REVIEW 3 major objections 5 minor 58 references
A North-South Metallicity Asymmetry in the Outer Galactic disk -- Evidence for the Pericentric Passage of the Sagittarius Dwarf Galaxy
T0 review · 3 major / 5 minor · reviewed 2026-08-06 · deepseek-v4-flash
Pith's one-line read Beyond 11 kpc, the Milky Way's disk is chemically lopsided: stars north of the plane are up to 0.15 dex richer in metals toward the anti-center, which the authors attribute to the Sagittarius dwarf's recent passage through the disk.
desk verdict A plausible outer-disk metallicity asymmetry that needs a selection-function analysis before I'd believe it isn't a LAMOST/APOGEE footprint artifact. 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 load-bearing objects are red clump stars, core helium-burning giants whose nearly constant intrinsic luminosity makes them standard candles with distances accurate to roughly 5--10 percent, combined with survey-based metallicities and ages. The argument's machinery is the $R$--$Z$ metallicity-offset map: stars are split into six azimuthal bins, the mean metallicity in each radial bin is subtracted to remove the known radial gradient, and the residual north--south offset is read off the maps and summarized by the asymmetry measure $A$. Mono-age cuts in 2 Gyr steps are what connect the asymmetry to a recent event, because younger populations should retain a vertical perturbation better than older, kinematically hotter ones.
What would settle it
Recompute the metallicity-offset maps with a sample whose selection function is matched on both sides of the plane, such as a strictly magnitude-limited all-sky catalog with uniform footprint, and check whether the north--south difference at $R > 11$ kpc and $-5^\circ < \Phi < 15^\circ$ persists; if it disappears, the claim is refuted. A second decisive test is to run the identical analysis on mock observations drawn from an axisymmetric chemical model observed through the real survey footprints; if the footprints alone reproduce a north--south offset near 0.1 dex, the interpretation collapses.
Extended reading notes
Core claim
The discovery is an azimuthally localized chemical asymmetry in the outer disk. After removing the radial metallicity gradient by subtracting the mean $[\mathrm{Fe/H}]$ in each $R$ bin, the mean-metallicity-offset maps in the $R$--$Z$ plane show mirror symmetry for $R < 11$ kpc but not beyond it: in the wedge $-5^\circ < \Phi < 15^\circ$ the northern side is more metal-rich by up to $0.15$ dex. The paper quantifies this with the asymmetry measure $A = ([\mathrm{Fe/H}]_{\rm North} - [\mathrm{Fe/H}]_{\rm South})/([\mathrm{Fe/H}]_{\rm North} + [\mathrm{Fe/H}]_{\rm South})$, which is positive near the midplane and declines with height. Splitting the sample by age, the asymmetry is present for all populations but is significantly weaker for $\tau > 8$ Gyr, which the authors attribute to larger age uncertainties, fewer stars in the outer disk, and the kinematically hotter nature of old populations. They conclude that the most plausible origin is the perturbing passage and tidal force of the Sagittarius dwarf galaxy within the last few gigayears.
Load-bearing premise
The two surveys observe the northern and southern sides of the disk with different footprints and target selection, and the paper does not model or correct for these selection effects; if the northern sample is biased toward brighter, more metal-rich stars, the measured 0.0 to 0.15 dex asymmetry would be an artifact rather than a property of the Galaxy.
Editorial extensions
If this is right
- If the asymmetry is physical, the outer disk's chemical profile cannot be reduced to a single vertical gradient; models of the disk must accommodate a localized north--south chemical offset near the anti-center.
- The confinement of the signal to $R > 11$ kpc and $-5^\circ < \Phi < 15^\circ$ gives a spatial anchor for where a perturbing dwarf crossed the disk.
- The presence of the asymmetry in every mono-age population, strongest for stars younger than about 6 Gyr, implies the event occurred recently enough that it has not yet been fully phase-mixed away.
- The weaker signal in stars older than 8 Gyr is consistent with kinematic heating and larger age errors, and predicts that better age measurements should sharpen the old-population asymmetry if the interpretation is correct.
- The azimuthal localization argues against the Galactic warp's line of nodes as the cause and points instead to a disk-crossing dwarf, with the Sagittarius dwarf galaxy as the leading candidate.
Reading between the lines
- A direct test the paper does not carry out: simulate the same survey selection functions and ask whether they alone produce a false north--south difference of order 0.1 dex; if they do, the Sagittarius interpretation is unsupported.
- If the gas-compression picture is right, the northern outer disk should show a localized excess of young stars and elevated star formation in the same azimuthal wedge, which future high-precision photometry and astrometry could confirm.
- The same analysis applied to external edge-on or mildly inclined disk galaxies with recent minor mergers could search for analogous chemical asymmetries across their midplanes.
- Because the oldest populations show the weakest signal, targeted observations of outer-disk red giants with precise ages are the most direct way to decide whether the age dependence is physical or a sample-size effect.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper combines LAMOST DR8 and APOGEE DR17 red clump stars (110,550 and 35,512 stars) to construct mean-metallicity-offset maps in the Galactocentric R–Z plane in six azimuthal bins, after subtracting the mean metallicity per radial bin. The authors report that the inner disk (R < 11 kpc) is North–South symmetric, while the outer disk (R > 11 kpc), especially toward the anti-Galactic center (−5° < Φ < 15°), shows higher median metallicities in the North than in the South by about 0.0–0.15 dex. Splitting by stellar age, they claim the asymmetry is present across all mono-age populations but weaker for τ > 8 Gyr, and they interpret the signal as evidence of the recent pericentric passage and tidal force of the Sagittarius dwarf galaxy.
Significance. If the asymmetry is real, it would be an interesting, localized chemo-structural signature of external perturbation in the outer Milky Way disk, adding to the body of evidence linking Sgr passages to disk asymmetries. The analysis uses a large red clump sample with homogenized ages and metallicities, including an explicit cross-survey age calibration on common stars, which are genuine strengths. The main limitation is that the result currently rests on an unmodeled combination of two surveys with very different footprints and target selection; because the quoted asymmetry range includes 0.0 dex and no formal significance test is reported, the observational claim is not yet separated from survey systematics.
major comments (3)
- [Section 2.1 and Section 3.1] The paper does not model or correct for the target selection, completeness, magnitude limits, or footprint differences of LAMOST and APOGEE. The reported asymmetry is localized to R > 11 kpc and −5° < Φ < 15°, precisely the anti-center region where a declination-limited northern survey (LAMOST) and a target-flagged survey (APOGEE) are not symmetric about b = 0. In that region Z > 0 corresponds to positive Galactic latitude, so any latitude-dependent difference in survey mix, signal-to-noise completeness, or reddening coverage can produce a Z-dependent [Fe/H] offset of the quoted size. The sample definition in Section 2.1 and the radial-gradient subtraction in Section 3.1 do not address this. A survey-split analysis (LAMOST only, APOGEE only) or an explicit selection-function correction is necessary to support the claim that the asymmetry is a property of the Galaxy rather than of the sample.
- [Section 3.1 and Figure 4] No formal significance test is provided for the asymmetry. Figures 3–6 show binned maps and median profiles, and Equation (1) defines A as the difference of the Northern and Southern median metallicities divided by their sum, but the paper does not give uncertainties on A, confidence intervals, or a null-hypothesis test (e.g., bootstrap or permutation test) for the null A = 0. Because the reported metallicity difference is stated as 0.0–0.15 dex and the lower end of the quoted range is zero, the visual impression in the maps is not sufficient to establish a detection. The authors should quantify the significance of the asymmetry in the specific bins and azimuthal range where they claim it.
- [Section 3.2 and Figure 6c] The abstract and Section 3.2 state that the asymmetry is detected 'across all mono-age stellar populations,' but Figure 6c and the accompanying text in Section 3.2 say that for older populations (τ > 8 Gyr) the metallicity asymmetry is 'not so significant' and that the asymmetries shown in that panel 'are not significant.' These statements are inconsistent. Either the claim of detection for all mono-age populations should be weakened to a claim for younger populations, or additional evidence (e.g., a significance test for the old-age bins) must be provided. As written, the paper's own Figure 6c undermines the 'all populations' claim.
minor comments (5)
- [Abstract and header] There are typos in the abstract and running header: 'purturbation' should be 'perturbation', and the header 'Evidence for the percentric passage' should be 'pericentric passage'.
- [Section 2.1] In the sentence defining the coordinate system, 'Φ = 0 defined alone the anti-center Galactic direction' should read 'defined along the anti-center direction'.
- [Equation (1)] The definition A = ([Fe/H]_North − [Fe/H]_South)/([Fe/H]_North + [Fe/H]_South) is unconventional because the median metallicities are negative quantities, so A is not a fractional difference in the usual sense; a simple difference with bootstrap uncertainties would be more interpretable.
- [Section 3.2] The phrase 'In the case of these stars, we focused on investigating the metallicity asymmetry within the most heterogeneous stellar populations' is awkward and unclear; consider rewriting to say that the analysis is restricted to the azimuthal range −5° < Φ < 15°.
- [Figures 3 and 5] The color scales in Figures 3 and 5 are different, which makes visual comparison of the asymmetry amplitude between the full sample and the age-split sample difficult; using a common color scale would help the reader evaluate the claimed age dependence.
Circularity Check
No significant circularity; the north-south metallicity asymmetry is a direct observational statistic, the age/metallicity calibrations use external common-star anchors, and the Sagittarius origin is explicitly speculative rather than derived.
full rationale
The central claim is a direct empirical statistic: Eq. (1) defines A from observed median metallicities, and the reported 0.0–0.15 dex offset is read off the resulting maps, not produced by any fitted parameter. The only calibration steps are (i) the COBS age relation in §2.2, fit to common LAMOST/APOGEE stars and then subtracted from the age scale, and (ii) the LAMOST metallicity scale, which is anchored to APOGEE via common-star training (Wang et al. 2022); both are external anchors, and neither is varied to produce the asymmetry. The radial-gradient removal in §3.1 subtracts the mean metallicity in each R bin, a standard centering procedure that does not by construction generate a North-South difference. The interpretation involving a Sagittarius passage is presented as a possible origin ('may be the consequence'), not as a derived consequence of the data, and is supported by independent simulations (Chequers et al. 2018) and prior observations (An 2019). Self-citations (Wang et al. 2019b, 2022, 2023) supply published catalogs and a prior azimuthal constraint, but the asymmetry measurement does not reduce to them. The unmodeled North/South selection functions of LAMOST and APOGEE are a real systematic risk that the paper does not address, but that is a data-quality concern, not a circularity: no equation in the paper is equivalent to its own input by construction.
Assumptions & free parameters
free parameters (2)
- COBS age-correction polynomial =
Coefficients not reported
- Outer-disk cutoff =
11 kpc
assumptions (4)
- domain assumption Red clump stars are standard candles with 5-10% distance accuracy.
- domain assumption LAMOST and APOGEE metallicities are on a consistent scale with no systematic north-south offset.
- domain assumption The radial metallicity gradient can be removed by subtracting the mean metallicity in each R bin without introducing an artificial north-south asymmetry.
- ad hoc to paper The sample selection functions of LAMOST and APOGEE do not produce a spurious metallicity difference between hemispheres.
Cite this review
Pith. "Pith review of A North-South Metallicity Asymmetry in the Outer Galactic disk -- Evidence for the Pericentric Passage of the Sagittarius Dwarf Galaxy." pith.science (2026). https://pith.science/paper/AFTCDLI2
@misc{pith2026250721551,
author = {Pith},
title = {Pith review of: A North-South Metallicity Asymmetry in the Outer Galactic disk -- Evidence for the Pericentric Passage of the Sagittarius Dwarf Galaxy},
year = {2026},
howpublished = {\url{https://pith.science/paper/AFTCDLI2}},
note = {Machine review of arXiv:2507.21551}
}
abstract
We present maps of the mean metallicity distributions on the Galactocentric $R$--$Z$ plane at different azimuthal angles using red clump stars selected from the LAMOST and APOGEE surveys. In the inner disk ($R < $ 11\,kpc), the metallicity distribution is symmetric between the upper and lower disk. However, we find a North-South metallicity asymmetry in the outer disk ($R > 11$\,kpc), especially towards the anti-Galactic center ($-5^\circ < \Phi < 15^\circ$) direction. By further dissecting the map in age space, we detect this asymmetry across all mono-age stellar populations. However, the asymmetry is less pronounced in older populations ($\tau > 8$ Gyr) compared to younger ones ($\tau < 6$\,Gyr). This reduced significance likely stems from three factors: larger age uncertainties, fewer stars in the outer disk, and the kinematically hotter nature of older populations. The observed metallicity asymmetry may be the consequence of the purturbation of the recent pericentric passage through the Galactic disk and tidal force of the well-known Sagittarius dwarf galaxy.
Figures
Figures from the paper (5 more)
Reference graph
Works this paper leans on
-
[1]
2019, ApJL, 878, L31, doi: 10.3847/2041-8213/ab2467
An, D. 2019, ApJL, 878, L31, doi: 10.3847/2041-8213/ab2467
-
[2]
Anders, F., Gispert, P., Ratcliffe, B., et al. 2023, arXiv e-prints, arXiv:2304.08276, doi: 10.48550/arXiv.2304.08276
work page Pith review arXiv doi:10.48550/arxiv.2304.08276 2023
-
[3]
Johnson, J. A. 2017, ApJ, 835, 224, doi: 10.3847/1538-4357/835/2/224
-
[4]
2023, MNRAS, doi: 10.1093/mnras/stad3244
Annem, B., & Khoperskov, S. 2023, MNRAS, doi: 10.1093/mnras/stad3244
-
[5]
2008, A&A, 490, 135, doi: 10.1051/0004-6361:200809519
Antoja, T., Figueras, F., Fern´ andez, D., & Torra, J. 2008, A&A, 490, 135, doi: 10.1051/0004-6361:200809519
-
[6]
2018, Nature, 561, 360, doi: 10.1038/s41586-018-0510-7
Antoja, T., Helmi, A., Romero-G´ omez, M., et al. 2018, Nature, 561, 360, doi: 10.1038/s41586-018-0510-7
-
[7]
2019, MNRAS, 482, 1417, doi: 10.1093/mnras/sty2813
Bennett, M., & Bovy, J. 2019, MNRAS, 482, 1417, doi: 10.1093/mnras/sty2813
-
[8]
1992, ARA&A, 30, 51, doi: 10.1146/annurev.aa.30.090192.000411
Binney, J. 1992, ARA&A, 30, 51, doi: 10.1146/annurev.aa.30.090192.000411
Show all 58 references
-
[9]
2021, MNRAS, 504, 3168, doi: 10.1093/mnras/stab704
Bland-Hawthorn, J., & Tepper-Garc ´ ıa, T. 2021, MNRAS, 504, 3168, doi: 10.1093/mnras/stab704
2021 doi
-
[10]
L., Rix, H.-W., et al
Bovy, J., Nidever, D. L., Rix, H.-W., et al. 2014, ApJ, 790, 127, doi: 10.1088/0004-637X/790/2/127
2014 doi
-
[11]
L., DeLaunay, J., Newberg, H
Carlin, J. L., DeLaunay, J., Newberg, H. J., et al. 2013, ApJL, 777, L5, doi: 10.1088/2041-8205/777/1/L5
2013 doi
-
[12]
2019, Nature Astronomy, 3, 320, doi: 10.1038/s41550-018-0686-7
Chen, X., Wang, S., Deng, L., et al. 2019, Nature Astronomy, 3, 320, doi: 10.1038/s41550-018-0686-7
2019 doi
-
[13]
H., Widrow, L
Chequers, M. H., Widrow, L. M., & Darling, K. 2018, MNRAS, 480, 4244, doi: 10.1093/mnras/sty2114
2018 doi
-
[14]
2008, A&A, 483, 401, doi: 10.1051/0004-6361:200809413
Colavitti, E., Matteucci, F., & Murante, G. 2008, A&A, 483, 401, doi: 10.1051/0004-6361:200809413
2008 doi
-
[15]
2024, MNRAS, 527, 4505, doi: 10.1093/mnras/stad3344
Das, P., Huang, Y., Ciuc˘ a, I., & Fragkoudi, F. 2024, MNRAS, 527, 4505, doi: 10.1093/mnras/stad3344
2024 doi
-
[16]
1999, ApJL, 524, L35, doi: 10.1086/312299
Dehnen, W. 1999, ApJL, 524, L35, doi: 10.1086/312299
1999 doi
-
[17]
J., Liu, C., et al
Deng, L.-C., Newberg, H. J., Liu, C., et al. 2012, Research in Astronomy and Astrophysics, 12, 735, doi: 10.1088/1674-4527/12/7/003 Garc ´ ıa P´ erez, A. E., Allende Prieto, C., Holtzman, J. A., et al. 2016a, AJ, 151, 144, doi: 10.3847/0004-6256/151/6/144 —. 2016b, AJ, 151, 14...
2012
-
[18]
Grillmair, C. J. 2006, ApJL, 651, L29, doi: 10.1086/509255
2006 doi
-
[19]
2018, ArXiv e-prints
Grisoni, V., Spitoni, E., & Matteucci, F. 2018, ArXiv e-prints. https://arxiv.org/abs/1805.11415
2018 arXiv
-
[20]
D., Di Matteo, P., et al
Haywood, M., Lehnert, M. D., Di Matteo, P., et al. 2016, A&A, 589, A66, doi: 10.1051/0004-6361/201527567
2016 doi
-
[21]
C., & Zhang, H
Huang, Y., Yuan, H., Beers, T. C., & Zhang, H. 2021, ApJL, 910, L5, doi: 10.3847/2041-8213/abe69a
2021 doi
-
[22]
2015, Research in Astronomy and Astrophysics, 15, 1240, doi: 10.1088/1674-4527/15/8/010
Huang, Y., Liu, X.-W., Zhang, H.-W., et al. 2015, Research in Astronomy and Astrophysics, 15, 1240, doi: 10.1088/1674-4527/15/8/010
2015 doi
-
[23]
2024, Nature Astronomy, 8, 1294, doi: 10.1038/s41550-024-02309-5 J¨ onsson, H., Holtzman, J
Huang, Y., Feng, Q., Khachaturyants, T., et al. 2024, Nature Astronomy, 8, 1294, doi: 10.1038/s41550-024-02309-5 J¨ onsson, H., Holtzman, J. A., Allende Prieto, C., et al. 2020a, AJ, 160, 120, doi: 10.3847/1538-3881/aba592 —. 2020b, AJ, 160, 120, doi: 10.3847/1538-3881/aba592 ...
2024 doi
-
[24]
2011, ApJ, 729, 16, doi: 10.1088/0004-637X/729/1/16
Kobayashi, C., & Nakasato, N. 2011, ApJ, 729, 16, doi: 10.1088/0004-637X/729/1/16
2011 doi
-
[25]
Laporte, C. F. P., Belokurov, V., Koposov, S. E., Smith, M. C., & Hill, V. 2020, MNRAS, 492, L61, doi: 10.1093/mnrasl/slz167 10 W ang C. et al
2020 doi
-
[26]
2018, MNRAS, 481, 286, doi: 10.1093/mnras/sty1574
Garavito-Camargo, N., & Besla, G. 2018, MNRAS, 481, 286, doi: 10.1093/mnras/sty1574
2018 doi
-
[27]
Laporte, C. F. P., Minchev, I., Johnston, K. V., & G´ omez, F. A. 2019, MNRAS, 485, 3134, doi: 10.1093/mnras/stz583
2019 doi
-
[28]
Larson, R. B. 1976, MNRAS, 176, 31, doi: 10.1093/mnras/176.1.31
1976 doi
-
[29]
S., Blitz, L., & Heiles, C
Levine, E. S., Blitz, L., & Heiles, C. 2006, ApJ, 643, 881, doi: 10.1086/503091
2006 doi
-
[30]
Y., Huang, Y., Chen, B
Li, X. Y., Huang, Y., Chen, B. Q., et al. 2020, ApJ, 901, 56, doi: 10.3847/1538-4357/aba61e
2020 doi
-
[31]
2014, in IAU
Liu, X.-W., Yuan, H.-B., Huo, Z.-Y., et al. 2014, in IAU
2014
-
[32]
298, IAU Symposium, ed
Symposium, Vol. 298, IAU Symposium, ed. S. Feltzing, G. Zhao, N. A. Walton, & P. Whitelock, 310–321, doi: 10.1017/S1743921313006510
-
[33]
R., Roˇ skar, R., Debattista, V
Loebman, S. R., Roˇ skar, R., Debattista, V. P., et al. 2011, ApJ, 737, 8, doi: 10.1088/0004-637X/737/1/8
2011 doi
-
[34]
R., Schiavon, R
Majewski, S. R., Schiavon, R. P., Frinchaboy, P. M., et al. 2017, AJ, 154, 94, doi: 10.3847/1538-3881/aa784d
2017 doi
-
[35]
2018, MNRAS, 481, 1645, doi: 10.1093/mnras/sty2033
Minchev, I., Anders, F., Recio-Blanco, A., et al. 2018, MNRAS, 481, 1645, doi: 10.1093/mnras/sty2033
2018 doi
-
[36]
J., Yanny, B., Rockosi, C., et al
Newberg, H. J., Yanny, B., Rockosi, C., et al. 2002, ApJ, 569, 245, doi: 10.1086/338983
2002 doi
-
[37]
T., & Maechler, M
Ng, P. T., & Maechler, M. 2015, COBS: COnstrained
2015
-
[38]
2004, A&A, 418, 989, doi: 10.1051/0004-6361:20035959
B-Splines, Astrophysics Source Code Library, record ascl:1505.010 Nordstr¨ om, B., Mayor, M., Andersen, J., et al. 2004, A&A, 418, 989, doi: 10.1051/0004-6361:20035959
2004 doi
-
[39]
2016, MNRAS, 455, 2308, doi: 10.1093/mnras/stv2397
Pezzulli, G., & Fraternali, F. 2016, MNRAS, 455, 2308, doi: 10.1093/mnras/stv2397
2016 doi
-
[40]
2020, Nature Astronomy, 4, 590, doi: 10.1038/s41550-020-1017-3
Poggio, E., Drimmel, R., Andrae, R., et al. 2020, Nature Astronomy, 4, 590, doi: 10.1038/s41550-020-1017-3
2020 doi
-
[41]
2011, Nature, 477, 301, doi: 10.1038/nature10417
Chakrabarti, S. 2011, Nature, 477, 301, doi: 10.1038/nature10417
2011 doi
-
[42]
J., Hernquist, L., & Fullagar, D
Quinn, P. J., Hernquist, L., & Fullagar, D. P. 1993, ApJ, 403, 74, doi: 10.1086/172184
1993 doi
-
[43]
J., Menten, K
Reid, M. J., Menten, K. M., Brunthaler, A., et al. 2014, ApJ, 783, 130, doi: 10.1088/0004-637X/783/2/130 Roˇ skar, R., Debattista, V. P., Quinn, T. R., Stinson, G. S., & Wadsley, J. 2008, ApJL, 684, L79, doi: 10.1086/592231
2014 doi
-
[44]
J., & Cassisi, S
Ruiz-Lara, T., Gallart, C., Bernard, E. J., & Cassisi, S. 2020, Nature Astronomy, 4, 965, doi: 10.1038/s41550-020-1097-0 Sch¨ onrich, R., & Binney, J. 2009, MNRAS, 399, 1145, doi: 10.1111/j.1365-2966.2009.15365.x
2020
-
[45]
A., & Binney, J
Sellwood, J. A., & Binney, J. J. 2002, MNRAS, 336, 785, doi: 10.1046/j.1365-8711.2002.05806.x Tepper-Garc ´ ıa, T., & Bland-Hawthorn, J. 2018, MNRAS, 478, 5263, doi: 10.1093/mnras/sty1359
2002
-
[46]
2018, ApJL, 865, L19, doi: 10.3847/2041-8213/aae1f3
Tian, H.-J., Liu, C., Wu, Y., Xiang, M.-S., & Zhang, Y. 2018, ApJL, 865, L19, doi: 10.3847/2041-8213/aae1f3
2018 doi
-
[47]
2018, ApJ, 855, 104, doi: 10.3847/1538-4357/aab044
Toyouchi, D., & Chiba, M. 2018, ApJ, 855, 104, doi: 10.3847/1538-4357/aab044
2018 doi
-
[48]
Velazquez, H., & White, S. D. M. 1999, MNRAS, 304, 254, doi: 10.1046/j.1365-8711.1999.02354.x Villalobos, ´A., & Helmi, A. 2008, MNRAS, 391, 1806, doi: 10.1111/j.1365-2966.2008.13979.x
1999
-
[49]
2022, ApJS, 259, 51, doi: 10.3847/1538-4365/ac4df7
Wang, C., Huang, Y., Yuan, H., et al. 2022, ApJS, 259, 51, doi: 10.3847/1538-4365/ac4df7
2022 doi
-
[50]
2023, A&A, 675, A26, doi: 10.1051/0004-6361/202245809
Wang, C., Huang, Y., Zhou, Y., & Zhang, H. 2023, A&A, 675, A26, doi: 10.1051/0004-6361/202245809
2023 doi
-
[51]
W., Xiang, M
Wang, C., Liu, X. W., Xiang, M. S., et al. 2019a, MNRAS, 482, 2189, doi: 10.1093/mnras/sty2797
-
[52]
B., et al
Wang, C., Huang, Y., Yuan, H. B., et al. 2019b, ApJL, 877, L7, doi: 10.3847/2041-8213/ab1fdd
-
[53]
2012, ApJL, 750, L41, doi: 10.1088/2041-8205/750/2/L41
Chen, H.-Y. 2012, ApJL, 750, L41, doi: 10.1088/2041-8205/750/2/L41
2012 doi
-
[54]
Williams, M. E. K., Steinmetz, M., Binney, J., et al. 2013, MNRAS, 436, 101, doi: 10.1093/mnras/stt1522
2013 doi
-
[55]
2015, Research in Astronomy and Astrophysics, 15, 1209, doi: 10.1088/1674-4527/15/8/009
Xiang, M.-S., Liu, X.-W., Yuan, H.-B., et al. 2015, Research in Astronomy and Astrophysics, 15, 1209, doi: 10.1088/1674-4527/15/8/009
2015 doi
-
[56]
2013, ApJ, 777, 91, doi: 10.1088/0004-637X/777/2/91
Yanny, B., & Gardner, S. 2013, ApJ, 777, 91, doi: 10.1088/0004-637X/777/2/91
2013 doi
-
[57]
2025, AJ, 169, 61, doi: 10.3847/1538-3881/ad9582
Yu, Z., Chen, B., Lian, J., Wang, C., & Liu, X. 2025, AJ, 169, 61, doi: 10.3847/1538-3881/ad9582
2025 doi
-
[58]
Yuan, H.-B., Liu, X.-W., Huo, Z.-Y., et al. 2015, MNRAS, 448, 855, doi: 10.1093/mnras/stu2723 Evidence for the percentric passage of the Sagittarius dwarf galaxy 11 -2 -1 0 1 2 Z (kpc) 35 < < 15 15 < < 5 5 < < 0 -2 -1 0 1 2 Z (kpc) 35 < < 15 15 < < 5 5 < < 0 -2 -1 0 1 2 Z (kpc...
2015 doi
Reviewed August 6, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.