REVIEW 2 major objections 6 minor 31 references
Gas found floating above a Milky Way-like galaxy's disk
Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →
2026-07-09 22:59 UTC pith:MVGJKK2X
load-bearing objection Real detection of off-plane CO in NGC 4565, but the inflow interpretation rests on an unresolved velocity-component degeneracy. the 2 major comments →
A CO detection in the off-plane region of the edge-on galaxy NGC 4565 with the Nobeyama 45-m telescope
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Molecular gas is detected at kiloparsec heights above the disk of NGC 4565, a normal non-starburst galaxy. The off-plane CO intensity fraction (~0.34) exceeds what geometrically thin-disk models can produce through projection alone, requiring genuinely elevated gas. A subset of this gas moves at velocities offset by ~100 km/s from local disk rotation, carrying kinetic energy (~10^54 erg) that is hard to attribute to disk-driven feedback alone.
What carries the argument
The argument rests on three linked pieces: (1) CO detections at off-plane positions that exceed conservative beam-pattern contamination limits, (2) forward modelling with 3D-BAROLO showing that thin-disk projection at i ≈ 88.5° cannot reproduce the observed off-plane fraction, and (3) an energy argument showing that the high-velocity component's kinetic energy (~10^54 erg) would require ~10^4 supernovae concentrated in a single ~1 kpc beam, which is implausible for a galaxy with NGC 4565's star formation rate.
Load-bearing premise
The beam-pattern contamination estimate relies on scaling an 86 GHz beam measurement to 115 GHz by the beam-size ratio, because no dedicated 115 GHz beam pattern was measured. If the actual 115 GHz sidelobe response is higher than the adopted 20% limit, the off-plane detections could be partially or fully explained by disk emission leaking through the telescope beam.
What would settle it
A dedicated 115 GHz beam-pattern measurement showing sidelobe responses above 20% at one-beam offsets would reduce or eliminate the OP1–OP3 detections as genuine off-plane signals, undermining the entire chain of argument.
If this is right
- If molecular gas at kpc heights is common in normal disk galaxies, it represents a reservoir for disk replenishment that is currently missing from galaxy evolution models.
- The high-velocity component, if confirmed as inflow, would provide direct observational evidence for cold accretion in a Milky Way analogue, constraining how galaxies sustain star formation over cosmic time.
- Wide-field CO surveys of edge-on galaxies could determine whether thick molecular layers are ubiquitous or restricted to specific environments like dust filaments.
- Comparison with face-on galaxy surveys (e.g., M83 HVCs) could test whether the same population of high-velocity molecular clouds is seen from both viewing angles.
- If the CO-to-H2 conversion factor is higher for off-plane gas than for disk gas, the inferred molecular masses would increase proportionally, strengthening the energy budget argument.
Where Pith is reading between the lines
- The detection is limited to one field targeting a dust filament; a galaxy-wide thick molecular disk is not established. If the filament is atypical, the result may represent a local phenomenon rather than a general property of disk galaxies.
- The projected spiral-arm crossing explanation for the high-velocity component is acknowledged but not quantitatively ruled out. If the galaxy's spiral structure produces velocity offsets comparable to 100 km/s at this inclination, the inflow interpretation weakens.
- The energy argument assumes the full high-velocity mass moves coherently at 100 km/s; if the gas is a superposition of smaller clouds with a range of velocities, the kinetic energy could be overestimated.
- Interferometric follow-up at higher angular resolution could resolve whether the off-plane gas forms a coherent structure (supporting inflow or fountain) or is a collection of unrelated clouds (weakening a single-origin interpretation).
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This letter reports the detection of 12CO(J=1-0) emission at three off-plane positions (z ~ 0.85 kpc) in the edge-on galaxy NGC 4565, using Nobeyama 45-m observations. The authors evaluate beam-pattern contamination and projection effects, concluding that the off-plane emission cannot be explained solely by a geometrically thin disk. They identify a high-velocity component offset by ~100 km/s from local disk rotation, estimate its kinetic energy at ~10^54 erg, and argue that disk-driven feedback is energetically insufficient, making external inflow a possible origin. The paper is clearly written and addresses the two main confounds (beam contamination and projection) with reasonable methods. The central detection claim at OP1-OP3 appears robust under the authors' conservative contamination limits.
Significance. The paper presents a genuine detection of off-plane molecular gas in a non-starburst, Milky Way-like edge-on galaxy, which is observationally valuable and adds to a small but growing sample. The forward-modeling approach using 3D-BAROLO to quantify projection effects is a methodological strength. The quantitative energy argument, while subject to the degeneracy discussed below, provides a falsifiable framework for distinguishing feedback from inflow. The comparison to M83 HVCs (Nagata et al. 2025) is well-placed and contextualizes the result within the emerging picture of off-plane molecular gas in normal galaxies.
major comments (2)
- §4.3, Eq. (7): The E_kin ~ 10^54 erg argument and the inflow interpretation rest on the high-velocity component being physically distinct gas rather than projected spiral-arm emission. The authors acknowledge this degeneracy ('a projected spiral-arm crossing could also contribute to this velocity-offset emission') but do not attempt to resolve or even bound it. This is load-bearing for two reasons: (1) the E_kin calculation is the primary quantitative evidence against feedback and for inflow; if ΔV ~ 100 km/s is a projection artifact rather than a physical bulk velocity, Eq. (7) is invalid. (2) The high-velocity component contributes roughly 40% of the off-plane emission (f_off drops from 0.34 to 0.20 when excluded, §4.2), so its interpretation also affects the 'thick molecular disk' claim. The authors should either provide a quantitative test (e.g., can a spiral-arm model at i=88.5° and
- §4.3: The 'high-velocity component' is defined observationally as CO emission outside v_pk,GP ± 50 km/s. This window width is not physically motivated — it appears to be chosen to capture the main disk component in the GP spectra. If the window were ±75 or ±100 km/s, the inferred M_HV and E_kin would change substantially. The authors should justify this choice or, at minimum, demonstrate that their conclusions are robust to reasonable variations in the window width (e.g., ±40 to ±80 km/s). As it stands, a key derived quantity depends on an unexamined parameter.
minor comments (6)
- §2: The use of an 11th-order polynomial baseline with visual inspection for line-free channel selection is acknowledged as subjective. The authors state they repeated the process and confirmed reproducibility, which is good. It would strengthen the paper to briefly note the typical change in W_CO between different reasonable baseline choices, to quantify this subjectivity.
- §4.1: The beam pattern is scaled from 86 GHz to 115 GHz by FWHM ratio. The authors adopt conservative contamination limits (20% at one-beam offsets). This is a reasonable approach given the lack of 115 GHz measurements, but the paper could note whether the FOREST beam pattern is expected to scale simply with frequency, or whether additional structure might appear.
- Table 2: The molecular mass uncertainties include only statistical uncertainties propagated from W_CO. Given that α_CO dominates the systematic uncertainty and may differ for off-plane gas (as discussed in §3.1), a brief note in the table caption reminding the reader of this would be useful.
- Figure 3: The horizontal positions of the red crosses and blue triangles are described as scale heights inferred by matching to the i=88.5° model. It would help to label these inferred z_0 values on the figure or in the caption, so the reader can directly read off the required scale heights for the observed f_off values (0.22-0.44).
- §4.2: The statement 'reproducing the largest observed value, f_off,2 = 0.44, within this inclined disk model requires a scale height of ~0.9 kpc' is used to argue against a thin disk. However, the mean f_off = 0.34 requires z_0 ~ 0.5 kpc, which is already large but less dramatic. The paper should clarify whether the argument against a thin disk rests primarily on the mean or on the outlier.
- The reference 'Jiménez-López et al. 2026' (arXiv:2603.06913) appears to be a future-dated preprint. The authors should verify the citation details and update if a published version is available.
Circularity Check
No circularity found; derivation chain is self-contained with external benchmarks
full rationale
The paper's derivation chain is straightforward and non-circular. (1) The CO detections at OP1–OP3 are direct observational measurements, with beam-contamination estimates derived from an externally measured beam pattern (Minamidani et al. 2016), not from the paper's own data. (2) The molecular mass M_mol uses α_CO = 4.35 adopted from Bolatto et al. (2013), an external citation. (3) The thin-disk forward models (§4.2) use 3D-BAROLO GALMOD with geometry and kinematics fixed from literature values (Table 1), not fitted to the off-plane data; the observed f_off values are compared against model predictions, which is standard forward modeling. (4) The high-velocity component is defined observationally (emission outside v_pk,GP ± 50 km/s), and E_kin = ½ M_HV ΔV² (Eq. 7) is a direct application of the standard kinetic energy formula with measured quantities. The citation to Nagata et al. (2025) — which shares some co-authors — is for the methodology of applying this formula to HVCs and for comparative discussion of M83, not for a uniqueness theorem or an unverified ansatz. The ±50 km/s window choice and the spiral-arm degeneracy are acknowledged by the authors as interpretation limitations, but these are correctness/robustness concerns, not circularity: no step in the derivation reduces to its own inputs by construction.
Axiom & Free-Parameter Ledger
free parameters (4)
- α_CO =
4.35 M_sun (K km/s pc^2)^-1
- Contamination limits (beam pattern) =
20% at one-beam offset, 10% at two-beam offset
- Local disk velocity window width =
±50 km/s around v_pk,GP
- R_mol / R_25 =
0.7
axioms (3)
- domain assumption The CO-to-H2 conversion factor α_CO is the same for off-plane gas as for disk gas.
- domain assumption The 86 GHz FOREST beam pattern, when scaled by FWHM ratio, is a valid approximation for the 115 GHz beam pattern.
- ad hoc to paper The high-velocity component is not dominated by projected spiral-arm crossing emission.
Cite this review
Pith. "Pith review of A CO detection in the off-plane region of the edge-on galaxy NGC 4565 with the Nobeyama 45-m telescope." pith.science (2026). https://pith.science/paper/MVGJKK2X
@misc{pith2026260706914,
author = {Pith},
title = {Pith review of: A CO detection in the off-plane region of the edge-on galaxy NGC 4565 with the Nobeyama 45-m telescope},
year = {2026},
howpublished = {\url{https://pith.science/paper/MVGJKK2X}},
note = {Machine review of arXiv:2607.06914}
}
read the original abstract
Understanding the cycling of interstellar medium (ISM) between the galactic plane and off-plane regions is crucial for tracing the evolution of disk galaxies. We present $^{12}$CO($J=1-0$) multi-pointing observations of the edge-on, Milky Way-like galaxy NGC 4565 obtained with the Nobeyama 45-m telescope, with an angular resolution of 14 arcsec, corresponding to about 0.8 kpc. Along a prominent dust filament, we detect significant CO emission at three off-plane positions above the galactic plane. After evaluating possible beam-pattern contamination, the detections remain robust. The derived per-beam molecular masses are $M_{\rm mol} \simeq (2.1-4.3) \times 10^7 M_\odot$. While the off-plane spectra show broader effective line widths, $\sigma_{\rm eff}=83-115$ km s$^{-1}$, than the disk spectra, they contain CO components consistent with the local disk rotation. The mean observed off-plane CO intensity fraction is about 0.34. Comparison with geometrically thin-disk models suggests that this large fraction is best explained by gas above the disk. The large $\sigma_{\rm eff}$ values are partly attributable to a high-velocity component with molecular gas mass $M_{\rm mol}^{\rm HV} \sim 10^7 M_\odot$ that is offset by about 100 km s$^{-1}$ from the local disk velocity. The kinetic energy of this component is estimated to be $E_{\rm kin} \sim 10^{54}$ erg. Such a large energy requirement is difficult to explain by disk-driven feedback in NGC 4565, which has a Milky Way-like star formation rate. External inflow is therefore one possibility.
Figures
Reference graph
Works this paper leans on
- [1]
-
[2]
Bolatto, A. D., Wolfire, M., & Leroy, A. K. 2013, ARA&A, 51, 207 Caldú-Primo, A., Schruba, A., Walter, F., et al. 2013, AJ, 146, 150
work page 2013
-
[3]
Chen, B.-Q., Liu, X.-W., Yuan, H.-B., Huang, Y ., & Xiang, M.-S. 2015, MNRAS, 448, 2187
work page 2015
-
[4]
Chevalier, R. A. 1974, ApJ, 188, 501
work page 1974
-
[5]
Cormier, D., Bigiel, F., Wang, J., et al. 2016, MNRAS, 463, 1724
work page 2016
- [6]
-
[7]
2007, A&A, 473, 863 Di Teodoro, E
Dessauges-Zavadsky, M., Combes, F., & Pfenniger, D. 2007, A&A, 473, 863 Di Teodoro, E. M., & Fraternali, F. 2015, MNRAS, 451, 3021
work page 2007
-
[8]
Garcia-Burillo, S., Guelin, M., Cernicharo, J., & Dahlem, M. 1992, A&A, 266, 21
work page 1992
- [9]
-
[10]
Huchtmeier, W. K., Seiradakis, J. H., & Tammann, G. A. 1980, A&A, 89, 95
work page 1980
-
[11]
Irwin, J., Beck, R., Benjamin, R. A., et al. 2012, AJ, 144, 43 Jiménez-López, D., García-Burillo, S., Querejeta, M., Usero, A., & Tarrío, P. 2026, arXiv e-prints, arXiv:2603.06913
work page internal anchor Pith review arXiv 2012
-
[12]
Kalberla, P. M. W., McClure-Griffiths, N. M., Pisano, D. J., et al. 2010, A&A, 521, A17
work page 2010
-
[13]
Kamazaki, T., Okumura, S. K., Chikada, Y ., et al. 2012, PASJ, 64, 29
work page 2012
-
[14]
Kissler-Patig, M., Ashman, K. M., Zepf, S. E., & Freeman, K. C. 1999, AJ, 118, 197
work page 1999
- [15]
-
[16]
K., Walter, F., Martini, P., et al
Leroy, A. K., Walter, F., Martini, P., et al. 2015, ApJ, 814, 83
work page 2015
-
[17]
Lilly, S. J., Carollo, C. M., Pipino, A., Renzini, A., & Peng, Y . 2013, ApJ, 772, 119 Martínez-Lombilla, C., Infante-Sainz, R., Jiménez-Ibarra, F., et al. 2023, A&A, 678, A62 Martínez-Lombilla, C., Trujillo, I., & Knapen, J. H. 2019, MNRAS, 483, 664
work page 2013
-
[18]
2016, in Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series, V ol
Minamidani, T., Nishimura, A., Miyamoto, Y ., et al. 2016, in Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series, V ol. 9914, Millimeter, Submillimeter, and Far-Infrared Detectors and Instrumentation for Astronomy VIII, ed. W. S. Holland & J. Zmuidzinas, 99141Z
work page 2016
-
[19]
Mosenkov, A., Rich, R. M., Koch, A., et al. 2020, MNRAS, 494, 1751
work page 2020
- [20]
-
[21]
Nakamura, F., Ogawa, H., Yonekura, Y ., et al. 2015, PASJ, 67, 117
work page 2015
-
[22]
Nakamura, F., Chiong, C.-C., Taniguchi, K., et al. 2024, PASJ, 76, 563
work page 2024
- [23]
-
[24]
Radburn-Smith, D. J., de Jong, R. S., Seth, A. C., et al. 2011, ApJS, 195, 18
work page 2011
-
[25]
Rossa, J., & Dettmar, R. J. 2000, A&A, 359, 433
work page 2000
-
[26]
Sancisi, R., Fraternali, F., Oosterloo, T., & van der Hulst, T. 2008, A&AR, 15, 189
work page 2008
- [27]
-
[28]
Ulich, B. L., & Haas, R. W. 1976, ApJS, 30, 247 van de Sande, J., Fraser-McKelvie, A., Fisher, D. B., et al. 2024, in IAU
work page 1976
- [29]
-
[30]
Zheng, Y ., Wang, J., Irwin, J., et al. 2022, MNRAS, 513, 1329
work page 2022
-
[31]
Zschaechner, L. K., Rand, R. J., Heald, G. H., Gentile, G., & Józsa, G. 2012, ApJ, 760, 37
work page 2012
This paper was first reviewed by glm-5.2 on July 9, 2026.
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.