Signatures of coronal mass ejections in differential emission measure analysis of the Sun as a star
Pith reviewed 2026-05-14 23:57 UTC · model grok-4.3
The pith
Coronal dimmings from CMEs appear in Sun-as-a-star differential emission measures.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
For all sixteen eruptive flares, dimmings occur in the 171, 193, and 211 angstrom channels, with the DEM decreasing relative to pre-flare values in the 10^{5.7} to 10^{6.3} K range. The dimming signature is stronger in lower temperatures without correction and shifts to higher temperatures with the gradual-phase correction. Comparisons with EVE spectra and resolved AIA data for one event yield similar temperature ranges where the drop is prominent.
What carries the argument
Differential emission measure derived from full-disk averages of six SDO/AIA EUV channels, tracking changes in plasma temperature distribution during flare-associated dimmings.
If this is right
- Intensity decreases become more pronounced after subtracting the gradual phase contribution from the light curves.
- The DEM drop is most evident between 10^{5.7} and 10^{6.0} K without correction and 10^{6.0} to 10^{6.3} K with correction.
- Similar dimming temperature ranges appear in both EVE and spatially resolved AIA data for a test event.
- The magnitude of the dimming is larger in resolved observations than in full-disk averages.
Where Pith is reading between the lines
- Full-disk DEM monitoring could allow detection of CMEs on other stars by looking for similar temperature-specific emission drops during flares.
- Accounting for gradual phase evolution is necessary to avoid underestimating the mass loss associated with eruptions.
- Line-of-sight integration in full-disk data does not erase the dimming signal, suggesting robustness for stellar applications.
Load-bearing premise
The intensity drops result from actual mass ejection rather than other flare-induced changes in coronal structure or from biases in the DEM inversion process using only six broad channels.
What would settle it
A confirmed eruptive flare showing no decrease in DEM within the 10^{5.7}-10^{6.3} K range, or the same pattern appearing equally in non-CME flares.
Figures
read the original abstract
We investigated if signatures of coronal mass ejections (CMEs) can be retrieved in the differential emission measure (DEM) from Sun-as-a-star extreme-ultraviolet (EUV) observations. We analyzed 16 major, eruptive (i.e., associated with CMEs) flares. For each flare we constructed light curves of the average intensity of full-disk images taken by the SDO/AIA mission in EUV channels centered at 94, 131, 171, 193, 211, and 335 Angstrom. We also corrected the light curves for the flare gradual phase. From the analysis of the light curves we find that all the studied flares exhibit dimmings, where the intensity decreases with respect to the pre-flare phase, mainly in the 171, 193, and 211 Angstrom channels. The dimmings in these channels become more pronounced upon applying the gradual-phase correction. Calculation of the DEM from the six AIA EUV channels shows that during all the observed dimmings, the DEM decreases with respect to its value in the pre-flare phase in the temperature range $10^{5.7}-10^{6.3}$ K. The signature of the dimming is more pronounced in the range $10^{5.7}-10^{6.0}$ K for the DEMs calculated with the original light curves, and in the range $10^{6.0}-10^{6.3}$ K for the DEMs calculated by taking into account the gradual-phase correction. For a sample event, we also calculated DEMs from EVE and spatially resolved AIA observations of the source region to assess the impact of spectral resolution and full-disk averaging. For both these cases the temperature range where the dimming in the DEM is more pronounced is similar to that resulting from the analysis of the spatially averaged AIA data; the magnitude of the dimming is similar for the EVE and larger for the spatially resolved AIA observations. Coronal dimmings associated with CMEs can be detected in Sun-as-a-star DEMs. The flare gradual phase can lead to an underestimation of the magnitude of the dimming.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper claims that coronal mass ejection (CME) signatures can be detected in Sun-as-a-star differential emission measure (DEM) analysis. Using full-disk SDO/AIA EUV light curves in six channels for 16 eruptive flares, the authors apply a gradual-phase correction, identify intensity dimmings (most pronounced in 171, 193, and 211 Å), and show corresponding DEM decreases in the 10^{5.7}–10^{6.3} K range. The dimming signature shifts to higher temperatures within this band after correction. A single-event comparison with EVE spectra and spatially resolved AIA data yields consistent temperature ranges, with larger magnitude in resolved data. The conclusion is that CME-associated dimmings are recoverable in unresolved DEMs, though the gradual phase can underestimate their strength.
Significance. If the DEM drops can be securely attributed to CME mass loss, the result supplies a practical observational pathway for identifying CMEs in stellar EUV data where spatial resolution is unavailable. The consistency across 16 events and the cross-check with EVE and resolved AIA strengthen the case for applicability to Sun-as-a-star studies of stellar activity.
major comments (2)
- [Event selection and analysis] Event selection (abstract and § on sample): the study analyzes only 16 eruptive flares. No parallel analysis of a control sample of confined (non-CME) flares is reported. Without this comparison, the observed DEM decrease in 10^{5.7}–10^{6.3} K cannot be unambiguously attributed to CME mass removal rather than generic flare-driven effects such as temperature redistribution or residual cooling.
- [DEM inversion] DEM calculation (section describing inversion from six AIA channels): uncertainties arising from the under-constrained inversion and from line-of-sight mixing of active-region and quiet-Sun emission are not quantified. This omission directly affects in the reported temperature-specific DEM drops and their interpretation as mass-loss signatures.
minor comments (2)
- [Methods] The gradual-phase correction procedure is referenced but its exact implementation (functional form, fitting window, validation against non-eruptive cases) is not described in sufficient detail for reproducibility.
- [Figures] Figures showing light curves and DEM time series would benefit from explicit pre-flare baseline annotations and error bars derived from the DEM inversion.
Simulated Author's Rebuttal
We thank the referee for the constructive review and positive assessment of our work. We address each major comment below and have revised the manuscript to incorporate the suggestions where feasible.
read point-by-point responses
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Referee: [Event selection and analysis] Event selection (abstract and § on sample): the study analyzes only 16 eruptive flares. No parallel analysis of a control sample of confined (non-CME) flares is reported. Without this comparison, the observed DEM decrease in 10^{5.7}–10^{6.3} K cannot be unambiguously attributed to CME mass removal rather than generic flare-driven effects such as temperature redistribution or residual cooling.
Authors: We agree that a control sample of confined flares would strengthen the case for attributing the DEM drops specifically to CME mass loss. Our study was intentionally restricted to eruptive events with confirmed CME associations to isolate the expected mass-ejection signature. Literature on spatially resolved observations indicates that confined flares rarely produce comparable EUV dimmings. We have added a dedicated paragraph in the discussion section acknowledging this limitation and recommending that future Sun-as-a-star studies include such a control sample. The multi-event consistency, the shift in temperature range after gradual-phase correction, and the agreement with both EVE spectra and resolved AIA data for the sample event provide supporting evidence for the CME interpretation. revision: partial
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Referee: [DEM inversion] DEM calculation (section describing inversion from six AIA channels): uncertainties arising from the under-constrained inversion and from line-of-sight mixing of active-region and quiet-Sun emission are not quantified. This omission directly affects in the reported temperature-specific DEM drops and their interpretation as mass-loss signatures.
Authors: We thank the referee for highlighting this important point. In the revised manuscript we have added a new subsection that quantifies these uncertainties. We performed a Monte Carlo analysis by adding Gaussian noise to the input light curves consistent with the measurement uncertainties and recomputed the DEMs 1000 times; the resulting standard deviations show that the reported DEM decreases in the 10^{5.7}–10^{6.3} K range remain significant. We also discuss the effect of line-of-sight mixing by comparing the full-disk DEMs to the active-region-only DEMs derived from the spatially resolved AIA data for the sample event, confirming that the temperature range of the dimming is robust. revision: yes
Circularity Check
No significant circularity; purely observational analysis
full rationale
The paper conducts a direct observational study of 16 eruptive flares using full-disk SDO/AIA EUV light curves, applies a standard gradual-phase correction, and computes DEMs via established inversion from the six AIA channels. No equations, derivations, or fitted parameters are introduced that reduce to the paper's own inputs by construction. Results rest on external data and off-the-shelf DEM codes rather than self-definitions, self-citations as load-bearing premises, or renamings of known results. The central claim (detection of dimmings in Sun-as-a-star DEMs) is tested against the data without circular reduction.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption The six AIA EUV channels provide sufficient temperature coverage and response functions to invert for DEM in the 10^5.7-10^6.3 K range without major bias from line blending or background subtraction.
- domain assumption Intensity decreases in the 171, 193, and 211 Å channels during the dimming phase are dominated by removal of coronal plasma rather than changes in temperature distribution or non-thermal effects.
Reference graph
Works this paper leans on
-
[1]
S., Barnes, R., Cohen, O., et al
Airapetian, V . S., Barnes, R., Cohen, O., et al. 2020, Int. J. Astrobiol., 19, 136
work page 2020
-
[2]
Aschwanden, M. J., Nitta, N. V ., Wuelser, J.-P., et al. 2009, ApJ, 706, 376
work page 2009
-
[3]
Chen, P. F. 2011, Liv. Rev. Sol. Phys., 8, 1 Del Zanna, G. & Mason, H. E. 2018, Liv. Rev. Sol. Phys., 15, 5 Del Zanna, L. et al. 2021, ApJ, 909, 38
work page 2011
-
[4]
Dere, K. P. et al. 1997, A&AS, 125, 149
work page 1997
-
[5]
M., Temmer, M., Podladchikova, T., & Vanninathan, K
Dissauer, K., Veronig, A. M., Temmer, M., Podladchikova, T., & Vanninathan, K. 2018, ApJ, 863, 169
work page 2018
-
[6]
J., Cheimets, P., Garraffo, C., et al
Drake, J. J., Cheimets, P., Garraffo, C., et al. 2021, in Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series, V ol. 11821, UV , X-Ray, and Gamma-Ray Space Instrumentation for Astronomy XXII, ed. O. H. Sieg- mund, 1182108
work page 2021
-
[7]
France, K., Fleming, B., Youngblood, A., et al. 2022, J. Astron. Telesc. Instrum. Syst., 8, 014006
work page 2022
- [8]
-
[9]
Hannah, I. G. & Kontar, E. P. 2012, A&A, 539, A146
work page 2012
-
[10]
Harra, L. K. & Sterling, A. C. 2001, ApJ, 561, L215 Hernandez Camero, J., Green, L. M., & Piñel Neparidze, A. 2025, ApJ, 979, 63
work page 2001
- [11]
-
[12]
Jain, S., Podladchikova, T., Chikunova, G., Dissauer, K., & Veronig, A. M. 2024, A&A, 683, A15
work page 2024
-
[13]
Jin, M., Cheung, M. C. M., DeRosa, M. L., Nitta, N. V ., & Schrijver, C. J. 2022, ApJ, 928, 154
work page 2022
-
[14]
Kraaikamp, Emil & Verbeeck, Cis. 2015, J. Space Weather Space Clim., 5, A18
work page 2015
-
[15]
Lammer, H., Lichtenegger, H. I. M., Kulikov, Y . N., et al. 2007, Astrobiology, 7, 185
work page 2007
-
[16]
Lemen, J. R., Title, A. M., Akin, D. J., et al. 2012, Sol. Phys., 275, 17
work page 2012
-
[17]
Loyd, R. O. P., Mason, J. P., Jin, M., et al. 2022, ApJ, 936, 170
work page 2022
-
[18]
Mason, J. P., Woods, T. N., Caspi, A., Thompson, B. J., & Hock, R. A. 2014, ApJ, 789, 61
work page 2014
- [19]
-
[20]
P., Youngblood, A., France, K., Veronig, A
Mason, J. P., Youngblood, A., France, K., Veronig, A. M., & Jin, M. 2025, ApJ, 988, 167
work page 2025
- [21]
-
[22]
Patsourakos, S., V ourlidas, A., & Kliem, B. 2010, A&A, 522, A100
work page 2010
-
[23]
Reinard, A. A. & Biesecker, D. A. 2008, ApJ, 674, 576
work page 2008
-
[24]
Robbrecht, E., Patsourakos, S., & V ourlidas, A. 2009, ApJ, 701, 283
work page 2009
-
[25]
Samara, E., Patsourakos, S., & Georgoulis, M. K. 2021, ApJ, 909, L12
work page 2021
- [26]
-
[27]
W., Xia, L., He, J., & Wang, X
Tian, H., McIntosh, S. W., Xia, L., He, J., & Wang, X. 2012, ApJ, 748, 106
work page 2012
-
[28]
Vanninathan, K., Veronig, A. M., Dissauer, K., & Temmer, M. 2018, ApJ, 857, 62
work page 2018
-
[29]
M., Dissauer, K., Kliem, B., et al
Veronig, A. M., Dissauer, K., Kliem, B., et al. 2025, Liv. Rev. Sol. Phys., 22, 2
work page 2025
-
[30]
M., Odert, P., Leitzinger, M., et al
Veronig, A. M., Odert, P., Leitzinger, M., et al. 2021, Nat. Astron., 5, 697 V ourlidas, A., Patsourakos, S., & Savani, N. P. 2019, Phil. Trans. R. Soc. A., 377, 20180096
work page 2021
-
[31]
Webb, D. F. & Howard, T. A. 2012, Liv. Rev. Sol. Phys., 9, 3
work page 2012
-
[32]
Woods, T. N., Eparvier, F. G., Hock, R., et al. 2012, Sol. Phys., 275, 115
work page 2012
- [33]
-
[34]
Xu, Y ., Tian, H., Veronig, A. M., & Dissauer, K. 2024, ApJ, 970, 60
work page 2024
-
[35]
Yashiro, S., Gopalswamy, N., Michalek, G., et al. 2004, J. Geophys. Res. (Space Phys.), 109, A07105
work page 2004
-
[36]
Zhang, J., Temmer, M., Gopalswamy, N., et al. 2021, Prog. Earth Planet Sci., 8, 56 Article number, page 8 of 8
work page 2021
discussion (0)
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