A stellar bar hidden in an extreme gas-rich disk galaxy at z=4.055
Pith reviewed 2026-05-19 15:51 UTC · model grok-4.3
The pith
A stellar bar has formed in a gas-rich disk galaxy at z=4.055, showing bars can develop rapidly despite high gas content.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The detection of a stellar bar in GN20 demonstrates that gas-rich disks do support rapid stellar bar formation in the early Universe.
What carries the argument
The stellar bar identified in GN20 via JWST imaging of the stellar light distribution, supported by baryon and gas mass fractions measured from combined stellar, gas, and dust observations.
If this is right
- Gas-rich disks at high redshift can form stellar bars on short timescales.
- Bars may provide an early mechanism for redistributing angular momentum and driving gas inflows.
- This process could contribute to rapid galaxy assembly and quenching within the first 1.5 billion years.
Where Pith is reading between the lines
- Models of early galaxy evolution may need to allow bar instabilities to grow even when gas dominates the baryonic mass.
- The same mechanism could explain other JWST detections of early bars in apparently gas-rich systems.
- Bars in gas-rich disks might accelerate the conversion of gas into stars and thereby hasten quenching.
Load-bearing premise
The central structure is correctly identified as a stellar bar and the reported baryon and gas mass fractions are accurate.
What would settle it
Kinematic maps or higher-resolution imaging that show the central feature is not a rotating bar, or revised mass measurements that place the gas fraction well below 50 percent, would falsify the central claim.
Figures
read the original abstract
The classical picture for the formation of stellar bars -- key dynamical drivers of the evolution of galaxies -- is through secular evolution of instability in gas poor, stellar-dominated disks. The detection with the James Webb Space Telescope (JWST) of stellar bars and spiral arms in galaxies at early cosmic times has thus challenged LambdaCDM-based expectations, which recent studies reconcile by suggesting that these galaxies are baryon-dominated and have already consumed most of their gas. Yet, a paradox arises, as early galaxies are expected to be increasingly rich in gas, which is generally considered to prevent or slow down stellar bar formation. Here, we show the detection of a stellar bar in GN20, a gas-rich star-forming disk galaxy at a redshift of z=4.055, only 1.5 billion years after the Big Bang. Simultaneous observations of the stars, gas, and dust reveal that GN20 is indeed baryon-dominated (over dark matter; 70+/-30%), but the baryonic mass is largely in the form of gas (75+/-25%). This discovery demonstrates that gas-rich disks do support rapid stellar bar formation in the early Universe, motivating a new theoretical perspective on bar formation in gas-rich systems, and providing a potential new mechanism for very early galaxy assembly and quenching.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports the detection of a stellar bar in the gas-rich star-forming disk galaxy GN20 at z=4.055 using JWST NIRCam imaging, combined with simultaneous constraints on stars, gas, and dust. It claims the galaxy is baryon-dominated (70±30% over dark matter) with baryonic mass largely gaseous (75±25%), demonstrating that extreme gas-rich conditions do not prevent rapid stellar bar formation in the early Universe and motivating revised theoretical models.
Significance. If the bar identification and mass fractions hold, the result would be significant for galaxy evolution studies: it provides direct observational evidence that stellar bars can form rapidly in gas-dominated systems at z>4, challenging the classical secular-evolution picture and existing simulation expectations that high gas fractions suppress bars. The use of joint stellar-gas-dust fitting from JWST data is a strength that enables the extreme gas-fraction claim.
major comments (2)
- [§3] §3 (Bar detection and morphology): The identification of the central elongated feature as a stellar bar formed by disk instability lacks explicit quantitative criteria (e.g., ellipse-fit ellipticity thresholds, Fourier m=2 amplitude, or comparison to mock images), and no kinematic confirmation such as non-circular velocity fields or orbit modeling is reported; given the clumpy high-z morphology, this leaves open the possibility that the structure is a transient clump or interaction remnant rather than a stable bar.
- [§4] §4 (Mass fraction derivation): The reported baryon dominance (70±30%) and gas fraction within baryons (75±25%) are derived from simultaneous fitting, but the error budget, degeneracy handling between stellar, gas, and dust components, and sensitivity to assumptions (e.g., IMF or dust model) are not detailed; the large uncertainties mean the gas fraction could plausibly be ~50%, which would reduce tension with models expecting bars to form more readily below ~60-70% gas and weaken the 'extreme gas-rich' claim.
minor comments (2)
- [Figure 2] Figure 2 caption: The scale bar and orientation relative to the disk major axis should be stated explicitly to aid visual assessment of the bar alignment.
- [Introduction] Introduction: A brief reference to the most recent (post-2023) JWST bar detections at z>2 would better contextualize the novelty relative to the cited works.
Simulated Author's Rebuttal
We thank the referee for their constructive and detailed comments, which have prompted us to strengthen the quantitative support for our claims. We address each major point below and outline the revisions we will make.
read point-by-point responses
-
Referee: §3 (Bar detection and morphology): The identification of the central elongated feature as a stellar bar formed by disk instability lacks explicit quantitative criteria (e.g., ellipse-fit ellipticity thresholds, Fourier m=2 amplitude, or comparison to mock images), and no kinematic confirmation such as non-circular velocity fields or orbit modeling is reported; given the clumpy high-z morphology, this leaves open the possibility that the structure is a transient clump or interaction remnant rather than a stable bar.
Authors: We agree that the original manuscript would benefit from more explicit quantitative criteria for the bar identification. In the revised version we will add ellipse-fitting results that show the radial ellipticity profile and position-angle behavior expected for a bar, together with a Fourier m=2 amplitude measurement. We will also include a direct comparison of the observed morphology to mock NIRCam images generated from hydrodynamic simulations of gas-rich, high-redshift disks that contain stable bars. These additions will help distinguish the feature from a transient clump. Kinematic confirmation via non-circular motions or orbit modeling is not possible with the available broadband imaging data; we will explicitly note this limitation while emphasizing that the morphological signatures, combined with the previously reported rotating molecular-gas disk, remain consistent with a bar. revision: partial
-
Referee: §4 (Mass fraction derivation): The reported baryon dominance (70±30%) and gas fraction within baryons (75±25%) are derived from simultaneous fitting, but the error budget, degeneracy handling between stellar, gas, and dust components, and sensitivity to assumptions (e.g., IMF or dust model) are not detailed; the large uncertainties mean the gas fraction could plausibly be ~50%, which would reduce tension with models expecting bars to form more readily below ~60-70% gas and weaken the 'extreme gas-rich' claim.
Authors: We acknowledge that the error budget and degeneracy analysis were insufficiently detailed. In the revision we will expand the methods section to describe the joint fitting procedure, the treatment of degeneracies between stellar, gas and dust components, and the results of sensitivity tests to IMF choice and dust models. These tests indicate that the gas fraction remains above ~60% for the majority of plausible parameter combinations, although the large uncertainties are real. We will present the full posterior distributions and will moderate the wording around 'extreme gas-rich' to reflect the range of allowed values while retaining the central conclusion that the system is still gas-dominated enough to challenge existing bar-formation expectations. revision: yes
- Kinematic confirmation of the bar (non-circular velocity fields or orbit modeling) cannot be provided because the observations consist solely of broadband NIRCam imaging; no integral-field spectroscopy is available for GN20.
Circularity Check
No significant circularity in observational detection report
full rationale
The paper is an observational report of a JWST-detected stellar bar in GN20 at z=4.055, with baryon and gas mass fractions presented as direct measurements from simultaneous stellar-gas-dust fitting (70+/-30% baryon-dominated, 75+/-25% gas). No derivation chain, equations, or predictions are described that reduce by construction to fitted inputs, self-definitions, or self-citation load-bearing steps. The central claim follows from external imaging and mass estimation data without internal circular reduction, making this a standard non-circular observational finding.
Axiom & Free-Parameter Ledger
free parameters (2)
- baryon dominance fraction =
70+/-30%
- gas fraction of baryons =
75+/-25%
axioms (2)
- domain assumption Stellar bars form via secular evolution in gas-poor stellar-dominated disks
- domain assumption The central structure detected by JWST is a stellar bar
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/BranchSelection.leanbranch_selection unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
f_baryon=0.7±0.3, f_gas=0.75±0.25 from M_dyn, M_star, M_mol
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
- [1]
-
[2]
Amvrosiadis, A., Lange, S., Nightingale, J. W., et al. 2025, MNRAS, 537, 1163, doi: 10.1093/mnras/staf048
-
[3]
Aravena, M., Heintz, K., Dessauges-Zavadsky, M., et al. 2024, A&A, 682, A24, doi: 10.1051/0004-6361/202347281
-
[4]
and Labiano, Alvaro and Álvarez-Márquez, Javier and Patapis, Polychronis and Kavanagh, Patrick J
Argyriou, I., Glasse, A., Law, D. R., et al. 2023, A&A, 675, A111, doi: 10.1051/0004-6361/202346489
-
[5]
Athanassoula, E., Machado, R. E. G., & Rodionov, S. A. 2013, MNRAS, 429, 1949, doi: 10.1093/mnras/sts452
-
[6]
Athanassoula, E., & Misiriotis, A. 2002, MNRAS, 330, 35, doi: 10.1046/j.1365-8711.2002.05028.x
-
[7]
Barro, G., Faber, S. M., Koo, D. C., et al. 2017, ApJ, 840, 47, doi: 10.3847/1538-4357/aa6b05
-
[8]
Battisti, A. J., Cunha, E. d., Shivaei, I., & Calzetti, D. 2020, ApJ, 888, 108, doi: 10.3847/1538-4357/ab5fdd
-
[9]
2017, A&A, 597, A85, doi: 10.1051/0004-6361/201526749
Leroy, A. 2017, A&A, 597, A85, doi: 10.1051/0004-6361/201526749
-
[10]
2024, A&A, 686, A3, doi: 10.1051/0004-6361/202348845
Bik, A., ´Alvarez-M´ arquez, J., Colina, L., et al. 2024, A&A, 686, A3, doi: 10.1051/0004-6361/202348845
-
[11]
2008, Galactic Dynamics: Second Edition
Binney, J., & Tremaine, S. 2008, Galactic Dynamics: Second Edition
work page 2008
-
[12]
2024, ApJ, 968, 86, doi: 10.3847/1538-4357/ad4118
Federrath, C. 2024, ApJ, 968, 86, doi: 10.3847/1538-4357/ad4118
-
[13]
2023, ApJ, 947, 80, doi: 10.3847/1538-4357/acc469
Freeman, K. 2023, ApJ, 947, 80, doi: 10.3847/1538-4357/acc469
-
[14]
Bland-Hawthorn, J., Tepper-Garcia, T., Agertz, O., et al. 2025, ApJ, 994, 22, doi: 10.3847/1538-4357/ae0931
-
[15]
Blitz, L., & Spergel, D. N. 1991, ApJ, 379, 631, doi: 10.1086/170535 B¨ oker, T., Arribas, S., L¨ utzgendorf, N., et al. 2022, A&A, 661, A82, doi: 10.1051/0004-6361/202142589
-
[16]
A., Decarli, R., Walter, F., et al
Boogaard, L. A., Decarli, R., Walter, F., et al. 2023, ApJ, 945, 111, doi: 10.3847/1538-4357/acb4f0
-
[17]
A., Walter, F., Weiß, A., et al
Boogaard, L. A., Walter, F., Weiß, A., et al. 2026, ApJ, 996, 19, doi: 10.3847/1538-4357/ae14eb
-
[18]
2015, PASP, 127, 612, doi: 10.1086/682254
Bouchet, P., Garc´ ıa-Mar´ ın, M., Lagage, P.-O., et al. 2015, PASP, 127, 612, doi: 10.1086/682254
-
[19]
Bournaud, F., Combes, F., & Semelin, B. 2005, MNRAS, 364, L18, doi: 10.1111/j.1745-3933.2005.00096.x
-
[20]
2020, astropy/photutils: 1.0.0, 1.0.0 Zenodo, doi: 10.5281/zenodo.4044744
Bradley, L., Sip˝ ocz, B., Robitaille, T., et al. 2020, astropy/photutils: 1.0.0, 1.0.0 Zenodo, doi: 10.5281/zenodo.4044744
-
[21]
2003, MNRAS, 344, 1000, doi: 10.1046/j.1365-8711.2003.06897.x
Bruzual, G., & Charlot, S. 2003, MNRAS, 344, 1000, doi: 10.1046/j.1365-8711.2003.06897.x
-
[22]
2023, JWST Calibration Pipeline, 1.13.1 Zenodo, doi: 10.5281/zenodo.10407298
Bushouse, H., Eisenhamer, J., Dencheva, N., et al. 2023, JWST Calibration Pipeline, 1.13.1 Zenodo, doi: 10.5281/zenodo.10407298
-
[23]
Buttitta, C., Corsini, E. M., Cuomo, V., et al. 2022, A&A, 664, L10, doi: 10.1051/0004-6361/202244297
-
[24]
Calzetti, D., Armus, L., Bohlin, R. C., et al. 2000, ApJ, 533, 682, doi: 10.1086/308692
work page internal anchor Pith review doi:10.1086/308692 2000
-
[25]
L., Hodge, J., Walter, F., et al
Carilli, C. L., Hodge, J., Walter, F., et al. 2011, ApJL, 739, L33, doi: 10.1088/2041-8205/739/1/L33
-
[26]
L., Daddi, E., Riechers, D., et al
Carilli, C. L., Daddi, E., Riechers, D., et al. 2010, ApJ, 714, 1407, doi: 10.1088/0004-637X/714/2/1407
-
[27]
Carnall, A. C., McLure, R. J., Dunlop, J. S., et al. 2023, Nature, 619, 716, doi: 10.1038/s41586-023-06158-6
-
[28]
Galactic Stellar and Substellar Initial Mass Function
Chabrier, G. 2003, PASP, 115, 763, doi: 10.1086/376392
work page internal anchor Pith review doi:10.1086/376392 2003
-
[29]
2017, ApJS, 233, 19, doi: 10.3847/1538-4365/aa97da
Chang, Y.-Y., Le Floc’h, E., Juneau, S., et al. 2017, ApJS, 233, 19, doi: 10.3847/1538-4365/aa97da
-
[30]
Charlot, S., & Fall, S. M. 2000, ApJ, 539, 718, doi: 10.1086/309250
work page internal anchor Pith review doi:10.1086/309250 2000
-
[31]
2023, A&A, 673, L6, doi: 10.1051/0004-6361/202346535
Colina, L., Crespo G´ omez, A.,´Alvarez-M´ arquez, J., et al. 2023, A&A, 673, L6, doi: 10.1051/0004-6361/202346535
-
[32]
2013, A&A, 558, A124, doi: 10.1051/0004-6361/201322288
Combes, F., Garc´ ıa-Burillo, S., Casasola, V., et al. 2013, A&A, 558, A124, doi: 10.1051/0004-6361/201322288
-
[33]
Costantin, L., P´ erez-Gonz´ alez, P. G., M´ endez-Abreu, J., et al. 2021, ApJ, 913, 125, doi: 10.3847/1538-4357/abef72
-
[34]
Costantin, L., P´ erez-Gonz´ alez, P. G., Guo, Y., et al. 2023, Nature, 623, 499, doi: 10.1038/s41586-023-06636-x 16
-
[35]
Costantin, L., Gillman, S., Boogaard, L. A., et al. 2025, A&A, 699, A360, doi: 10.1051/0004-6361/202451330 Crespo G´ omez, A., Colina, L.,´Alvarez-M´ arquez, J., et al. 2024, A&A, 691, A325, doi: 10.1051/0004-6361/202449750 da Cunha, E., Charlot, S., & Elbaz, D. 2008, MNRAS, 388, 1595, doi: 10.1111/j.1365-2966.2008.13535.x da Cunha, E., Walter, F., Smail,...
-
[36]
2009, ApJ, 694, 1517, doi: 10.1088/0004-637X/694/2/1517 de Graaff, A., Setton, D
Daddi, E., Dannerbauer, H., Stern, D., et al. 2009, ApJ, 694, 1517, doi: 10.1088/0004-637X/694/2/1517 de Graaff, A., Setton, D. J., Brammer, G., et al. 2025, Nature Astronomy, 9, 280, doi: 10.1038/s41550-024-02424-3 de Vaucouleurs, G. 1964, in IAU Symposium, Vol. 20, The Galaxy and the Magellanic Clouds, ed. F. J. Kerr, 195
-
[37]
Debattista, V. P., Corsini, E. M., & Aguerri, J. A. L. 2002, MNRAS, 332, 65, doi: 10.1046/j.1365-8711.2002.05269.x
-
[38]
Debattista, V. P., Mayer, L., Carollo, C. M., et al. 2006, ApJ, 645, 209, doi: 10.1086/504147
-
[39]
2016, ApJ, 833, 69, doi: 10.3847/1538-4357/833/1/69
Decarli, R., Walter, F., Aravena, M., et al. 2016, ApJ, 833, 69, doi: 10.3847/1538-4357/833/1/69
-
[40]
2019, ApJ, 882, 138, doi: 10.3847/1538-4357/ab30fe
Decarli, R., Walter, F., G´ onzalez-L´ opez, J., et al. 2019, ApJ, 882, 138, doi: 10.3847/1538-4357/ab30fe
-
[41]
2023, MNRAS, 518, 2712, doi: 10.1093/mnras/stac3184 Dudzeviˇ ci¯ ut˙ e, U., Smail, I., Swinbank, A
Dehnen, W., Semczuk, M., & Sch¨ onrich, R. 2023, MNRAS, 518, 2712, doi: 10.1093/mnras/stac3184 Dudzeviˇ ci¯ ut˙ e, U., Smail, I., Swinbank, A. M., et al. 2020, MNRAS, 494, 3828, doi: 10.1093/mnras/staa769
-
[42]
2006, MNRAS, 366, 575, doi: 10.1111/j.1365-2966.2005.09884.x
Erwin, P. 2005, MNRAS, 364, 283, doi: 10.1111/j.1365-2966.2005.09560.x
-
[43]
Eskridge, P. B., Frogel, J. A., Pogge, R. W., et al. 2000, AJ, 119, 536, doi: 10.1086/301203
-
[44]
Ferreira, L., Adams, N., Conselice, C. J., et al. 2022, ApJL, 938, L2, doi: 10.3847/2041-8213/ac947c
-
[45]
Fragkoudi, F., Grand, R. J. J., Pakmor, R., et al. 2025, MNRAS, 538, 1587, doi: 10.1093/mnras/staf389
-
[46]
Fritz, J., Franceschini, A., & Hatziminaoglou, E. 2006, MNRAS, 366, 767, doi: 10.1111/j.1365-2966.2006.09866.x
-
[47]
S., B´ edorf, J., Baba, J., & Portegies Zwart, S
Fujii, M. S., B´ edorf, J., Baba, J., & Portegies Zwart, S. 2018, MNRAS, 477, 1451
work page 2018
-
[48]
Gardner, J. P., Mather, J. C., Abbott, R., et al. 2023, PASP, 135, 068001, doi: 10.1088/1538-3873/acd1b5 G´ eron, T., Smethurst, R. J., Dickinson, H., et al. 2025, ApJ, 987, 74, doi: 10.3847/1538-4357/add7d0
-
[49]
Guo, Y., Jogee, S., Finkelstein, S. L., et al. 2023, ApJL, 945, L10, doi: 10.3847/2041-8213/acacfb
-
[50]
2025, ApJ, 985, 181, doi: 10.3847/1538-4357/adc8a7
Guo, Y., Jogee, S., Wise, E., et al. 2025, ApJ, 985, 181, doi: 10.3847/1538-4357/adc8a7
-
[51]
Hodge, J. A., Carilli, C. L., Walter, F., et al. 2012, ApJ, 760, 11, doi: 10.1088/0004-637X/760/1/11
-
[52]
A., Riechers, D., Decarli, R., et al
Hodge, J. A., Riechers, D., Decarli, R., et al. 2015, ApJL, 798, L18, doi: 10.1088/2041-8205/798/1/L18
-
[53]
A., Smail, I., Walter, F., et al
Hodge, J. A., Smail, I., Walter, F., et al. 2019, ApJ, 876, 130, doi: 10.3847/1538-4357/ab1846
-
[54]
2025, Nature, 641, 861, doi: 10.1038/s41586-025-08914-2
Huang, S., Kawabe, R., Umehata, H., et al. 2025, Nature, 641, 861, doi: 10.1038/s41586-025-08914-2
-
[55]
Huertas-Company, M., Iyer, K. G., Angeloudi, E., et al. 2024, A&A, 685, A48, doi: 10.1051/0004-6361/202346800
-
[56]
Inoue, A. K. 2011, MNRAS, 415, 2920, doi: 10.1111/j.1365-2966.2011.18906.x
-
[57]
Jakobsen, P., Ferruit, P., Alves de Oliveira, C., et al. 2022, A&A, 661, A80, doi: 10.1051/0004-6361/202142663
work page internal anchor Pith review doi:10.1051/0004-6361/202142663 2022
-
[58]
Jedrzejewski, R. I. 1987, MNRAS, 226, 747, doi: 10.1093/mnras/226.4.747
-
[59]
Jogee, S., Barazza, F. D., Rix, H.-W., et al. 2004, ApJL, 615, L105, doi: 10.1086/426138
-
[60]
Johnson, H. M. 1957, AJ, 62, 19, doi: 10.1086/107441
-
[61]
Kalita, B. S., Ho, L. C., Silverman, J. D., et al. 2025, arXiv e-prints, arXiv:2512.04163, doi: 10.48550/arXiv.2512.04163
-
[62]
Kormendy, J., & Kennicutt, Jr., R. C. 2004, ARA&A, 42, 603, doi: 10.1146/annurev.astro.42.053102.134024
-
[63]
2012, ApJ, 757, 60, doi: 10.1088/0004-637X/757/1/60 Le Conte, Z
Kraljic, K., Bournaud, F., & Martig, M. 2012, ApJ, 757, 60, doi: 10.1088/0004-637X/757/1/60 Le Conte, Z. A., Gadotti, D. A., Ferreira, L., et al. 2025, MNRAS, doi: 10.1093/mnras/staf2010
-
[64]
Lelli, F., Di Teodoro, E. M., Fraternali, F., et al. 2021, Science, 371, 713, doi: 10.1126/science.abc1893
-
[65]
2024, ApJ, 976, 70, doi: 10.3847/1538-4357/ad7fee
Li, J., Da Cunha, E., Gonz´ alez-L´ opez, J., et al. 2024, ApJ, 976, 70, doi: 10.3847/1538-4357/ad7fee
-
[66]
2007, ApJ, 659, 1176, doi: 10.1086/512355
Marinova, I., & Jogee, S. 2007, ApJ, 659, 1176, doi: 10.1086/512355
-
[67]
Martinez-Valpuesta, I., Shlosman, I., & Heller, C. 2006, ApJ, 637, 214, doi: 10.1086/498338 Men´ endez-Delmestre, K., Sheth, K., Schinnerer, E., Jarrett, T. H., & Scoville, N. Z. 2007, ApJ, 657, 790, doi: 10.1086/511025
-
[68]
X., Kanekar, N., & Rafelski, M
Neeleman, M., Prochaska, J. X., Kanekar, N., & Rafelski, M. 2020, Nature, 581, 269, doi: 10.1038/s41586-020-2276-y
-
[69]
1990, ApJ, 357, 71, doi: 10.1086/168892
Ohta, K., Hamabe, M., & Wakamatsu, K.-I. 1990, ApJ, 357, 71, doi: 10.1086/168892
-
[70]
Pacifici, C., Iyer, K. G., Mobasher, B., et al. 2023, ApJ, 944, 141, doi: 10.3847/1538-4357/acacff
-
[71]
Padilla, N. D., & Strauss, M. A. 2008, MNRAS, 388, 1321, doi: 10.1111/j.1365-2966.2008.13480.x
-
[72]
Pastras, S., Genzel, R., Tacconi, L. J., et al. 2025, A&A, 704, A329, doi: 10.1051/0004-6361/202555430 17
-
[73]
Pontzen, A., Roˇ skar, R., Stinson, G., & Woods, R. 2013, pynbody: N-Body/SPH analysis for python,, Astrophysics Source Code Library, record ascl:1305.002 http://ascl.net/1305.002
work page 2013
-
[74]
2006, MNRAS, 366, 575, doi: 10.1111/j.1365-2966.2005.09884.x
Pope, A., Borys, C., Scott, D., et al. 2005, MNRAS, 358, 149, doi: 10.1111/j.1365-2966.2005.08759.x
-
[75]
Pope, A., Scott, D., Dickinson, M., et al. 2006, MNRAS, 370, 1185, doi: 10.1111/j.1365-2966.2006.10575.x
-
[76]
Raha, N., Sellwood, J. A., James, R. A., & Kahn, F. D. 1991, Nature, 352, 411, doi: 10.1038/352411a0
-
[77]
Reddish, J., Kraljic, K., Petersen, M. S., et al. 2022, MNRAS, 512, 160, doi: 10.1093/mnras/stac494
-
[78]
A., Pope, A., Daddi, E., et al
Riechers, D. A., Pope, A., Daddi, E., et al. 2014, ApJ, 786, 31, doi: 10.1088/0004-637X/786/1/31
-
[79]
Riechers, D. A., Pavesi, R., Sharon, C. E., et al. 2019, ApJ, 872, 7, doi: 10.3847/1538-4357/aafc27
-
[80]
o ker , J. Bouwman , L. Colina , A. Glasse , K. D. Gordon , T. P. Greene , M. G \
Rieke, G. H., Wright, G. S., B¨ oker, T., et al. 2015, PASP, 127, 584, doi: 10.1086/682252
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.