Relics simulations harbour the strongest Lyα transmission during reionisation, while Neyer et al. (2024) show in Thesan that ionised bubbles preferentially form in overdense regions of space, which in Flares preferentially host the largest AGN (Wilkins et al. 2025); potentially allowing galaxies within these large ionised structures to remain exposed to elevated radiation pressure for extended periods of time. These findings support a picture in which early-forming, overdense environments not only facilitate the rapid assembly of massive galaxies, but also modulate the thermodynamic conditions under which quenching unfolds. ...

The thesan project: Connecting ionized bubble sizes to their local environments during the Epoch of Reionization
  • Citing Article
  • May 2024

Monthly Notices of the Royal Astronomical Society

... However, given that the average variation on the stellar mass estimates is only about 0.02 dex, we chose to retain 30 kpc as our baseline.9 We have also computed a light-weighted velocity dispersion, using the ratio of the particle luminosity over the total luminosity as weight, obtaining the same distribution of [ ★, ] , consistently with the recent findings fromSohn et al. (2024), hence we decided to keep the simple Eq.(19). ...

Velocity Dispersions of Quiescent Galaxies in IllustrisTNG

The Astrophysical Journal

... In this section, we first outline the setup, initial conditions, and input parameters for our model SPH planets and impact simulations. All SPH impact simulations were run with the SWIFT (version 0.9.0) hydrodynamics and gravity code (Schaller et al. 2016;Kegerreis et al. 2019;Schaller et al. 2023) using the subtask speedup branch (Schaller et al. 2024). The version of the code used is archived on Zenodo. ...

Swift : A modern highly-parallel gravity and smoothed particle hydrodynamics solver for astrophysical and cosmological applications
  • Citing Article
  • March 2024

Monthly Notices of the Royal Astronomical Society

... It also employs a subcycling algorithm, in which radiative transfer is resampled multiple times within each hydrodynamical timestep. This allows efficient tracking of multiple photon energy bins coupled to gas hydrodynamics in real time, allowing ionisation fronts to form dynamically and interact with the local environment (Garaldi et al. , 2024Shen et al. 2024b). Coupled with non-equilibrium thermochemistry, the self-consistent modelling of reionisation and galaxy formation in Thesan influences gas heating, cooling, and ionisation; ultimately allowing for a more detailed picture of star formation, particularly in low-mass haloes and at high redshifts Zier et al. 2025). ...

The thesan project: public data release of radiation-hydrodynamic simulations matching reionization-era JWST observations
  • Citing Article
  • March 2024

Monthly Notices of the Royal Astronomical Society