REVIEW 3 major objections 6 minor 1 cited by
The disrupting and growing open cluster spiral arm patterns of the Milky Way
T0 review · 3 major / 6 minor · reviewed 2026-08-10 · deepseek-v4-flash
Pith's one-line read The Milky Way's spiral arms are transient, multi-armed structures, not a fixed grand-design pattern.
desk verdict Larger-sample confirmation that Milky Way arms lack a steady age pattern, but the pattern-speed estimator needs a mock-recovery test before the transient-arm claim carries its full weight. 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 object is the open-cluster catalogue assembled from Gaia DR3, containing 5,866 clusters with ages from isochrone fitting, of which 2,692 are younger than 100 Myr and trace the arms. Cluster membership in each arm uses the adopted five-arm model with $\sigma$ boundaries adjusted to 1-, 2-, or 3-$\sigma$ where the 2-$\sigma$ strip fails. The age-pattern test compares the azimuthal positions of three age groups in $10^\circ$ bins, with bootstrap resampling and $\pm0.1$ dex age errors. The pattern-speed test uses the backward-orbit method: each cluster's birth position is retraced in the adopted Galactic potential, and the pattern speed that best aligns those birth positions with the present arm is selected; 1000 iterations propagate sample, age, distance, and velocity uncertainties. Finally, the vertex deviation $l_v$—the inclination of the velocity ellipsoid between radial and azimuthal motion—is computed for clusters younger than 300 Myr to diagnose whether each arm is growing or disrupting.
What would settle it
A targeted age-gradient survey of the Perseus arm: for open clusters between $R_{\mathrm{GC}} \approx 9.5$ and 11 kpc, bin ages in 10 Myr steps and measure their azimuthal offset from the arm center. Quasi-stationary density wave theory predicts a monotonic, systematically increasing offset with age (reversing at corotation), while the transient-arm picture predicts no ordered trend; a clean monotonic offset of 0.1–0.5 kpc would refute the paper's central claim.
Extended reading notes
Core claim
The paper's central claim is that the Milky Way's stellar disk does not host a grand-design spiral pattern with a single pattern speed. Using 2,692 open clusters younger than 100 Myr assigned to five arms from the adopted arm model, it compares the positions of clusters with ages <20 Myr, 20–50 Myr, and 50–100 Myr. Only the Sagittarius-Carina arm shows a significant young-to-old offset (0.1–0.5 kpc), and that offset does not grow with distance from corotation; the Local arm shows only a weak, direction-reversing offset, and the Perseus arm shows none. Retracing cluster orbits in the adopted Galactic potential yields pattern speeds $\Omega_p \approx 41$–47 (Scu-Cen), 29 (Sag-Car), 33–35 (Local), 16–21 (Perseus), and 31–46 $\mathrm{km\,s^{-1}\,kpc^{-1}}$ (Outer), broadly agreeing with prior studies and following the rotation curve rather than a single global speed. Vertex deviations for clusters younger than 300 Myr are negative in the Local arm and positive in Sag-Car and Perseus, which the paper interprets, in the dynamic-arm scenario, as growth and disruption respectively. The paper concludes that the arms are transient features that continuously emerge and dissipate.
Load-bearing premise
The load-bearing premise is that every cluster has been assigned to the correct spiral arm, using arm-boundary widths that are adjusted post hoc to 1-sigma or 3-sigma wherever the 2-sigma strip fails; if those boundaries misclassify clusters, the measured age patterns, pattern speeds, and vertex deviations—and with them the transient-arm conclusion—could change.
Editorial extensions
If this is right
- No single pattern speed: the Scu-Cen, Sag-Car, Local, and Perseus arms each rotate at a different rate, and, except for the poorly sampled Outer arm, those rates match the local circular speed.
- The Local arm is growing while the Sag-Car and Perseus arms are disrupting, so the disk is a multi-armed system whose arms continuously emerge and dissipate.
- Cluster ages within an arm are mixed, so the Sag-Car offset should not be read as evidence for steady density-wave flow.
- Any analysis that assumes one global pattern speed—for instance, to locate the corotation radius—will be misleading for the Milky Way.
- A larger cluster sample, especially for the Outer arm, is needed to decide whether its high pattern speed is real or an artifact of small numbers.
Reading between the lines
- An extension left implicit in the paper: if arms are transient and roughly corotating, then the age distribution inside an arm should become progressively more mixed with time, so young clusters should be the tightest tracers of the arm and older clusters should be progressively more scattered.
- The same reasoning could be applied to external galaxies: resolved stellar populations in flocculent or multi-armed galaxies should show weak or absent age gradients if transient arms are the general mechanism, whereas grand-design galaxies should show them.
- A quantitative prediction worth testing is that the fraction of clusters still sitting exactly on their birth arm should fall with age; measuring that decay rate would give a direct estimate of arm lifetime, which the paper does not attempt.
- If pattern speeds really track the rotation curve, the classical winding problem for the Milky Way disappears, and arm pitch angles should change over time; comparing arm pitch angles between young and older clusters could reveal such evolution.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper uses the largest available Gaia DR3 open-cluster catalogue (5,866 clusters) to test quasi-stationary density wave theory for the Milky Way's spiral arms. The authors examine the Galactocentric radial and azimuthal positions of clusters in three age groups (<20, 20–50, and 50–100 Myr) along five arms defined by the Reid et al. (2019) model, and report no systematic age pattern in the Local and Perseus arms, an offset in the Sagittarius-Carina arm that does not follow the predicted trend, and an overall 'absence of a theoretical age pattern.' They then derive pattern speeds for the arms using backward orbit integration in the MWPotential2014 model, following the Dias & Lépine (2005) method, and find values generally consistent with the rotation curve. Vertex deviations of clusters younger than 300 Myr are used to infer that the Local arm is growing, while the Sagittarius-Carina and Perseus arms are disrupting. The paper concludes that the Milky Way's spiral arms are transient, multi-armed structures rather than a grand-design pattern with a single pattern speed.
Significance. The paper's conclusion, if robust, would be an important observational constraint on spiral arm theory for the Milky Way, supporting transient-arm scenarios over quasi-stationary density waves. The analysis uses a substantially larger sample than previous works (threefold over the Gaia DR2 era) and includes a careful treatment of bootstrap and age uncertainties in the age-pattern analysis. The age-pattern null result is an independent observational test that does not rely on the pattern-speed fitting method. However, the pattern-speed measurement is not validated against a known input pattern speed, and the arm-membership boundaries are adjusted in a post hoc manner, so the quantitative support for the transient-arm conclusion is only as strong as these two steps. The paper also offers a new application of vertex deviation measurements to open clusters, which agrees with prior Cepheid-based results for the Perseus arm. With the requested validation and robustness checks, the paper could be a valuable contribution to the debate.
major comments (3)
- [Section 4, bullet list in 'SPIRAL ARM PATTERN SPEED'] The pattern-speed estimator as described may be circular. The method retraces the birthplace of each open cluster by backward orbit integration, rotates that birthplace by Ωp × age, and then compares the result with the contemporary spiral-arm configuration. If the comparison is effectively against the clusters' present-day positions (or if the arm model used in the comparison is the same Reid et al. (2019) model that defined the membership), the best-fitting Ωp is approximately the mean angular velocity of the clusters themselves, i.e., the rotation curve, rather than an independent property of the spiral pattern. The exact objective function is not stated. The manuscript should specify the objective function (or provide pseudo-code/equations) and validate the estimator with a mock catalog generated from a density-wave simulation with a known pattern speed, demonstrating that the method recovers the input pattern speed and not the rotation curve. Without such validation, the statement in the abstract that 'pattern speeds are consistent with the rotation curve' cannot be distinguished from an artifact of the fitting procedure, which is load-bearing for the transient-arm conclusion.
- [Section 3, first paragraph 'OC SPIRAL ARM AGE PATTERNS'] The assignment of open clusters to spiral arms uses sigma boundaries that are adjusted 'as necessary' to 1σ, 2σ, or 3σ. This is a post hoc, hypothesis-dependent choice: the boundaries determine exactly which clusters are included in the age-pattern and pattern-speed analyses. For example, the Sag-Car arm uses [-1, 1.5], which may exclude the 50–100 Myr clusters that are predicted to be offset from the arm center under quasi-stationary density wave theory, while the Perseus arm uses [-2, 3], which may include inter-arm clusters that dilute a genuine offset. The manuscript should adopt a fixed, pre-defined membership criterion (e.g., a common 2σ cutoff for all arms) and demonstrate that the qualitative conclusions (no ordered age pattern in the Local arm, no offset in the Perseus arm) are robust to reasonable variations in the sigma limits. If the asymmetric boundaries are necessary due to known spiral-arm geometry, the paper should justify each boundary choice with an objective rule rather than 'as necessary.'
- [Section 3 and Figure 2] The central null result—the absence of a theoretical age pattern—is not accompanied by a sensitivity or power analysis. The paper does not quantify the expected offset in the positions of 50–100 Myr clusters relative to <20 Myr clusters for a plausible quasi-stationary density wave (e.g., using the rotation curve and a pattern speed of 28.2 km s−1 kpc−1 as in Appendix A), nor the minimum offset that the current sample size, bin width (10°), and membership boundaries could detect. Without such a calculation, the failure to detect a systematic offset in the Local and Perseus arms may simply reflect limited statistical power, especially since the arms are only traced over ~30° segments. The paper should include a mock injection test or a simple analytic estimate of the expected age-dependent offset and show that the null result is meaningfully constraining for the density-wave hypothesis.
minor comments (6)
- [Section 4, bullet list] The sentence 'The present-day positions of the clusters are then compared across various pattern speeds with the contemporary spiral arm configuration' is grammatically unclear; it should state that the rotated birth positions are compared with the present-day arm model (as opposed to the clusters' present-day positions).
- [Table 1] Table 1 lists pattern speeds with uncertainties from sample, age, distance, and velocity, but it does not give the number of clusters used for each arm and each age range. Adding the sample sizes per arm and per age bin would aid reproducibility and help assess the reliability of the Outer-arm measurement.
- [Figure 3 caption] The figure caption should clarify which row of Table 1 is plotted (e.g., the sample-only case without the bar potential) and what the horizontal bars represent (the quoted radial range of clusters in each arm).
- [Section 6, first bullet] The conclusion states that the pattern speed of the Outer arm significantly exceeds the rotation curve, but earlier in Section 4 this is attributed to small sample size. The conclusion should carry the same caveat to avoid overstating the result.
- [Appendix A] The sketch map in Figure A1 uses a fixed pattern speed of 28.2 km s−1 kpc−1 and a fixed 50 Myr offset as an illustrative example; the text should explicitly state that this is a schematic, not a fit to the data.
- [Data Availability] The data availability statement says the data and simulation snapshots 'will be shared through a request to the corresponding author.' For a paper whose conclusions rest on a new large catalogue and dynamical simulations, a public repository or at least a detailed data description would improve reproducibility and is strongly recommended.
Circularity Check
Pattern-speed estimates in §4 are fitted cluster angular speeds, so the 'consistent with the rotation curve' claim is partly circular; the age-pattern and vertex-deviation analyses remain independent.
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fitted input called prediction
[Section 4, 'SPIRAL ARM PATTERN SPEED' bullet list]
"Assuming that OCs are born within spiral arms — implying that the birth position of each OC indicates the location of a spiral arm at the time of the OC’s formation — we retrace the birthplaces of star clusters in a specified segment of the arm, typically spanning less than 50-80 Myr. Assuming that the pattern of the spiral arm remains unchanged, we apply a range of pattern speeds to evolve these birthplace coordinates to their expected present-day position."
The alignment condition solved for each cluster is approximately θ_birth + Ωp·age ≈ θ_now, so the best-fit Ωp ≈ (θ_now − θ_birth)/age, i.e. the cluster's own mean orbital angular velocity. In the MWPotential2014 axisymmetric background this is essentially the circular speed, so the reported 'pattern speeds are consistent with the rotation curve' is a property of the estimator rather than an independent measurement of a spiral-arm pattern speed. The assumption that clusters are born in arms and the pattern remains unchanged forces the fitted Ωp to track the clusters' orbital motion; a quasi-stationary density wave, in which clusters drift through the arm, is excluded by construction.
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other
[Section 4, final paragraph and Section 6 conclusion]
"Moreover, aside from the Outer arm, the pattern speeds of the spiral arms are consistent with the Galactic rotation curve, indicating a more dynamic structure for the arms. ... The pattern speeds of the spiral arms, apart from the Local arm and Outer arm, decrease with increasing distance from the Galactic center."
This statement is used as evidence against quasi-stationary density wave theory, but the decrease with Galactocentric distance is the same decrease seen in the rotation curve, which the fitting procedure imprints by construction. The conclusion that the arms are 'dynamic' therefore borrows its quantitative support from the circular pattern-speed measurement, whereas the age-pattern and vertex-deviation analyses are independent tests that could stand on their own.
full rationale
The paper has two main quantitative pillars: the absence of a theoretical age pattern in open-cluster positions (§3) and pattern speeds consistent with the rotation curve (§4). The age-pattern analysis is an independent morphological test: it uses a pre-existing arm model (Reid et al. 2019) and compares positions of different-age clusters, with bootstrap and uncertainty propagation; this does not reduce to its inputs. The vertex-deviation analysis (§5) borrows its sign convention from an external N-body simulation calibration (F24), so it is also independent. However, the pattern-speed measurement in §4 is circular in the sense that the fitted Ωp is, for each cluster, essentially (θ_now − θ_birth)/age, the cluster's own mean angular speed. Reporting this as 'consistent with the rotation curve' and using that consistency as a falsification of quasi-stationary density wave theory is a fitted-input-called-prediction: the agreement is built into the estimator rather than being a test of the theory. The paper does not show that the method can recover a pattern speed different from the rotation curve in a controlled simulation with a known input pattern speed. Because one of the two central quantitative supports is circular, but the other is not, the overall circularity score is 6 rather than higher. There is no self-citation load-bearing chain and no imported uniqueness theorem; the circularity is confined to the pattern-speed procedure and its interpretive use.
Assumptions & free parameters
free parameters (3)
- Spiral arm membership boundaries (sigma ranges) =
[-3,2] Scu-Cen, [-1,1.5] Sag-Car, [-3,2] Local, [-2,3] Perseus, [-0.5,1] Outer
- Age uncertainty injection =
±0.1 dex random error
- Pattern speed age ranges =
10-50 Myr, 50-80 Myr, 10-80 Myr
assumptions (5)
- domain assumption Open clusters are born within spiral arms, so their birth positions trace the arm at formation time.
- domain assumption The MWPotential2014 model in Galpy accurately describes the Galactic gravitational potential for backward orbital integration.
- domain assumption The Reid et al. (2019) logarithmic spiral arm model correctly represents the current spiral arm locations.
- domain assumption Vertex deviation sign interpretation from Funakoshi et al. (2024) N-body simulations (positive = disruption, negative = growth) applies to open clusters.
- domain assumption The quasi-stationary density wave theory predictions (age gradients, fixed pattern speed) are correctly summarized.
Cite this review
Pith. "Pith review of The disrupting and growing open cluster spiral arm patterns of the Milky Way." pith.science (2026). https://pith.science/paper/V3CJXSXM
@misc{pith2026250114215,
author = {Pith},
title = {Pith review of: The disrupting and growing open cluster spiral arm patterns of the Milky Way},
year = {2026},
howpublished = {\url{https://pith.science/paper/V3CJXSXM}},
note = {Machine review of arXiv:2501.14215}
}
read the original abstract
Star clusters provide unique advantages for investigating Galactic spiral arms, particularly due to their precise ages, positions, and kinematic properties, which are further enhanced by ongoing updates from the astrometric data. In this study, we employ the latest extensive catalogue of open clusters from Gaia DR3 to examine the positional deviations of clusters belonging to different age groups. Additionally, we employ dynamical simulations to probe the evolutionary behavior of spiral arm positions. Our analysis reveals an absence of a theoretical age pattern in the spiral arms traced by open clusters, and the pattern speeds of the spiral arms are consistent with the rotation curve. Both of these results do not align with the predictions of quasi-stationary density wave theory, suggesting a more dynamic or transient arm scenario for the Milky Way. From this perspective, combined with vertex deviation estimates, it appears that the Local arm is in a state of growth. In contrast, the Sagittarius-Carina arm and the Perseus arm exhibit opposing trends. Consequently, we speculate that the Galactic stellar disk does not exhibit a grand-design spiral pattern with a fixed pattern speed, but rather manifests as a multi-armed structure with arms that continuously emerge and dissipate.
Figures
Figures from the paper (1 more)
Forward citations
Cited by 1 Pith paper
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The Galactic inner spiral arms revealed by the Gaia ESO Survey chemical abundances. Metallicity and [Mg/Fe] ratios
Chemical abundance excess maps from Gaia-ESO Survey data reveal enhanced [Fe/H] and depleted [Mg/Fe] along the Scutum and Sagittarius inner spiral arms.
Reference graph
Works this paper leans on
-
[1]
Am \^o res E. B., L \'e pine J. R. D., Mishurov Y. N., 2009, @doi [ ] 10.1111/j.1365-2966.2009.15611.x , https://ui.adsabs.harvard.edu/abs/2009MNRAS.400.1768A 400, 1768
arXiv 2009
-
[2]
Asano T., Kawata D., Fujii M. S., Baba J., 2024, @doi [ ] 10.1093/mnrasl/slad190 , https://ui.adsabs.harvard.edu/abs/2024MNRAS.529L...7A 529, L7
-
[3]
Baba J., Kawata D., Matsunaga N., Grand R. J. J., Hunt J. A. S., 2018, @doi [ ] 10.3847/2041-8213/aaa839 , https://ui.adsabs.harvard.edu/abs/2018ApJ...853L..23B 853, L23
-
[4]
Bovy J., 2015, @doi [ ] 10.1088/0067-0049/216/2/29 , https://ui.adsabs.harvard.edu/abs/2015ApJS..216...29B 216, 29
-
[5]
Bovy J., Rix H.-W., 2013, @doi [ ] 10.1088/0004-637X/779/2/115 , https://ui.adsabs.harvard.edu/abs/2013ApJ...779..115B 779, 115
-
[6]
Bressan A., Marigo P., Girardi L., Salasnich B., Dal Cero C., Rubele S., Nanni A., 2012, @doi [ ] 10.1111/j.1365-2966.2012.21948.x , https://ui.adsabs.harvard.edu/abs/2012MNRAS.427..127B 427, 127
arXiv 2012
-
[7]
Cantat-Gaudin T., et al., 2018, @doi [ ] 10.1051/0004-6361/201833476 , https://ui.adsabs.harvard.edu/abs/2018A&A...618A..93C 618, A93
-
[8]
Cantat-Gaudin T., et al., 2020, @doi [ ] 10.1051/0004-6361/202038192 , https://ui.adsabs.harvard.edu/abs/2020A&A...640A...1C 640, A1
Show all 70 references
-
[9]
Castro-Ginard A., et al., 2020, @doi [ ] 10.1051/0004-6361/201937386 , https://ui.adsabs.harvard.edu/abs/2020A&A...635A..45C 635, A45
2020 doi
-
[10]
Castro-Ginard A., et al., 2021, @doi [ ] 10.1051/0004-6361/202039751 , https://ui.adsabs.harvard.edu/abs/2021A&A...652A.162C 652, A162
2021 doi
-
[11]
Castro-Ginard A., et al., 2022, @doi [ ] 10.1051/0004-6361/202142568 , https://ui.adsabs.harvard.edu/abs/2022A&A...661A.118C 661, A118
2022 doi
-
[12]
Cheng X., Liu C., Mao S., Cui W., 2019, @doi [ ] 10.3847/2041-8213/ab020e , https://ui.adsabs.harvard.edu/abs/2019ApJ...872L...1C 872, L1
2019 doi
-
[13]
J., Williams B
Choi Y., Dalcanton J. J., Williams B. F., Weisz D. R., Skillman E. D., Fouesneau M., Dolphin A. E., 2015, @doi [ ] 10.1088/0004-637X/810/1/9 , https://ui.adsabs.harvard.edu/abs/2015ApJ...810....9C 810, 9
2015 doi
-
[14]
S., Cong H., Dame T
Cohen R. S., Cong H., Dame T. M., Thaddeus P., 1980, @doi [ ] 10.1086/183290 , https://ui.adsabs.harvard.edu/abs/1980ApJ...239L..53C 239, L53
1980 doi
-
[15]
M., Thaddeus P., 2011, @doi [ ] 10.1088/2041-8205/734/1/L24 , https://ui.adsabs.harvard.edu/abs/2011ApJ...734L..24D 734, L24
Dame T. M., Thaddeus P., 2011, @doi [ ] 10.1088/2041-8205/734/1/L24 , https://ui.adsabs.harvard.edu/abs/2011ApJ...734L..24D 734, L24
2011 doi
-
[16]
Dehnen W., 1999, @doi [ ] 10.1086/312299 , https://ui.adsabs.harvard.edu/abs/1999ApJ...524L..35D 524, L35
1999 doi
-
[17]
S., L \'e pine J
Dias W. S., L \'e pine J. R. D., 2005, @doi [ ] 10.1086/431456 , https://ui.adsabs.harvard.edu/abs/2005ApJ...629..825D 629, 825
2005 doi
-
[18]
S., Monteiro H., L \'e pine J
Dias W. S., Monteiro H., L \'e pine J. R. D., Barros D. A., 2019, @doi [ ] 10.1093/mnras/stz1196 , https://ui.adsabs.harvard.edu/abs/2019MNRAS.486.5726D 486, 5726
2019 doi
-
[19]
Dobbs C., Baba J., 2014, @doi [ ] 10.1017/pasa.2014.31 , https://ui.adsabs.harvard.edu/abs/2014PASA...31...35D 31, e035
2014 doi
- [21]
-
[22]
Gaia Collaboration et al., 2018, @doi [ ] 10.1051/0004-6361/201833051 , https://ui.adsabs.harvard.edu/abs/2018A&A...616A...1G 616, A1
2018 doi
-
[23]
Gaia Collaboration et al., 2021, @doi [ ] 10.1051/0004-6361/202039657 , https://ui.adsabs.harvard.edu/abs/2021A&A...649A...1G 649, A1
2021 doi
-
[24]
Gaia Collaboration et al., 2023, @doi [ ] 10.1051/0004-6361/202243797 , https://ui.adsabs.harvard.edu/abs/2023A&A...674A..37G 674, A37
2023 doi
-
[25]
C., Harding P., Garner C
Garner R., Mihos J. C., Harding P., Garner C. R., 2024, @doi [ ] 10.3847/1538-4357/ad0e63 , https://ui.adsabs.harvard.edu/abs/2024ApJ...961..217G 961, 217
2024 doi
-
[26]
M., Georgelin Y
Georgelin Y. M., Georgelin Y. P., 1976, , https://ui.adsabs.harvard.edu/abs/1976A&A....49...57G 49, 57
1976
-
[27]
Goldreich P., Tremaine S., 1978, @doi [ ] 10.1086/156203 , https://ui.adsabs.harvard.edu/abs/1978ApJ...222..850G 222, 850
1978 doi
-
[28]
He Z., 2023, @doi [ ] 10.3847/2041-8213/ace77d , https://ui.adsabs.harvard.edu/abs/2023ApJ...954L...9H 954, L9
2023 doi
-
[29]
He Z.-H., Xu Y., Hou L.-G., 2021a, @doi [Research in Astronomy and Astrophysics] 10.1088/1674-4527/21/1/9 , https://ui.adsabs.harvard.edu/abs/2021RAA....21....9H 21, 009
-
[30]
He Z.-H., Xu Y., Hao C.-J., Wu Z.-Y., Li J.-J., 2021b, @doi [Research in Astronomy and Astrophysics] 10.1088/1674-4527/21/4/93 , https://ui.adsabs.harvard.edu/abs/2021RAA....21...93H 21, 093
-
[31]
He Z., et al., 2022a, @doi [ ] 10.3847/1538-4365/ac5cbb , https://ui.adsabs.harvard.edu/abs/2022ApJS..260....8H 260, 8
-
[32]
He Z., Wang K., Luo Y., Li J., Liu X., Jiang Q., 2022b, @doi [ ] 10.3847/1538-4365/ac7c17 , https://ui.adsabs.harvard.edu/abs/2022ApJS..262....7H 262, 7
-
[33]
He Z., Liu X., Luo Y., Wang K., Jiang Q., 2023a, @doi [ ] 10.3847/1538-4365/ac9af8 , https://ui.adsabs.harvard.edu/abs/2023ApJS..264....8H 264, 8
-
[34]
He Z., Luo Y., Wang K., Ren A., Peng L., Cui Q., Liu X., Jiang Q., 2023b, @doi [ ] 10.3847/1538-4365/acd6fa , https://ui.adsabs.harvard.edu/abs/2023ApJS..267...34H 267, 34
-
[35]
G., Han J
Hou L. G., Han J. L., 2014, @doi [ ] 10.1051/0004-6361/201424039 , https://ui.adsabs.harvard.edu/abs/2014A&A...569A.125H 569, A125
2014 doi
-
[36]
G., Han J
Hou L. G., Han J. L., 2015, @doi [ ] 10.1093/mnras/stv1904 , https://ui.adsabs.harvard.edu/abs/2015MNRAS.454..626H 454, 626
2015 doi
-
[37]
L., Reffert S., 2021, @doi [ ] 10.1051/0004-6361/202039341 , https://ui.adsabs.harvard.edu/abs/2021A&A...646A.104H 646, A104
Hunt E. L., Reffert S., 2021, @doi [ ] 10.1051/0004-6361/202039341 , https://ui.adsabs.harvard.edu/abs/2021A&A...646A.104H 646, A104
2021 doi
-
[38]
L., Reffert S., 2023, @doi [ ] 10.1051/0004-6361/202346285 , https://ui.adsabs.harvard.edu/abs/2023A&A...673A.114H 673, A114
Hunt E. L., Reffert S., 2023, @doi [ ] 10.1051/0004-6361/202346285 , https://ui.adsabs.harvard.edu/abs/2023A&A...673A.114H 673, A114
2023 doi
-
[39]
C., Malhotra S., 2023, @doi [ ] 10.3847/1538-3881/acf7c8 , https://ui.adsabs.harvard.edu/abs/2023AJ....166..170J 166, 170
Joshi Y. C., Malhotra S., 2023, @doi [ ] 10.3847/1538-3881/acf7c8 , https://ui.adsabs.harvard.edu/abs/2023AJ....166..170J 166, 170
2023 doi
-
[40]
Katz D., et al., 2023, @doi [ ] 10.1051/0004-6361/202244220 , https://ui.adsabs.harvard.edu/abs/2023A&A...674A...5K 674, A5
2023 doi
-
[41]
G., 2020, @doi [ ] 10.3847/1538-3881/abc0e6 , https://ui.adsabs.harvard.edu/abs/2020AJ....160..279K 160, 279
Kounkel M., Covey K., Stassun K. G., 2020, @doi [ ] 10.3847/1538-3881/abc0e6 , https://ui.adsabs.harvard.edu/abs/2020AJ....160..279K 160, 279
2020 doi
-
[42]
S., Blitz L., Heiles C., 2006, @doi [Science] 10.1126/science.1128455 , https://ui.adsabs.harvard.edu/abs/2006Sci...312.1773L 312, 1773
Levine E. S., Blitz L., Heiles C., 2006, @doi [Science] 10.1126/science.1128455 , https://ui.adsabs.harvard.edu/abs/2006Sci...312.1773L 312, 1773
2006 doi
-
[43]
C., Shu F
Lin C. C., Shu F. H., 1964, @doi [ ] 10.1086/147955 , https://ui.adsabs.harvard.edu/abs/1964ApJ...140..646L 140, 646
1964 doi
-
[44]
C., Shu F
Lin C. C., Shu F. H., 1966, @doi [Proceedings of the National Academy of Science] 10.1073/pnas.55.2.229 , https://ui.adsabs.harvard.edu/abs/1966PNAS...55..229L 55, 229
1966 doi
-
[45]
Lin Z., Xu Y., Hou L., Liu D., Li Y., Hao C., Li J., Bian S., 2022, @doi [ ] 10.3847/1538-4357/ac67a6 , https://ui.adsabs.harvard.edu/abs/2022ApJ...931...72L 931, 72
2022 doi
-
[46]
Liu L., Pang X., 2019, @doi [ ] 10.3847/1538-4365/ab530a , https://ui.adsabs.harvard.edu/abs/2019ApJS..245...32L 245, 32
2019 doi
-
[47]
A., L \'e pine J
Michtchenko T. A., L \'e pine J. R. D., P \'e rez-Villegas A., Vieira R. S. S., Barros D. A., 2018, @doi [ ] 10.3847/2041-8213/aad804 , https://ui.adsabs.harvard.edu/abs/2018ApJ...863L..37M 863, L37
2018 doi
-
[48]
Monari G., Famaey B., Siebert A., Grand R. J. J., Kawata D., Boily C., 2016, @doi [ ] 10.1093/mnras/stw1564 , https://ui.adsabs.harvard.edu/abs/2016MNRAS.461.3835M 461, 3835
2016 doi
-
[49]
W., Whitford A
Morgan W. W., Whitford A. E., Code A. D., 1953, @doi [ ] 10.1086/145754 , https://ui.adsabs.harvard.edu/abs/1953ApJ...118..318M 118, 318
1953 doi
-
[50]
G., Merrifield M
Peterken T. G., Merrifield M. R., Arag \'o n-Salamanca A., Drory N., Krawczyk C. M., Masters K. L., Weijmans A.-M., Westfall K. B., 2019, @doi [Nature Astronomy] 10.1038/s41550-018-0627-5 , https://ui.adsabs.harvard.edu/abs/2019NatAs...3..178P 3, 178
2019 doi
-
[51]
J., et al., 2019, @doi [ ] 10.3847/1538-4357/ab4a11 , https://ui.adsabs.harvard.edu/abs/2019ApJ...885..131R 885, 131
Reid M. J., et al., 2019, @doi [ ] 10.3847/1538-4357/ab4a11 , https://ui.adsabs.harvard.edu/abs/2019ApJ...885..131R 885, 131
2019 doi
-
[52]
W., 1969, @doi [ ] 10.1086/150177 , https://ui.adsabs.harvard.edu/abs/1969ApJ...158..123R 158, 123
Roberts W. W., 1969, @doi [ ] 10.1086/150177 , https://ui.adsabs.harvard.edu/abs/1969ApJ...158..123R 158, 123
1969 doi
-
[53]
A., 2011, @doi [ ] 10.1111/j.1365-2966.2010.17545.x , https://ui.adsabs.harvard.edu/abs/2011MNRAS.410.1637S 410, 1637
Sellwood J. A., 2011, @doi [ ] 10.1111/j.1365-2966.2010.17545.x , https://ui.adsabs.harvard.edu/abs/2011MNRAS.410.1637S 410, 1637
2011
-
[54]
A., Carlberg R
Sellwood J. A., Carlberg R. G., 1984, @doi [ ] 10.1086/162176 , https://ui.adsabs.harvard.edu/abs/1984ApJ...282...61S 282, 61
1984 doi
-
[55]
A., Carlberg R
Sellwood J. A., Carlberg R. G., 2014, @doi [ ] 10.1088/0004-637X/785/2/137 , https://ui.adsabs.harvard.edu/abs/2014ApJ...785..137S 785, 137
2014 doi
-
[56]
A., Carlberg R
Sellwood J. A., Carlberg R. G., 2019, @doi [ ] 10.1093/mnras/stz2132 , https://ui.adsabs.harvard.edu/abs/2019MNRAS.489..116S 489, 116
2019 doi
-
[57]
Shabani F., et al., 2018, @doi [ ] 10.1093/mnras/sty1277 , https://ui.adsabs.harvard.edu/abs/2018MNRAS.478.3590S 478, 3590
2018 doi
-
[58]
H., 2016, @doi [ ] 10.1146/annurev-astro-081915-023426 , https://ui.adsabs.harvard.edu/abs/2016ARA&A..54..667S 54, 667
Shu F. H., 2016, @doi [ ] 10.1146/annurev-astro-081915-023426 , https://ui.adsabs.harvard.edu/abs/2016ARA&A..54..667S 54, 667
2016 doi
-
[59]
H., Milione V., Roberts William W
Shu F. H., Milione V., Roberts William W. J., 1973, @doi [ ] 10.1086/152270 , https://ui.adsabs.harvard.edu/abs/1973ApJ...183..819S 183, 819
1973 doi
-
[60]
H., Ann H
Sim G., Lee S. H., Ann H. B., Kim S., 2019, @doi [Journal of Korean Astronomical Society] 10.5303/JKAS.2019.52.5.145 , https://ui.adsabs.harvard.edu/abs/2019JKAS...52..145S 52, 145
2019 doi
-
[61]
T., Shen J., Koposov S
Simion I. T., Shen J., Koposov S. E., Ness M., Freeman K., Bland-Hawthorn J., Lewis G. F., 2021, @doi [ ] 10.1093/mnras/stab073 , https://ui.adsabs.harvard.edu/abs/2021MNRAS.502.1740S 502, 1740
2021 doi
-
[62]
M., et al., 2019, @doi [Science] 10.1126/science.aau3181 , https://ui.adsabs.harvard.edu/abs/2019Sci...365..478S 365, 478
Skowron D. M., et al., 2019, @doi [Science] 10.1126/science.aau3181 , https://ui.adsabs.harvard.edu/abs/2019Sci...365..478S 365, 478
2019 doi
-
[63]
Sun Y., Xu Y., Yang J., Li F.-C., Du X.-Y., Zhang S.-B., Zhou X., 2015, @doi [ ] 10.1088/2041-8205/798/2/L27 , https://ui.adsabs.harvard.edu/abs/2015ApJ...798L..27S 798, L27
2015 doi
-
[64]
V., Nikiforov I., 2020, @doi [Research in Astronomy and Astrophysics] 10.1088/1674-4527/20/12/209 , https://ui.adsabs.harvard.edu/abs/2020RAA....20..209V 20, 209
Veselova A. V., Nikiforov I., 2020, @doi [Research in Astronomy and Astrophysics] 10.1088/1674-4527/20/12/209 , https://ui.adsabs.harvard.edu/abs/2020RAA....20..209V 20, 209
2020 doi
-
[65]
I., Theis C., 2008, @doi [ ] 10.1111/j.1365-2966.2007.12476.x , https://ui.adsabs.harvard.edu/abs/2008MNRAS.383..817V 383, 817
Vorobyov E. I., Theis C., 2008, @doi [ ] 10.1111/j.1365-2966.2007.12476.x , https://ui.adsabs.harvard.edu/abs/2008MNRAS.383..817V 383, 817
2008
-
[66]
R., 2011, @doi [ ] 10.1088/0004-637X/735/1/1 , https://ui.adsabs.harvard.edu/abs/2011ApJ...735....1W 735, 1
Wada K., Baba J., Saitoh T. R., 2011, @doi [ ] 10.1088/0004-637X/735/1/1 , https://ui.adsabs.harvard.edu/abs/2011ApJ...735....1W 735, 1
2011 doi
-
[67]
Xu Y., et al., 2016, @doi [Science Advances] 10.1126/sciadv.1600878 , https://ui.adsabs.harvard.edu/abs/2016SciA....2E0878X 2, e1600878
2016 doi
-
[68]
Xu Y., et al., 2018, @doi [ ] 10.1051/0004-6361/201833407 , https://ui.adsabs.harvard.edu/abs/2018A&A...616L..15X 616, L15
2018 doi
-
[69]
J., Liu D
Xu Y., Hao C. J., Liu D. J., Lin Z. H., Bian S. B., Hou L. G., Li J. J., Li Y. J., 2023, @doi [ ] 10.3847/1538-4357/acc45c , https://ui.adsabs.harvard.edu/abs/2023ApJ...947...54X 947, 54
2023 doi
-
[70]
C., 2018, @doi [ ] 10.3847/1538-4357/aaeacd , https://ui.adsabs.harvard.edu/abs/2018ApJ...869...29Y 869, 29
Yu S.-Y., Ho L. C., 2018, @doi [ ] 10.3847/1538-4357/aaeacd , https://ui.adsabs.harvard.edu/abs/2018ApJ...869...29Y 869, 29
2018 doi
-
[71]
N., Rich R
Zhao H., Spergel D. N., Rich R. M., 1994, @doi [ ] 10.1086/117227 , https://ui.adsabs.harvard.edu/abs/1994AJ....108.2154Z 108, 2154
1994 doi
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