REVIEW 3 major objections 5 minor 4 cited by
Predictions for the Detectability of Milky Way Satellite Galaxies and Outer-Halo Star Clusters with the Vera C. Rubin Observatory
T0 review · 3 major / 5 minor · reviewed 2026-08-16 · deepseek-v4-flash
Pith's one-line read The paper calculates that Rubin's LSST should detect 89 ± 20 Milky Way satellite galaxies, falling to 67–83 with realistic star/galaxy separation, and that faint compact systems are recovered with >50% efficiency out to ~250 kpc.
desk verdict A careful, useful LSST satellite forecast whose headline 89±20 is not broken, but the quoted uncertainty omits the one systematic that could move it most: the search is run at each satellite's true distance modulus rather than over a blind grid. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The machinery has three linked pieces. First, catalog-level injection: each artificial satellite is a Plummer-profile stellar population with a Chabrier initial mass function and Marigo isochrones, assigned detection, classification, and photometric-uncertainty properties from the DC2 catalog so it can be merged directly into the data. Second, the search: a matched-filter code (called 'simple' in the paper) that applies an isochrone color-magnitude selection, smooths the filtered density field, and outputs a Poisson detection significance SIG, whose 50% efficiency contour is parameterized by $\log_{10} r_{1/2} = A_0(D)/(M_V - M_{V,0}(D)) + \log_{10} r_{1/2,0}(D)$ at fixed $D$; a gradient-boosted decision tree trained on the $10^5$ outcomes captures the full efficiency surface. Third, population prediction: the resulting selection function is multiplied against the galaxy-halo connection model, applied to the masked ~18,300 deg2 wide-fast-deep footprint with extinction and bright-star masks, to produce the predicted luminosity function and the $89 \pm 20$ count.
What would settle it
Run the same matched-filter search on real early LSST wide-fast-deep images after injecting artificial satellites with known distance, size, and luminosity, and compare the recovered fraction with the 50% efficiency contour published here; in parallel, measure the actual star/galaxy classification efficiency near $r \sim 26$ mag using objects with independent morphological or proper-motion classifications and check whether it matches the DC2-derived curve that sets the predicted count.
Extended reading notes
Core claim
The central discovery is a quantitative observational selection function for resolved Milky Way satellites: the probability of detection as a function of heliocentric distance $D$, absolute magnitude $M_V$, and half-light radius $r_{1/2}$, derived by injecting $10^5$ artificial satellites into DC2 and processing them with the isochrone matched-filter search. The headline finding is that $>50\%$ detection efficiency reaches $D \sim 250$ kpc for faint compact systems ($M_V \sim 0$ mag, $r_{1/2} \sim 10$ pc) under perfect star/galaxy separation, while the measured EXTENDEDNESS classification produces a 22.4% false-positive rate at the nominal significance threshold and requires raising the threshold from SIG $>5.5$ to SIG $>8.4$ to match the perfect-classification false-positive rate. Convolving the selection function with a galaxy-halo connection model fit to current data predicts $89 \pm 20$ detectable satellites within 300 kpc in the perfect-classification case, $83 \pm 18$ with measured classification, and $67 \pm 14$ after the threshold correction—corresponding to 53, 47, or 31 new discoveries beyond the 36 satellites already known in the LSST wide-fast-deep footprint.
Load-bearing premise
The prediction stands or falls on whether the stars-versus-galaxies classification and photometric scatter measured in a roughly three-square-degree simulated patch represent how the real Rubin telescope and pipelines will treat faint objects across the entire 18,300-square-degree wide-fast-deep footprint, especially near magnitude 26 where classification efficiency drops sharply.
Editorial extensions
If this is right
- With perfect star/galaxy separation, the search should recover roughly 90% of the Milky Way's satellites with $M_V \lesssim 0$ mag, $r_{1/2} > 10$ pc, and $D < 300$ kpc that lie inside the LSST wide-fast-deep footprint.
- New detections should be fainter, more distant, and lower in surface brightness than the current census, extending satellite searches toward the galaxy-formation threshold.
- Under measured EXTENDEDNESS classification the false-positive rate is 22.4% at SIG > 5.5, which is why the realistic yield drops to $83 \pm 18$, or $67 \pm 14$ when the threshold is raised to match the perfect-classification false-positive rate.
- The analytic contour and trained machine-learning model can be used directly to compute completeness corrections for any future LSST-derived satellite sample.
Reading between the lines
- If the DC2 classification curve does not match real Rubin performance, the predicted count moves within the paper's stated 7–25% band; comparing early LSST point-source candidates against independent morphological or proper-motion classifications around $r \sim 26$ mag would settle which end of the 67–89 range is realized.
- Because the paper publishes both an analytic contour and a machine-learning selection function, future survey-strategy variants can be evaluated by reweighting the same $10^5$ injections rather than rerunning the full simulation—an exercise the authors leave implicit.
- The $89 \pm 20$ number, once real data arrive, becomes a test of the galaxy-halo connection itself: a robust count outside that range, after correcting for classification, would imply a different mapping between subhalos and luminous satellites at the faint end.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This paper uses simulated LSST data from DESC DC2 to derive a detection selection function for resolved Milky Way satellites and outer-halo star clusters. The authors inject 10^5 catalog-level stellar systems spanning log-uniform distances, masses, and sizes, run the simple isochrone matched-filter search under two star/galaxy classification scenarios (measured EXTENDEDNESS and perfect classification), characterize false positives with blank-sky null tests, and parameterize the resulting detection efficiency both analytically and with a gradient-boosted classifier. Combining this selection function with the Nadler et al. (2020) galaxy-halo model and the LSST WFD baseline footprint, they predict 89 +/- 20 detectable satellite galaxies for perfect star/galaxy separation, 83 +/- 18 for measured separation, and 67 +/- 14 after raising the threshold to equalize the false-positive rate. The main claim is that LSST will detect >50% of M_V = 0 mag, r_1/2 = 10 pc satellites out to ~250 kpc.
Significance. If the underlying simplification is valid, this is a valuable, quantitative upgrade over earlier analytic sensitivity estimates. Strengths include the large injection suite, injection at catalog level using DC2-derived photometric scatter, detection, and classification models, explicit null tests for background structure, a reproducible analysis path on the Rubin Science Platform, and the forward application of an independently fit galaxy-halo model without circular reuse of the target data. The prediction is falsifiable once LSST data accumulate, and the authors are transparent about several limitations. The central caveat is that the selection function is measured with the true distance modulus (and search region) supplied to the detector, so the headline prediction is conditional on an equivalence to a blind survey search that is asserted rather than demonstrated for DC2.
major comments (3)
- [Section 3.1 and Appendix A] The search is run at the true distance modulus of each injected satellite, and the false-positive control in Sections 3.2 and 4.1 is carried out in the same fixed-modulus configuration. A real WFD search over ~18,300 deg2 will scan a grid of distance moduli and independent sky positions, increasing the number of trials that must be held at the 2.3% false-positive rate used for the corrected scenario. The paper cites Drlica-Wagner et al. (2020) for the claim that this simplification induces trivial changes, but no test is shown for DC2; in fact, Section 4.1 demonstrates that the fixed distance modulus changes the overlap of the isochrone filter with misclassified background galaxies and produces a distance-dependent false-positive rate. Please rerun a subset of the 10^5 injections with the full distance-modulus scan (or at least several modulus offsets), compare the SIG distributions and 50% efficiency contours, compute the effective number of independent trials from blank-sky scans, and propagate the resulting threshold correction to the predicted number of detections. This is load-bearing because every efficiency contour and the headline 89 +/- 20 prediction is built on these fixed-distance significances.
- [Section 5 and Section 6] The population prediction uses a selection function that depends only on M_V, r_1/2, and D, with no dependence on foreground stellar density or sky position. DC2 is a single high-Galactic-latitude field, and the real WFD footprint spans a range of stellar densities even after the masks in Figure 7 are applied. The authors explicitly neglect this dependence in Section 5, but the magnitude of the resulting systematic is not quantified. Because the Nadler et al. (2020) model includes an LMC-associated anisotropic satellite distribution, a position-independent sensitivity can bias the 89 +/- 20 prediction in a nontrivial way. Please quantify this by injecting test satellites into regions of the footprint with different stellar densities, or by including stellar density as a feature in the machine-learning selection function and recomputing the predicted counts.
- [Abstract and Section 5] The quoted 89 +/- 20 uncertainty is sampled from the Nadler et al. (2020) posterior only; it does not include the distance-scan trial factor, the star/galaxy classification systematics, or the DC2-to-LSST transfer uncertainty. The paper itself reports the scenario spread (89, 83, 67), but the abstract headline uses 89 +/- 20, which is easily read as a total uncertainty. Please rephrase the headline so that the prediction is explicitly conditional on the simplifying assumptions, or provide a combined systematic uncertainty that includes the trial-factor and classification-model effects.
minor comments (5)
- [Abstract] Please state the parameter cuts used for the headline prediction (M_V < 0 mag, r_1/2 > 10 pc, D < 300 kpc) in the abstract itself; as written, '89 +/- 20 Milky Way satellite galaxies will be detectable' could be read as the full satellite census.
- [Section 3.1] There is a typo: 'Point-like sources are have EXTENDEDNESS = 0' should read 'Point-like sources have EXTENDEDNESS = 0'.
- [Section 5] There is a typo in the opening sentence: 'will be be observed' should be 'will be observed'. In addition, the Figure 7 caption spells 'Milk Way' and should be 'Milky Way'.
- [Section 4.1] Please state precisely how the false-positive rates 2.3% and 22.4% are defined (per blank-sky region, per fixed distance modulus, or per trial); this definition is needed to interpret the threshold correction from SIG > 5.5 to SIG > 8.4.
- [Section 4.2 and Table 2] The analytic 50% detection-efficiency contours are quoted without goodness-of-fit values or uncertainties on the fitted coefficients A0, M_V,0, and log10(r_1/2,0/pc); adding these would help users of the selection function estimate the impact of fit degeneracies.
Circularity Check
No significant circularity: the 89±20 prediction is a forward application of a DC2-measured selection function to an independently published galaxy–halo model posterior.
full rationale
The paper's derivation chain is a forward pipeline: characterize DC2 catalog detection, classification, and photometric-error efficiencies from the simulation; inject 10^5 simulated resolved stellar systems with physical parameters drawn from ranges representative of known satellites; run the simple matched-filter at each injected satellite's true distance modulus and record detection significance; fit analytic and gradient-boosted parameterizations of the resulting selection function; and convolve the Nadler et al. (2020) galaxy–halo model posterior with the selection function and an 18,300 deg2 masked WFD footprint to obtain 89±20. The population model is a published, externally fit model based on DES and Pan-STARRS1 data plus cosmological zoom-in simulations; it is not constructed from, nor fitted to, the LSST detection predictions made here. The selection function is an empirical measurement from DC2, not an input to the population model, so convolving the two is a genuine prediction rather than a rearrangement of inputs. The one salient self-citation is the claim that fixing the search distance modulus to the true value introduces only trivial changes relative to a blind scan, supported by Drlica-Wagner et al. (2020); that is an independent empirical result from DES analysis, not the present LSST result, and the paper explicitly notes the simplification and its computational motivation. All equations used for the selection-function parameterizations are fits to the injection outcomes, not definitions of the target prediction. Limitations the paper itself states, such as the high-latitude DC2 field, neglected stellar-density dependence, catalog-level rather than image-level injection, and trial factors in a real blind scan, are accuracy caveats rather than circularity. No load-bearing step reduces by construction to its own input.
Assumptions & free parameters
free parameters (3)
- Selection function coefficients A0, M_V,0, log10(r1/2,0/pc) per distance bin =
Table 2 lists values for six distance bins and three scenarios (e.g., idealized star/galaxy at 11.3 kpc: A0=22.7…
- Corrected detection threshold SIG > 8.4 =
8.4
- Magnitude cuts g < 26 and r < 26 =
26 mag
assumptions (4)
- domain assumption DC2's photometric depth, uncertainties, and EXTENDEDNESS-based star/galaxy classification are representative of the real LSST WFD survey in the unmasked footprint.
- domain assumption Catalog-level injection of resolved stellar populations adequately reproduces detectability without full image-level blending simulations.
- domain assumption Supplying the search with the true centroid and distance modulus of each injected satellite yields detection efficiencies representative of a blind scan.
- domain assumption The Nadler et al. 2020 galaxy-halo model, including its faint-end luminosity extrapolation and Kravtsov size relation, describes the Milky Way satellite population down to M_V = 0 mag.
Cite this review
Pith. "Pith review of Predictions for the Detectability of Milky Way Satellite Galaxies and Outer-Halo Star Clusters with the Vera C. Rubin Observatory." pith.science (2026). https://pith.science/paper/JQINDBCT
@misc{pith2026250416203,
author = {Pith},
title = {Pith review of: Predictions for the Detectability of Milky Way Satellite Galaxies and Outer-Halo Star Clusters with the Vera C. Rubin Observatory},
year = {2026},
howpublished = {\url{https://pith.science/paper/JQINDBCT}},
note = {Machine review of arXiv:2504.16203}
}
abstract
We predict the sensitivity of the Vera C. Rubin Observatory Legacy Survey of Space and Time (LSST) to faint, resolved Milky Way satellite galaxies and outer-halo star clusters. We characterize the expected sensitivity using simulated LSST data from the LSST Dark Energy Science Collaboration (DESC) Data Challenge 2 (DC2) accessed and analyzed with the Rubin Science Platform as part of the Rubin Early Science Program. We simulate resolved stellar populations of Milky Way satellite galaxies and outer-halo star clusters over a wide range of sizes, luminosities, and heliocentric distances, which are broadly consistent with expectations for the Milky Way satellite system. We inject simulated stars into the DC2 catalog with realistic photometric uncertainties and star/galaxy separation derived from the DC2 data itself. We assess the probability that each simulated system would be detected by LSST using a conventional isochrone matched-filter technique. We find that assuming perfect star/galaxy separation enables the detection of resolved stellar systems with $M_V$ = 0 mag and $r_{1/2}$ = 10 pc with >50% efficiency out to a heliocentric distance of ~250 kpc. Similar detection efficiency is possible with a simple star/galaxy separation criterion based on measured quantities, although the false positive rate is higher due to leakage of background galaxies into the stellar sample. When assuming perfect star/galaxy classification and a model for the galaxy-halo connection fit to current data, we predict that 89 +/- 20 Milky Way satellite galaxies will be detectable with a simple matched-filter algorithm applied to the LSST wide-fast-deep data set. Different assumptions about the performance of star/galaxy classification efficiency can decrease this estimate by ~7%-25%, which emphasizes the importance of high-quality star/galaxy separation for studies of the Milky Way satellite population with LSST.
Figures
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Forward citations
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Works this paper leans on
-
[1]
2021, ApJS, 253, 31, doi: 10.3847/1538-4365/abd62c
Abolfathi, B., Alonso, D., Armstrong, R., et al. 2021, ApJS, 253, 31, doi: 10.3847/1538-4365/abd62c
-
[2]
Ackermann, M., Albert, A., Anderson, B., et al. 2015, Phys. Rev. Lett., 115, 231301, doi: 10.1103/PhysRevLett.115.231301
-
[3]
Applebaum, E., Brooks, A. M., Christensen, C. R., et al. 2021, ApJ, 906, 96, doi: 10.3847/1538-4357/abcafa Astropy Collaboration, Robitaille, T. P., Tollerud, E. J., et al. 2013, A&A, 558, A33, doi: 10.1051/0004-6361/201322068 Astropy Collaboration, Price-Whelan, A. M., Sip˝ocz, B. M., et al. 2018, AJ, 156, 123, doi: 10.3847/1538-3881/aabc4f
-
[4]
Balbinot, E., Santiago, B. X., da Costa, L., et al. 2013, ApJ, 767, 101, doi: 10.1088/0004-637X/767/2/101
-
[5]
2015, ApJ, 807, 50, doi: 10.1088/0004-637X/807/1/50
Bechtol, K., Drlica-Wagner, A., Balbinot, E., et al. 2015, ApJ, 807, 50, doi: 10.1088/0004-637X/807/1/50
-
[6]
2025, arXiv e-prints, arXiv:2501.05739, doi: 10.48550/arXiv.2501.05739
Bechtol, K., Sevilla-Noarbe, I., Drlica-Wagner, A., et al. 2025, arXiv e-prints, arXiv:2501.05739, doi: 10.48550/arXiv.2501.05739
-
[7]
Benson, A. J., Frenk, C. S., Lacey, C. G., Baugh, C. M., & Cole, S. 2002, MNRAS, 333, 177, doi: 10.1046/j.1365-8711.2002.05388.x
arXiv 2002
-
[8]
Bica, E., Bonatto, C., Dutra, C. M., & Santos, J. F. C. 2008, MNRAS, 389, 678, doi: 10.1111/j.1365-2966.2008.13612.x
arXiv 2008
Show all 96 references
-
[9]
2018, PASJ, 70, S5, doi: 10.1093/pasj/psx080
Bosch, J., Armstrong, R., Bickerton, S., et al. 2018, PASJ, 70, S5, doi: 10.1093/pasj/psx080
2018 doi
-
[10]
R., Johnson, B
Boylan-Kolchin, M., Weisz, D. R., Johnson, B. D., et al. 2015, MNRAS, 453, 1503, doi: 10.1093/mnras/stv1736
2015 doi
-
[11]
2012, MNRAS, 427, 127, doi: 10.1111/j.1365-2966.2012.21948.x
Bressan, A., Marigo, P., Girardi, L., et al. 2012, MNRAS, 427, 127, doi: 10.1111/j.1365-2966.2012.21948.x
2012
-
[12]
O., Wechsler, R
Buch, D., Nadler, E. O., Wechsler, R. H., & Mao, Y.-Y. 2024, ApJ, 971, 79, doi: 10.3847/1538-4357/ad554c
2024 doi
-
[13]
R., & Peter, A
Buckley, M. R., & Peter, A. H. G. 2018, Phys. Rep., 761, 1, doi: 10.1016/j.physrep.2018.07.003
2018 doi
-
[14]
S., & Boylan-Kolchin, M
Bullock, J. S., & Boylan-Kolchin, M. 2017, ARA&A, 55, 343, doi: 10.1146/annurev-astro-091916-055313
2017 doi
-
[15]
M., Cautun, M., Deason, A
Callingham, T. M., Cautun, M., Deason, A. J., et al. 2019, MNRAS, 484, 5453, doi: 10.1093/mnras/stz365
2019 doi
-
[16]
J., et al
Cautun, M., Ben´ıtez-Llambay, A., Deason, A. J., et al. 2020, MNRAS, 494, 4291–4313, doi: 10.1093/mnras/staa1017
2020 doi
-
[17]
B., Drlica-Wagner, A., et al
Cerny, W., Pace, A. B., Drlica-Wagner, A., et al. 2021, ApJ, 910, 18, doi: 10.3847/1538-4357/abe1af
2021 doi
-
[18]
E., Drlica-Wagner, A., et al
Cerny, W., Mart´ınez-V´azquez, C. E., Drlica-Wagner, A., et al. 2023a, ApJ, 953, 1, doi: 10.3847/1538-4357/acdd78
-
[19]
S., et al
Cerny, W., Drlica-Wagner, A., Li, T. S., et al. 2023b, ApJ, 953, L21, doi: 10.3847/2041-8213/aced84
-
[20]
2001, ApJ, 554, 1274, doi: 10.1086/321401
Chabrier, G. 2001, ApJ, 554, 1274, doi: 10.1086/321401
2001 doi
-
[21]
Chen, T., & Guestrin, C. 2016, in Proceedings of the 22nd ACM SIGKDD International Conference on Knowledge Discovery and Data Mining, KDD ’16 (New York, NY, USA: Association for Computing Machinery), 785–794, doi: 10.1145/2939672.2939785
2016
-
[22]
G., Baugh, C
Cole, S., Lacey, C. G., Baugh, C. M., & Frenk, C. S. 2000, MNRAS, 319, 168, doi: 10.1046/j.1365-8711.2000.03879.x
2000
-
[23]
Corwin, H. G. 2004, VizieR Online Data Catalog, 7239, 0 Dal Tio, P., Pastorelli, G., Mazzi, A., et al. 2022, ApJS, 262, 22, doi: 10.3847/1538-4365/ac7be6
2004 doi
-
[24]
A., & Ng, K
Dekker, A., Ando, S., Correa, C. A., & Ng, K. C. Y. 2022, Phys. Rev. D, 106, 123026, doi: 10.1103/PhysRevD.106.123026 DES Collaboration, Abbott, T. M. C., Abdalla, F. B., et al. 2018, ApJS, 239, 18, doi: 10.3847/1538-4365/aae9f0 D’Onghia, E., & Lake, G. 2008, ApJ, 686, L61, do...
2022 doi
-
[25]
A., Peter, A
Dooley, G. A., Peter, A. H. G., Carlin, J. L., et al. 2017, MNRAS, 472, 1060, doi: 10.1093/mnras/stx2001
2017 doi
-
[26]
2020, ApJ, 893, 47, doi: 10.3847/1538-4357/ab7eb9 Detectability of Milky Way Satellites by Rubin Observatory 17
Drlica-Wagner, A., Bechtol, K., Mau, S., et al. 2020, ApJ, 893, 47, doi: 10.3847/1538-4357/ab7eb9 Detectability of Milky Way Satellites by Rubin Observatory 17
2020 doi
-
[27]
F., Pe˜narrubia, J., & Walker, M
Errani, R., Ibata, R., Navarro, J. F., Pe˜narrubia, J., & Walker, M. G. 2024, ApJ, 968, 89, doi: 10.3847/1538-4357/ad402d
2024 doi
-
[28]
2020, MNRAS, 491, 4591, doi: 10.1093/mnras/stz3349 Euclid Collaboration, Scaramella, R., Amiaux, J., et al
Errani, R., & Pe˜narrubia, J. 2020, MNRAS, 491, 4591, doi: 10.1093/mnras/stz3349 Euclid Collaboration, Scaramella, R., Amiaux, J., et al. 2022, ˚a, 662, A112, doi: 10.1051/0004-6361/202141938 Euclid Collaboration, Mellier, Y., Abdurro’uf, et al. 2025a, A&A, 697, A1, doi: 10.10...
2020 doi
-
[29]
W., & Willman, B
Fadely, R., Hogg, D. W., & Willman, B. 2012, ApJ, 760, 15, doi: 10.1088/0004-637X/760/1/15
2012 doi
- [30]
-
[31]
S., et al
Garrison-Kimmel, S., Wetzel, A., Bullock, J. S., et al. 2017, MNRAS, 471, 1709, doi: 10.1093/mnras/stx1710
2017 doi
-
[32]
S., Bullock, J
Graus, A. S., Bullock, J. S., Kelley, T., et al. 2019, MNRAS, 488, 4585, doi: 10.1093/mnras/stz1992
2019 doi
-
[33]
P., Cuillandre, J.-C., Bachelet, E., et al
Guy, L. P., Cuillandre, J.-C., Bachelet, E., et al. 2022, in Zenodo id. 5836022, Vol. 58, 5836022, doi: 10.5281/zenodo.5836022
2022 doi
-
[34]
P., Bechtol, K., Bellm, E., et al
Guy, L. P., Bechtol, K., Bellm, E., et al. 2023, Rubin Observatory Plans for an Early Science Program, RTN-011. https://rtn-011.lsst.io/
2023
- [35]
-
[36]
R., Willman, B., & Peter, A
Hargis, J. R., Willman, B., & Peter, A. H. G. 2014, ApJ, 795, L13, doi: 10.1088/2041-8205/795/1/L13
2014 doi
-
[37]
R., Millman, K
Harris, C. R., Millman, K. J., van der Walt, S. J., et al. 2020, Nature, 585, 357, doi: 10.1038/s41586-020-2649-2
2020 doi
-
[38]
Harris, W. E. 1996, AJ, 112, 1487, doi: 10.1086/118116
1996 doi
-
[39]
2019, ApJS, 245, 16, doi: 10.3847/1538-4365/ab4da1
Heitmann, K., Finkel, H., Pope, A., et al. 2019, ApJS, 245, 16, doi: 10.3847/1538-4365/ab4da1
2019 doi
-
[40]
1991, The Bright star catalogue (Yale University Observatory)
Hoffleit, D., & Jaschek, C. 1991, The Bright star catalogue (Yale University Observatory)
1991
-
[41]
2024, PASJ, 76, 733, doi: 10.1093/pasj/psae044
Homma, D., Chiba, M., Komiyama, Y., et al. 2024, PASJ, 76, 733, doi: 10.1093/pasj/psae044
2024 doi
-
[42]
Hunter, J. D. 2007, Computing in Science & Engineering, 9, 90, doi: 10.1109/MCSE.2007.55 Ivezi´c, ˇZ., Kahn, S. M., Tyson, J. A., et al. 2019, ApJ, 873, 111, doi: 10.3847/1538-4357/ab042c
2007 doi
-
[43]
2018, MNRAS, 473, 2060, doi: 10.1093/mnras/stx2330
Jethwa, P., Erkal, D., & Belokurov, V. 2018, MNRAS, 473, 2060, doi: 10.1093/mnras/stx2330
2018 doi
-
[44]
P., Frebel, A., Chiti, A., & Simon, J
Ji, A. P., Frebel, A., Chiti, A., & Simon, J. D. 2016, Nature, 531, 610, doi: 10.1038/nature17425
2016 doi
-
[45]
L., Yoachim, P., Chandrasekharan, S., et al
Jones, R. L., Yoachim, P., Chandrasekharan, S., et al. 2015, in American Astronomical Society Meeting Abstracts, Vol. 225, American Astronomical Society Meeting Abstracts #225, 336.40 Juri´c, M., Ivezi´c, ˇZ., Brooks, A., et al. 2008, ApJ, 673, 864, doi: 10.1086/523619
2015 doi
-
[46]
V., Zivick, P., et al
Kallivayalil, N., Sales, L. V., Zivick, P., et al. 2018, ApJ, 867, 19, doi: 10.3847/1538-4357/aadfee
2018 doi
-
[47]
V., Piskunov, A
Kharchenko, N. V., Piskunov, A. E., Schilbach, E., R¨oser, S., & Scholz, R.-D. 2013, A&A, 558, A53, doi: 10.1051/0004-6361/201322302
2013 doi
-
[48]
P., Mackey, D., & Da Costa, G
Kim, D., Jerjen, H., Milone, A. P., Mackey, D., & Da Costa, G. S. 2015, ApJ, 803, 63, doi: 10.1088/0004-637X/803/2/63
2015 doi
- [49]
-
[50]
Y., Peter, A
Kim, S. Y., Peter, A. H. G., & Hargis, J. R. 2018, Phys. Rev. Lett., 121, 211302, doi: 10.1103/PhysRevLett.121.211302
2018 doi
-
[51]
W., et al
Koposov, S., Belokurov, V., Evans, N. W., et al. 2008, ApJ, 686, 279, doi: 10.1086/589911
2008 doi
-
[52]
2019, ApJS, 245, 26, doi: 10.3847/1538-4365/ab510c Kov´acs, A., & Szapudi, I
Korytov, D., Hearin, A., Kovacs, E., et al. 2019, ApJS, 245, 26, doi: 10.3847/1538-4365/ab510c Kov´acs, A., & Szapudi, I. 2015, MNRAS, 448, 1305, doi: 10.1093/mnras/stv063
2019 doi
-
[53]
2022, MNRAS, 514, 2667, doi: 10.1093/mnras/stac1439
Kravtsov, A., & Manwadkar, V. 2022, MNRAS, 514, 2667, doi: 10.1093/mnras/stac1439
2022 doi
-
[54]
Kravtsov, A. V. 2013, ApJ, 764, L31, doi: 10.1088/2041-8205/764/2/L31
2013 doi
-
[55]
Li, Z.-Z., Qian, Y.-Z., Han, J., Wang, W., & Jing, Y. P. 2019, ApJ, 886, 69, doi: 10.3847/1538-4357/ab4f6d
2019 doi
-
[56]
K., et al
Loveday, J., Norberg, P., Baldry, I. K., et al. 2015, MNRAS, 451, 1540, doi: 10.1093/mnras/stv1013 LSST DESC, Abolfathi, B., Armstrong, R., et al. 2022, DESC DC2 Data Release Note. https://arxiv.org/abs/2101.04855
2015 arXiv
-
[57]
2016, ApJ, 830, 59, doi: 10.3847/0004-637X/830/2/59
Lu, Y., Benson, A., Mao, Y.-Y., et al. 2016, ApJ, 830, 59, doi: 10.3847/0004-637X/830/2/59
2016 doi
-
[58]
2012, ApJ, 746, 109, doi: 10.1088/0004-637X/746/1/109
Lunnan, R., Vogelsberger, M., Frebel, A., et al. 2012, ApJ, 746, 109, doi: 10.1088/0004-637X/746/1/109
2012 doi
-
[59]
1976, MNRAS, 174, 695, doi: 10.1093/mnras/174.3.695
Lynden-Bell, D. 1976, MNRAS, 174, 695, doi: 10.1093/mnras/174.3.695
1976 doi
-
[60]
Malhan, K., Valluri, M., Freese, K., & Ibata, R. A. 2022, ApJ, 941, L38, doi: 10.3847/2041-8213/aca6e5
2022 doi
-
[61]
Manwadkar, V., & Kravtsov, A. V. 2022, MNRAS, 516, 3944, doi: 10.1093/mnras/stac2452
2022 doi
-
[62]
Mao, Y.-Y., Williamson, M., & Wechsler, R. H. 2015, ApJ, 810, 21, doi: 10.1088/0004-637X/810/1/21
2015 doi
-
[63]
2017, ApJ, 835, 77, doi: 10.3847/1538-4357/835/1/77
Marigo, P., Girardi, L., Bressan, A., et al. 2017, ApJ, 835, 77, doi: 10.3847/1538-4357/835/1/77
2017 doi
-
[64]
2019, ApJ, 875, 154, doi: 10.3847/1538-4357/ab0bb8
Mau, S., Drlica-Wagner, A., Bechtol, K., et al. 2019, ApJ, 875, 154, doi: 10.3847/1538-4357/ab0bb8
2019 doi
-
[65]
M., Applebaum, E., et al
Munshi, F., Brooks, A. M., Applebaum, E., et al. 2021, ApJ, 923, 35, doi: 10.3847/1538-4357/ac0db6
2021 doi
-
[66]
J., Crnojevi´c, D., et al
Mutlu-Pakdil, B., Sand, D. J., Crnojevi´c, D., et al. 2021, ApJ, 918, 88, doi: 10.3847/1538-4357/ac0db8
2021 doi
-
[67]
L., Goumiri, I
Muyskens, A. L., Goumiri, I. R., Priest, B. W., et al. 2022, AJ, 163, 148, doi: 10.3847/1538-3881/ac4e93
2022 doi
-
[68]
O., Gluscevic, V., Driskell, T., et al
Nadler, E. O., Gluscevic, V., Driskell, T., et al. 2024, ApJ, 967, 61, doi: 10.3847/1538-4357/ad3bb1
2024 doi
-
[69]
O., Mao, Y.-Y., Green, G
Nadler, E. O., Mao, Y.-Y., Green, G. M., & Wechsler, R. H. 2019, ApJ, 873, 34, doi: 10.3847/1538-4357/ab040e
2019 doi
-
[70]
O., Mao, Y.-Y., Wechsler, R
Nadler, E. O., Mao, Y.-Y., Wechsler, R. H., Garrison-Kimmel, S., & Wetzel, A. 2018, ApJ, 859, 129, doi: 10.3847/1538-4357/aac266
2018 doi
-
[71]
O., Wechsler, R
Nadler, E. O., Wechsler, R. H., Bechtol, K., et al. 2020, ApJ, 893, 48, doi: 10.3847/1538-4357/ab846a
2020 doi
-
[72]
O., Drlica-Wagner, A., Bechtol, K., et al
Nadler, E. O., Drlica-Wagner, A., Bechtol, K., et al. 2021, Phys. Rev. Lett., 126, 091101, doi: 10.1103/PhysRevLett.126.091101
2021 doi
-
[73]
S., & Helly, J
Newton, O., Cautun, M., Jenkins, A., Frenk, C. S., & Helly, J. C. 2018, MNRAS, 479, 2853, doi: 10.1093/mnras/sty1085
2018 doi
-
[74]
Newton, O., Leo, M., Cautun, M., et al. 2021, J. Cosmology Astropart. Phys., 2021, 062, doi: 10.1088/1475-7516/2021/08/062
2021 doi
- [75]
-
[76]
Pace, A. B. 2024, arXiv e-prints, arXiv:2411.07424, doi: 10.48550/arXiv.2411.07424
2024 doi
-
[77]
2020, ApJ, 893, 121, doi: 10.3847/1538-4357/ab7b75
Patel, E., Kallivayalil, N., Garavito-Camargo, N., et al. 2020, ApJ, 893, 121, doi: 10.3847/1538-4357/ab7b75
2020 doi
-
[78]
2018, Scikit-learn: Machine Learning in Python
Pedregosa, F., Varoquaux, G., Gramfort, A., et al. 2018, Scikit-learn: Machine Learning in Python. https://arxiv.org/abs/1201.0490
2018 arXiv
-
[79]
2020, MNRAS, 497, 1547, doi: 10.1093/mnras/staa1980
Pieres, A., Girardi, L., Balbinot, E., et al. 2020, MNRAS, 497, 1547, doi: 10.1093/mnras/staa1980
2020 doi
-
[80]
Plummer, H. C. 1911, MNRAS, 71, 460, doi: 10.1093/mnras/71.5.460
1911 doi
-
[81]
2019, HealSparse: A sparse implementation of HEALPix
Rykoff, E., & S´anchez, J. 2019, HealSparse: A sparse implementation of HEALPix. https://healsparse.readthedocs.io/
2019
-
[82]
J., Finkbeiner, D
Schlegel, D. J., Finkbeiner, D. P., & Davis, M. 1998, ApJ, 500, 525, doi: 10.1086/305772
1998 doi
-
[83]
J., et al
Sevilla-Noarbe, I., Hoyle, B., March˜a, M. J., et al. 2018, MNRAS, 481, 5451, doi: 10.1093/mnras/sty2579 18 Tsiane, Mau, Drlica-Wagner et al
2018 doi
- [84]
-
[85]
Simon, J. D. 2019, ARA&A, 57, 375, doi: 10.1146/annurev-astro-091918-104453
2019 doi
-
[86]
T., ˇZeljko Ivezi´c, & Lupton, R
Slater, C. T., ˇZeljko Ivezi´c, & Lupton, R. H. 2020, The Astronomical Journal, 159, 65, doi: 10.3847/1538-3881/ab6166
2020 doi
-
[87]
Smith, S. E. T., Cerny, W., Hayes, C. R., et al. 2024, ApJ, 961, 92, doi: 10.3847/1538-4357/ad0d9f
2024 doi
- [88]
-
[89]
J., Bullock, J
Tollerud, E. J., Bullock, J. S., Strigari, L. E., & Willman, B. 2008, ApJ, 688, 277, doi: 10.1086/592102
2008 doi
-
[90]
E., et al
Torrealba, G., Belokurov, V., Koposov, S. E., et al. 2019, MNRAS, 488, 2743, doi: 10.1093/mnras/stz1624
2019 doi
-
[91]
E., et al
Virtanen, P., Gommers, R., Oliphant, T. E., et al. 2020, Nature Methods, 17, 261, doi: 10.1038/s41592-019-0686-2
2020 doi
-
[92]
M., Willman, B., & Jerjen, H
Walsh, S. M., Willman, B., & Jerjen, H. 2008, The Astronomical Journal, 137, 450, doi: 10.1088/0004-6256/137/1/450
2008 doi
-
[93]
Webbink, R. F. 1985, in IAU Symposium, Vol. 113, Dynamics of Star Clusters, ed. J. Goodman & P. Hut, 541–577
1985
-
[94]
2011, The Astronomical Journal, 142, 128, doi: 10.1088/0004-6256/142/4/128
Willman, B., Geha, M., Strader, J., et al. 2011, The Astronomical Journal, 142, 128, doi: 10.1088/0004-6256/142/4/128
2011 doi
- [95]
-
[96]
Zonca, A., Singer, L., Lenz, D., et al. 2019, Journal of Open Source Software, 4, 1298, doi: 10.21105/joss.01298 A RUBIN SCIENCE PLATFORM PERFORMANCE Our analysis of the DC2 data is performed on the Rubin IDF using the RSP (O’Mullane et al. 2021), an online ser- vice that enab...
2019 doi
Reviewed August 16, 2026 · model on record in the stance chip above.
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