REVIEW 2 major objections 5 minor 29 references
HST Proper Motions of Andromeda V and VI
T0 review · 2 major / 5 minor · reviewed 2026-08-15 · deepseek-v4-flash
Pith's one-line read The paper measures absolute proper motions for two M31 dwarf satellites and derives their orbits, finding And VI co-orbits the disk while And V counter-orbits.
desk verdict First PMs for And V/VI; And VI's zero point has an internal 2.2σ chip discrepancy that should be addressed before relying on the co-rotation claim. 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 method rests on converting a relative proper motion into an absolute one using background galaxies as zero-point reference objects. For each satellite, early-epoch WFPC2 images from 2000 and late-epoch ACS/WFC images from 2020 are processed with the hst1pass code, and WFPC2 positions are refined by a deep-learning centering model that overcomes undersampling. Chip-to-chip and epoch-to-epoch transformations use polynomial fits, and the absolute proper motion is obtained as the mean motion of satellite members minus the weighted mean motion of roughly 100 galaxies per satellite. Orbit parameters come from integrating backward in time with Monte Carlo draws over distance, line-of-sight velocity, and proper-motion uncertainties, using two M31 potentials.
What would settle it
Compare the galaxy-based absolute proper motions with those from a future Gaia data release whose faint-end errors reach about 0.05-0.1 mas/yr for the same fields; a discrepancy larger than the quoted ~10-20 microarcsecond-per-year errors would falsify the galaxy calibration, as would a test with synthetic galaxies inserted into the WFPC2 and ACS frames showing systematic epoch- or filter-dependent centroid offsets.
Extended reading notes
Core claim
The paper reports two absolute proper motions: for And V, $(\mu_\alpha, \mu_\delta) = (26.1 \pm 21.5, -74.2 \pm 19.1)\ \mu\mathrm{as}\,\mathrm{yr}^{-1}$, and for And VI, $(\mu_\alpha, \mu_\delta) = (-1.6 \pm 12.3, -52.6 \pm 11.2)\ \mu\mathrm{as}\,\mathrm{yr}^{-1}$. These are the first proper motions for M31 satellites that lie far from the Great Plane of Andromeda but close to the M31 disk plane. Orbit integrations using two M31 mass models and two M31 proper motions show that And VI's orbit is well aligned with the M31 disk and co-rotates with it, while And V's orbit is consistent with a counter-rotating alignment, though less tightly constrained. Both satellites are bound to M31, and And VI remains at distances of at least about 90 kpc, supporting the interpretation that its cuspy central mass profile is preserved by a weak tidal field.
Load-bearing premise
Background galaxies have zero net motion and their centroids, measured with a stellar point-spread-function model, are unbiased between the 2000 WFPC2 and 2020 ACS epochs and filters.
Editorial extensions
If this is right
- The sample of M31 satellites with measured proper motions grows to six, including two objects outside the Great Plane of Andromeda but near the M31 disk.
- And VI's orbit, which keeps it beyond about 90 kpc from M31, corroborates the idea that its steep central mass profile results from a weak tidal history.
- Both satellites are well bound to M31, so they do not directly constrain M31's total mass, but they can be used in satellite-based mass constraints.
- The last pericenters of both satellites occurred on the far side of M31, offering a possible clue to the observed lopsidedness of the M31 satellite system.
- A future Gaia data release with improved faint-end precision could check the galaxy-based zero-point against the EDR3 stars identified in these fields.
Reading between the lines
- If And VI genuinely co-orbits the disk plane at about 280 kpc, the disk-aligned population of M31 satellites extends far beyond the Great Plane; a testable prediction is that other distant dwarf spheroidals near the disk plane will show the same co-rotation.
- The deep-learning centering of undersampled WFPC2 images could be applied to other archival HST two-epoch pairs, potentially yielding proper motions for many faint Local Group systems.
- A confirmed counter-orbiting And V would imply that disk-plane orbits around M31 are not all coherent in sense, complicating the single-rotating-plane picture.
- The zero-point precision is limited by galaxy centroid scatter; using a larger or morphologically curated galaxy sample could push the absolute proper motions below the current 10-20 microarcsecond-per-year level.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper measures absolute proper motions of the M31 dwarf satellites Andromeda V and Andromeda VI using HST WFPC2 (epoch ~2000) and ACS/WFC (epoch ~2020) images spanning a 20-year baseline. The WFPC2 data are processed with a deep-learning centering model and updated astrometric calibrations; the absolute zero-point is set by roughly 100 background galaxies per field. The resulting proper motions are combined with published distances, line-of-sight velocities, and two M31 proper-motion determinations to integrate orbits under two M31 mass models. The authors report that And VI is consistent, within uncertainties, with a co-planar, co-rotating orbit around M31's disk, while And V is consistent (with large errors) with a counter-orbiting alignment. They also find both satellites are well bound to M31 and that And VI remains beyond ~90 kpc, implying weak tidal effects.
Significance. If the measurements are correct, this is a valuable observational contribution: it increases the sample of M31 satellites with measured proper motions to six, adds the most distant satellite (And VI, ~280 kpc) to that sample, and provides the first orbit determinations for two satellites far from the Great Plane of Andromeda. The paper is careful with random-error propagation (Monte Carlo orbit realizations), uses an external reference frame (background galaxies) for the absolute zero-point, and makes the data sets available via MAST DOIs. The orbit analysis explores multiple M31 mass models and proper-motion choices, and the conclusions are appropriately hedged for And V. The central results, if robust, bear on the kinematics of M31's satellite system, the lopsidedness of the satellite distribution, and the tidal history of And VI.
major comments (2)
- [§4, Table 2] The absolute zero-point rests on the assumption that background-galaxy centroids measured with a stellar PSF model (hst1pass for ACS, the deep-learning model for WFPC2) are unbiased between the 2000 WFPC2 and 2020 ACS epochs and across filters. The manuscript presents no test of this assumption and assigns no systematic error to it. The data in Table 2 already contain a check: for And VI, the two ACS-chip zero-points are (µ_cor_alpha, µ_cor_delta) = (−27±12, 72±11) and (34±25, 69±21) µas/yr, which disagree in RA by 61±28 µas/yr (≈2.2σ), while the adopted absolute RA proper motion is only −1.6±12.3 µas/yr. Because And VI's disk-alignment conclusion depends on the direction of its ~50 µas/yr proper-motion vector, a shift of this size—well within the chip-2 solution's uncertainty—can rotate the orbital pole and weaken the co-planar, co-rotating claim. I request either a quantitative systematic-error term for the galaxy-centroid zero-point or a validation (e.g., splitting galaxies by morphology or color, or using the available Gaia EDR3 stars as a cross-check), and a discussion of the chip discrepancy.
- [§2.1, §4] The F450W WFPC2 data are processed with the F555W deep-learning centering model and PSF library (Section 2.1), while the ACS data use filter-specific models. For unresolved stars this may be acceptable, but for background galaxies—which are the sole absolute reference—a filter- or morphology-dependent centroid offset between epochs would appear directly as a spurious proper motion. The paper notes only that random positional errors for F450W are a few percent larger; it does not address the possibility of a systematic bias. This is a load-bearing point for the absolute proper motions and should be investigated or explicitly argued to be negligible.
minor comments (5)
- [Figure 7 caption] The caption reads 'Same an in Fig. 6' and should be corrected to 'Same as in Fig. 6'.
- [§6] The word 'immediatly' in the summary is a typo and should be 'immediately'.
- [§4] The sentence 'The final zero-point correction is a weighted average of all galaxies with total proper-motion values less than 2 mas yr−1' should specify whether the cut is on the quadrature sum of the two proper-motion components or on each component separately.
- [§5.2] The statement that the choice of M31 mass and proper motion 'does not strongly change the expected orbital characteristics' is followed by pericenter-time ranges of 1.5–2.0 Gyr for And VI; please quantify what 'not strongly' means in the text.
- [Keywords] The keyword list appears incomplete; consider adding 'dwarf galaxies' and 'galaxy kinematics' to improve discoverability.
Circularity Check
No circular derivation: absolute proper motions are anchored to an external background-galaxy reference frame, and the orbit conclusions use independent literature inputs; self-citations supply only centering and calibration tools.
full rationale
The measurement chain is self-contained against an external reference frame. Relative proper motions are derived from stellar positions across the 2000 WFPC2 and 2020 ACS epochs (Section 3), and the conversion to absolute proper motion is obtained by subtracting a zero point set by on the order of 100 background galaxies per satellite (Section 4: 'we rely solely on background galaxies to determine the correction to absolute proper motions'). The galaxies provide an inertial anchor independent of the satellite's own motion; no parameter is fitted to the final orbital alignment. The orbit analysis (Section 5) combines these proper motions with RR Lyrae distances (Savino et al. 2022), line-of-sight velocities (Collins et al. 2013), M31 potentials (Patel et al. 2017), and two M31 proper-motion estimates (Sohn et al. 2020; Pawlowski & Sohn 2021), with Monte Carlo propagation of uncertainties. The paper explicitly tests both M31 proper motions and both mass models, and the co-rotation/alignment conclusions are stated to hold across realizations, so the choice of M31 proper motion is not load-bearing. Self-citations (Casetti-Dinescu et al. 2021, 2024a, 2024b) provide WFPC2 distortion corrections and the deep-learning centering model; these are calibration tools validated on stellar images, not quantities fitted to the target proper motions, and they do not encode the orbit results. The noted 2.2-sigma disagreement between the two ACS-chip zero-point solutions for And VI is an internal systematic-precision issue, not a circularity.
Assumptions & free parameters
free parameters (4)
- Dynamical friction mass for And V (M_DF, AndV) =
2e9 M_sun
- Dynamical friction scale radius for And V (R_DF, AndV) =
0.7 kpc
- Dynamical friction mass for And VI (M_DF, AndVI) =
4e9 M_sun
- Dynamical friction scale radius for And VI (R_DF, AndVI) =
1.0 kpc
assumptions (4)
- domain assumption Background galaxies have zero net proper motion and provide an inertial reference frame
- domain assumption The F555W deep-learning centering model and distortion corrections are valid for F450W WFPC2 data
- domain assumption The Patel et al. (2017) M31 mass models (virial masses 1.5e12 and 2e12 M_sun) represent the gravitational potential
- domain assumption Published distances (Savino et al. 2022) and M31 proper motions (Sohn et al. 2020; Salomon et al. 2021) are adopted as inputs
Cite this review
Pith. "Pith review of HST Proper Motions of Andromeda V and VI." pith.science (2026). https://pith.science/paper/5RLVDWIM
@misc{pith2026250906215,
author = {Pith},
title = {Pith review of: HST Proper Motions of Andromeda V and VI},
year = {2026},
howpublished = {\url{https://pith.science/paper/5RLVDWIM}},
note = {Machine review of arXiv:2509.06215}
}
abstract
We measure the absolute proper motions of Andromeda V (And V) and Andromeda VI/Pegasus (And VI) dwarf galaxies, satellites of M31 located near its galactic plane. And VI is located the farthest from M31 among the six satellites with currently measured proper motions. A combination of ACS/WFC and WFPC2 exposures are utilized, spanning a 20-year time baseline. The WFPC2 exposures are processed using a recently developed deep-learning centering procedure as well as the most up-to-date astrometric calibration of the camera. We use on the order of 100 background galaxies per satellite to determine the correction to absolute proper motion. For And V we obtain an absolute proper motion of $(\mu_{\alpha} , \mu_{\delta})_{And\,V} = (26.1\pm21.5, -74.2\pm19.1)~\mu$as yr$^{-1}$. For And VI we obtain an absolute proper motion of $(\mu_{\alpha} , \mu_{\delta})_{And\,VI} = (-1.6\pm12.3, -52.6\pm11.2)~\mu$as yr$^{-1}$. Orbit integrations and analyses are made for these two Andromeda satellites using two estimates of both the mass and proper motion of M31. It is found that And V has an orbit consistent within errors with alignment with M31's disk and counter orbiting it, although this alignment is not well constrained. And VI's orbit is better determined and is very much consistent with co-orbiting with M31's disk. While currently at a distance of ~280 kpc from M31, And VI will remain beyond a distance of ~ 90 kpc from M31, thus experiencing low tidal influence compared to the other M31 satellites with known orbits. Both satellites are determined to be well-bound to M31.
Figures
Figures from the paper (3 more)
Reference graph
Works this paper leans on
-
[1]
2022, One-Pass HST Photometry with hst1pass, Instrument Science Report ACS 2022-02, ,
Anderson, J. 2022, One-Pass HST Photometry with hst1pass, Instrument Science Report ACS 2022-02, ,
work page 2022
-
[2]
Anderson, J., & King, I. R. 1999, PASP, 111, 1095 —. 2000, PASP, 112, 1360 —. 2003, PASP, 115, 113
work page 1999
- [3]
- [4]
- [5]
-
[6]
Menten, K. M. 2007, A&A, 462, 101
work page 2007
-
[7]
Casetti-Dinescu, D. I., Girard, T. M., Kozhurina-Platais, V., et al. 2021, PASP, 133, 064505
work page 2021
-
[8]
Collins, M. L. M., Chapman, S. C., Rich, R. M., et al. 2013, ApJ, 768, 172
work page 2013
Show all 29 references
-
[9]
R., Lewis, G
Conn, A. R., Lewis, G. F., Ibata, R. A., et al. 2013, ApJ, 766, 120
2013
-
[10]
I., Girard, T
Dinescu, D. I., Girard, T. M., van Altena, W. F., Mendez, R. A., & Lopez, C. E. 1997, AJ, 114, 1014
1997
-
[11]
Doliva-Dolinsky, A., Collins, M. L. M., & Martin, N. F. 2025, arXiv e-prints, arXiv:2502.06948 Gaia Collaboration, Brown, A. G. A., Vallenari, A., et al. 2021, A&A, 649, A1
2025 arXiv
-
[12]
Hamaker, H. C. 1978, Journal of the Royal Statistical Society. Series C (Applied Statistics), 27, 76
1978
-
[13]
A., Lewis, G
Ibata, R. A., Lewis, G. F., Conn, A. R., et al. 2013, Nature, 493, 62
2013
-
[14]
J., Pawlowski, M
Kanehisa, K. J., Pawlowski, M. S., & Libeskind, N. 2025, Nature Astronomy, 9, 692
2025
-
[15]
2015, ACS/WFC Revised Geometric Distortion for DrizzlePac, Instrument Science Report ACS/WFC 2015-06, 47 pages, ,
Grogin, N., & Hack, M. 2015, ACS/WFC Revised Geometric Distortion for DrizzlePac, Instrument Science Report ACS/WFC 2015-06, 47 pages, ,
2015
-
[16]
2018, Accuracy of the HST Standard Astrometric Catalogs w.r.t
Kozhurina-Platais, V., Grogin, N., & Sabbi, E. 2018, Accuracy of the HST Standard Astrometric Catalogs w.r.t. Gaia, Instrument Science Report ACS 2018-01, 17 pages, ,
2018
-
[17]
S., Kanehisa, K
Kumar, P., Pawlowski, M. S., Kanehisa, K. J., et al. 2025, arXiv e-prints, arXiv:2506.01459
2025 arXiv
-
[18]
McConnachie, A. W. 2012, AJ, 144, 4
2012
-
[19]
Patel, E., Besla, G., & Sohn, S. T. 2017, MNRAS, 464, 3825
2017
-
[20]
Patel, E., & Mandel, K. S. 2023, ApJ, 948, 104
2023
-
[21]
S., Kroupa, P., & Jerjen, H
Pawlowski, M. S., Kroupa, P., & Jerjen, H. 2013, MNRAS, 435, 1928
2013
-
[22]
S., & Sohn, S
Pawlowski, M. S., & Sohn, S. T. 2021, ApJ, 923, 42
2021
-
[23]
S., Collins, M
Pickett, C. S., Collins, M. L. M., Rich, R. M., et al. 2025, MNRAS, 540, 1701
2025
-
[24]
B., Ibata, R., Reyl´ e, C., et al
Salomon, J. B., Ibata, R., Reyl´ e, C., et al. 2021, MNRAS, 507, 2592
2021
-
[25]
R., Skillman, E
Savino, A., Weisz, D. R., Skillman, E. D., et al. 2022, ApJ, 938, 101
2022
-
[26]
R., Dolphin, A
Savino, A., Weisz, D. R., Dolphin, A. E., et al. 2025, ApJ, 979, 205
2025
-
[27]
T., Anderson, J., & van der Marel, R
Sohn, S. T., Anderson, J., & van der Marel, R. P. 2012, ApJ, 753, 7
2012
-
[28]
T., Patel, E., Fardal, M
Sohn, S. T., Patel, E., Fardal, M. A., et al. 2020, ApJ, 901, 43 van der Marel, R. P., Fardal, M. A., Sohn, S. T., et al. 2019, ApJ, 872, 24
2020
-
[29]
T., Kallivayalil, N., Zivick, P., et al
Warfield, J. T., Kallivayalil, N., Zivick, P., et al. 2023, MNRAS, 519, 1189
2023
Reviewed August 15, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.