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22 Newly Identified Repeating Changing-look AGNs and Evidence for Extreme Broad-line Region Breathing

T0 review · 1 major / 8 minor · reviewed 2026-08-01 · deepseek-v4-flash

Pith's one-line read Repeating changing-look AGNs show broad-line regions that persist and breathe rather than being destroyed and rebuilt

desk verdict A useful new RCL sample with careful follow-up, but the headline Eddington-ratio separation rests on a virial-calibration comparison that needs a robustness check. read the letter →

arxiv 2607.15564 v1 pith:TA6L3XA6 submitted 2026-07-17 astro-ph.GA astro-ph.HE

classification astro-ph.GAastro-ph.HE
keywords changing-lookAGNrepeatingbroad-lineregionBLRbreathingEddingtonratiovariabilityquasarspectroscopysupermassiveblackholes
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The reading

This paper identifies 25 repeating changing-look AGNs, 22 of them new, in which the same nucleus turns its broad emission lines off and on again, some within three to four years and possibly in as little as a few months. Its central claim is that these repeated transitions are not destruction and rebirth of the broad-line region (BLR), but 'breathing': the same BLR gas persists while the central accretion power rises and falls, carrying individual emission lines across visibility thresholds. The key quantitative result is a statistical separation between Hβ-only transitions and transitions involving both Hα and Hβ: Hβ-only events happen at higher off-state Eddington ratios, so Hβ fades from view at a higher accretion level than Hα. Seven sources with nearly continuous light curves show their spectral on/off states tracking multi-year optical excursions, with infrared dust emission following the same trends. If true, changing-look AGNs become a window onto a reversible, line-dependent BLR response to accretion variability rather than a catastrophic reconfiguration of the gas.

What carries the argument

The load-bearing instrument is the RCL AGN sample itself: because the same nucleus crosses the same physical boundary more than once, one-off destructive events or simple line-of-sight obscuration are excluded as explanations. Within that sample, the discriminant is the two-sample K-S test on off-state log Eddington ratios (D = 0.667, p = 2.17 × 10⁻⁵) between Hβ-only and Hα+Hβ transition groups, supplemented by an Anderson-Darling test. The proposed physical mechanism is BLR breathing: a radially stratified broad-line region whose line emissivities, responsivities, and detectability vary with the incident ionizing flux, so lines go below visibility thresholds in a fixed order as accretion fa

What would settle it

Recompute the Figure 6 comparison with one uniform virial calibration and one bolometric correction applied to all 74 sources; if the Hβ-only and Hα+Hβ off-state Eddington-ratio distributions then overlap (K-S p > 0.05), the line-dependent visibility threshold is not established. A complementary check: for the seven continuously monitored RCL AGNs, predict a third transition at the next optical light-curve extremum and observe whether the broad lines reappear or disappear with the continuum; if they do not, the breathing picture is falsified.

Watch

Extended reading notes

Core claim

The paper establishes, on its own terms, that repeated changing-look transitions — on–off–on or off–on–off sequences in the same active galactic nucleus — trace reversible changes in the central ionizing continuum. The broad-line region is not removed and re-formed each time; instead, the same structure 'breathes': as the ionizing flux weakens, broad Hβ falls below its detection threshold first, at a relatively high Eddington ratio, while broad Hα remains visible until the source sinks to a lower accretion level. The authors demonstrate this with a two-sample Kolmogorov-Smirnov test on off-state Eddington ratios (D = 0.667, p = 2.17 × 10⁻⁵) and an Anderson-Darling test, comparing Hβ-only and

Load-bearing premise

The load-bearing premise is that the two Eddington-ratio distributions compared in Figure 6 are measured on a common scale: the groups mix three black-hole-mass calibrations and two bolometric corrections, with RCL masses pinned to on-state values, so a systematic shift of roughly 0.3–0.5 dex correlated with the Hβ-only versus Hα+Hβ grouping would erase the threshold signal.

Editorial extensions

If this is right

  • A single changing-look event cannot distinguish destroyed gas from faded line emission; repeated transitions directly demonstrate that the broad-line region persists, so CL events should be treated as accretion-state diagnostics rather than evidence of BLR destruction.
  • Because Hβ fades at a higher Eddington ratio than Hα, off-state classification depends on which lines a spectrum covers; surveys that only measure Hβ will classify sources as 'off' earlier than those including Hα, so wavelength coverage must be reported in CL-AGN catalogs.
  • The driver of CL transitions must be reversible and operate on month-to-year timescales; candidate processes such as accretion-mode changes, heating/cooling fronts, magnetically supported disks, or radiation-pressure instability are constrained to produce smooth multi-year excursions rather than stochastic flickering.
  • The latest spectra of RCL AGNs fall on the expected side of the CL population in the Eddington-ratio versus black-hole-mass plane, supporting the use of optical light-curve extrema as predictors of spectroscopic state.
  • The line-dependent threshold sequence implies that Hβ, and later Hα, can be used as accretion-level indicators: when Hβ disappears while Hα remains, the source sits in an intermediate accretion state.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • A natural next test, not run in the paper, is whether Hβ-only, Mg II-only, and Hα-only transitions form an ordered ladder in off-state Eddington ratio; the paper's line-responsivity argument predicts Mg II sits between Hβ and Hα.
  • The K-S comparison mixes three black-hole-mass calibrations and two bolometric corrections; recomputing Figure 6 with a single uniform calibration, or separately by group, would settle whether the claimed threshold separation survives calibration systematics.
  • If BLR breathing is correct, high-cadence reverberation mapping across a second transition should show the emission-line lag, width, and responsivity returning toward their first-epoch values as the continuum recovers — a test that distinguishes breathing from stochastic gas rearrangement.
  • The same-nucleus logic could be extended to predict future transitions: unconfirmed candidates with moderate continuum changes are natural targets for monitoring at the next light-curve extremum.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

1 major / 8 minor

Summary. The paper searches the Guo et al. (2024, 2025a) and Dong et al. (2025b) changing-look AGN samples for objects whose broad Hβ turned off/on more than once. Using long-baseline ZTF/ATLAS/CRTS optical light curves, WISE/NEOWISE MIR light curves, archival SDSS/LAMOST/DESI spectra, and new LJT/DOT/HCT spectroscopy, the authors select 34 candidates, confirm 25 RCL AGNs (22 new), and classify nine non-confirmed cases. They report that the second transitions occur mostly on rest-frame timescales of 3–4 yr, that seven well-sampled objects show spectral states tracking smooth multi-year optical excursions, and that Hβ-only transitions occur at higher off-state Eddington ratios than Hα+Hβ transitions, based on a K-S test (D=0.667, p=2.17e-5). They interpret this as evidence for a line-dependent BLR visibility threshold and 'extreme BLR breathing', i.e., the BLR gas persists and re-emits rather than being destroyed and rebuilt.

Significance. If the statistical separation in Fig. 6 is robust, the paper would provide the largest sample of newly discovered repeating CL AGNs and a direct, repeated-nucleus test of line-dependent BLR visibility thresholds. The identification pipeline is genuinely careful: Rs>0.3 thresholding, visual inspection of all multi-epoch spectra, [O III] checks against data-quality artifacts, and individual discussion of the nine non-confirmed candidates are all strengths. The seven well-sampled sources with continuous light curves offer a useful link between spectroscopic state and continuum excursion. However, the headline K-S result compares Eddington ratios that are not placed on a common virial-calibration scale, and the paper does not show that the separation survives homogeneous recalibration. The central interpretive claim is therefore currently not established, though it is plausibly fixable with additional analysis.

major comments (1)
  1. [§4.2 / Fig. 6] The Anderson-Darling p-value is reported as '≤ 10^-3 (floored by numerical resolution)', which is inadequate for a claim of 'confidence level exceeding 99.9%'. A floor of 10^-3 is only 99.9% if the true value is exactly 0.001; reporting a one-sided inequality without a better determination, or using a Monte Carlo estimate, is not sufficient to support the stated confidence level. This is a secondary issue relative to the calibration mixing, but it should be corrected in any revision.
minor comments (8)
  1. [Abstract] 'As Seven RCL AGNs' should read 'Seven RCL AGNs' (capital A and misplaced 'As').
  2. [§2] Header 'Seciont' is a typo for 'Section'.
  3. [Fig. 5 caption] 'solide curves' should be 'solid curves'.
  4. [General] The solar-mass symbol appears as 'uni2299' in several axis labels and table headers; these are unicode rendering artifacts that should be fixed.
  5. [Eq. (1)] The definition of Rs as 'Sb − Sd / Sb' is ambiguous; it should be written as (Sb−Sd)/Sb.
  6. [Table A1] Several entries contain stray spaces ('5953 2', '6111 9a', '5739 5a'); the table needs a formatting pass.
  7. [§3.2] 'observed (rest-frame) timescales' mixes observer-frame and rest-frame terminology; the sentence should specify which quantity is which.
  8. [Data Availability] The statement that derived data are available 'on reasonable request' is weaker than the reproducibility standards common in this field; public tables or a machine-readable supplement would be preferable.

Circularity Check

1 steps flagged · score 3.0 of 10

No load-bearing circularity; the RCL sample and light-curve results are self-contained. Minor definitional circularity in the Fig. 3 consistency check; the Fig. 6 K-S retains empirical content and is not a forced fit.

  1. self definitional [Section 2.3, Section 3.1, Figure 3]
    "The identification was based on the broad Hβ component, whose appearance or disappearance was used to trace repeating transitions. ... The latest spectra show that the on/off states correspond to higher/lower Eddington-ratio, in the expected direction relative to the parent CL-AGN samples."

    The on/off state is defined by the presence or absence of broad Hβ, while the Eddington ratio is derived from the same spectra: 'The black hole masses MBH and Eddington ratios λEdd given in the table were derived only from the latest spectra obtained in this work.' Since Hβ visibility is expected to depend on the same ionizing continuum that enters λEdd, the statement that on-state sources have higher λEdd than off-state sources is substantially built into the classification. The paper labels this an expected-direction check rather than a test, so the damage to the central claims is limited.

full rationale

The paper's principal contributions — the identification of 25 RCL AGNs (22 new), the multi-epoch spectroscopic confirmation, and the correlation of spectral states with long-term optical/MIR light-curve excursions — are empirical and self-contained; they do not reduce to the assumptions they are meant to support. The only genuinely definitional element is the Figure 3 consistency check: because 'on' is defined as the presence of broad Hβ and λEdd is computed from the same spectra' continuum, the observed on/off λEdd ordering is largely a restatement of the classification. The paper itself treats this as a sanity check ('We note that the linear fits are not intended to define a universal boundary between the on and off states'), so this is a minor circularity rather than a load-bearing flaw. The Figure 6 K-S result (D=0.667, p=2.17e-5) is more subtle: the groups are defined by which broad lines changed, and the compared quantity is the off-state λEdd, the same accretion parameter expected to control line visibility. Thus the ordering is partly encoded in the group definitions. However, the λEdd values come from an independent measurement stream (continuum luminosity and virial masses), and the ordering could in principle have failed; the result is also supported by an external, independent relation (Guo et al. 2025b). The concern about mixed virial calibrations and bolometric corrections is a correctness/robustness risk, not a circularity, because it does not make the claim true by construction. There is no load-bearing self-citation: the cited prior work by the present authors is peripheral, and the central physical input is the externally established line-response sequence. Overall, the sample and variability evidence stand on their own, and the circularity score is modest.

Assumptions & free parameters 5 free parameters · 4 assumptions · 0 invented entities

The paper introduces no new physical entities; 'BLR breathing' and 'naked Type 2' are prior concepts. The load-bearing number inputs are literature virial calibrations and bolometric corrections plus several hand-chosen pipeline thresholds (Rs>0.3, zg<20.5, polynomial degree, visual selection). The principal unquantified assumption is the inter-comparability of λEdd across line-species calibrations and across the two samples used in the K-S test.

free parameters (5)
  • CL transition threshold Rs > 0.3 = 0.3
    Hand-chosen relative broad-Hβ flux change that counts as a CL transition (Eq. 1, §2.3).
  • zg < 20.5 mag observation limit = 20.5 mag
    Magnitude cut for scheduling follow-up spectroscopy; biases the sample toward brighter objects and excludes many candidates near the selected ones (§2.2).
  • Third-order polynomial for zg-band trends = degree 3
    Chosen to describe long-term continuum variations in §3.3/Fig. C3; imposes at most one extremum, which shapes the U/n classification of the seven well-sampled sources.
  • Candidate selection priorities (color-magnitude slope k, magnitude change Δzg) = not quantified
    Candidates chosen 'by visual examination... rather than by a strict criterion' (§2.2); the selection function is not exactly reproducible.
  • zg-like conversion hyperparameters (Huber regression, LOWESS smoothing) = source-specific
    The ac→zg mapping uses a per-source linear fit and LOWESS smoothing (§2.2); smoothing span and fitting choices are implementation parameters.
assumptions (4)
  • domain assumption Single-epoch virial mass relations (Eq. 2) give reliable MBH and λEdd at population level
    Uses Vestergaard & Peterson (2006), Greene & Ho (2005), Vestergaard & Osmer (2009) calibrations; known ~0.4 dex intrinsic scatter is not propagated into the K-S test (§3.1, Fig. 6).
  • domain assumption Bolometric corrections 9.26 L5100 and 5.15 L3000 (Richards et al. 2006) apply to all sources
    Used to convert monochromatic luminosities to Lbol (§3.1); the two transition groups use a mixture of these corrections, a possible systematic.
  • domain assumption Off states are intrinsic (weak ionizing continuum / weak BLR emission), not orientation-obscured
    Section 4.2 infers this from MIR following optical variations and variability amplitudes similar to Type 1 AGNs; X-ray data are not available for all sources.
  • domain assumption Parent-sample CL classifications (Guo et al. 2024, 2025a; Dong et al. 2025b) are correct and comparable to the authors' classifications
    RCL identification and the Fig. 6 grouping both start from these samples; their spectral-state and transition-type assignments are taken at face value.

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Cite this review

Pith. "Pith review of 22 Newly Identified Repeating Changing-look AGNs and Evidence for Extreme Broad-line Region Breathing." pith.science (2026). https://pith.science/paper/TA6L3XA6

@misc{pith2026260715564,
  author       = {Pith},
  title        = {Pith review of: 22 Newly Identified Repeating Changing-look AGNs and Evidence for Extreme Broad-line Region Breathing},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/TA6L3XA6}},
  note         = {Machine review of arXiv:2607.15564}
}
abstract

Changing-look active galactic nuclei (CL AGNs) show the appearance or disappearance of broad emission lines on timescales of years. Among them, the repeating CL (RCL) AGNs may provide a clear clue for our understanding of the CL transitions because the same nucleus crosses some physical boundaries more than once. We search for RCL AGNs in known CL-AGN samples using long-term multi-band light curves, and selected 34 candidates for spectroscopic follow-up. We confirm 25 RCL AGNs, including 22 newly identified cases. Properties of these RCL AGNs are analyzed. The observed rest-frame intervals of the second transitions are mostly 3--4 yr, while the variations of the optical light curves suggest that some transitions might occur on timescales of several months. The latest spectra show that the on/off states correspond to higher/lower Eddington-ratio, in the expected direction relative to the parent CL-AGN samples. As seven RCL AGNs are well covered by nearly continuous single-band light curves, their on/off states can be found to follow multi-year optical excursions, and their Eddington ratios vary consistently with the photometric changes. We also find that the H$\beta$-only transitions occur at higher Eddington ratios than the transitions involving both H$\alpha$ and H$\beta$, suggesting a line-dependent Broad-Line-Region (BLR) visibility threshold. These results support a picture in which different accretion-flow processes drive reversible changes in the central ionizing emissions, while the observed RCL transitions are produced by the BLR breathing across line-dependent visibility thresholds.

Figures

Figures reproduced from arXiv: 2607.15564 by the authors.

Figure 1
Figure 1. Distribution of the color–magnitude slope k ver￾sus the zg-band magnitude change ∆zg for the CL parent samples (gray triangles) and our selected candidates (con￾sisting of the confirmed RCL, marked with red or indian-red, and the non-confirmed RCL (nRCL), marked with yellow and orange). The up- and down-pointing triangles denotes the on and off spectral state, respectively. The background Type 1 (blue dots) and Type… view at source ↗
Figure 3
Figure 3. Distribution of Eddington ratio versus black hole mass. Upper panel: the latest on-state measurements of the on–off–on RCL AGNs (blue circles) compared with off-state CL AGNs (grey points) from the parent samples. Bottom panel: the latest off-state measurements of the off–on–off RCL AGNs (blue circles), compared with on-state CL AGNs (grey points) from the parent samples. Black squares mark the non-confirmed RCL-AGN… view at source ↗
Figure 4
Figure 4. Optical magnitude change versus the observed and photometric timescales (dt and dt1, respectively) for the second CL transition. dicating Eddington ratios higher than the typical off￾state CL AGNs. Similarly, the off–on–off sources tend to have lower Eddington ratios relative to the on-state CL AGNs. The trend is consistent with the spectral clas￾sifications of the latest spectra: sources returning to an on state ha… view at source ↗
Figures from the paper (3 more)
Figure 5
Figure 5. Figure 5: Comparison between the normalized fitted zg-band light-curve trends (solide curves) and the Eddington ratios of the seven well-sampled RCL AGNs. The Eddington ratios measured from the three spectroscopic epochs are con￾nected by lines of the same color as the trends fo…
Figure 6
Figure 6. Figure 6: Off-state Eddington ratios and black hole masses for CL and RCL AGNs, grouped by the broad lines involved in the transition. The filled symbols are CL AGNs from Dong et al. (2025b), where the transition types were classi￾fied from the changing broad lines. The open sym…
Figure 7
Figure 7. Figure 7: Rest-frame spectra comparing J0759 with UN￾AM-KIAS 613. The SDSS spectrum of UNAM-KIAS 613 has been divided by 5 and shifted downward by 12 for visual comparison. Among our RCL AGNs, we also note that J0759 may provide an interesting case in which the long-term accreti…

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Works this paper leans on

93 extracted references · 1 canonical work pages

  1. [1]

    N., Adelman-McCarthy, J

    Abazajian, K. N., Adelman-McCarthy, J. K., Ag¨ ueros, M. A., et al. 2009, ApJS, 182, 543

  2. [2]

    2020, ApJL, 890, L29

    Ai, Y., Dou, L., Yang, C., et al. 2020, ApJL, 890, L29

  3. [3]

    1993, ARA&A, 31, 473

    Antonucci, R. 1993, ARA&A, 31, 473

  4. [4]

    Terlevich, R. J. 1999, ApJL, 519, L123

  5. [5]

    C., Kulkarni, S

    Bellm, E. C., Kulkarni, S. R., Graham, M. J., et al. 2019, PASP, 131, 018002

  6. [6]

    C., Denney, K

    Bentz, M. C., Denney, K. D., Grier, C. J., et al. 2013, ApJ, 767, 149

  7. [7]

    K., Nicholl, M., Berger, E., et al

    Blanchard, P. K., Nicholl, M., Berger, E., et al. 2017, ApJ, 843, 106

  8. [8]

    R., & Bloom, J

    Butler, N. R., & Bloom, J. S. 2011, AJ, 141, 93

Show all 93 references
  1. [9]

    M., & Horne, K

    Cackett, E. M., & Horne, K. 2006, MNRAS, 365, 1180 Cer´ on-Meneses, J., Ar´ evalo, P., S´ anchez-S´ aez, P., et al. 2026, A&A, 709, A245

  2. [10]

    2026, arXiv e-prints, arXiv:2605.24429

    Chen, G., Yang, W., Ye, X., et al. 2026, arXiv e-prints, arXiv:2605.24429

  3. [11]

    2025, arXiv e-prints, arXiv:2511.15359

    Chen, Z.-Q., Jin, J.-J., Guo, W.-J., et al. 2025, arXiv e-prints, arXiv:2511.15359

  4. [12]

    Cleveland, W. S. 1979, Journal of the American Statistical Association, 74, 829

  5. [13]

    Foltz, C. B. 1986, ApJ, 311, 135 Cortes-Su´ arez, E., Marziani, P., Hern´ andez-Toledo, H. M., Arag´ on-Calvo, M. A., & Negrete, C. A. 2026, MNRAS, arXiv:2604.25219

  6. [14]

    Cowsik, R., Srinivasan, R., & Prabhu, T. P. 2002, Bulletin of the Astronomical Society of India, 30, 105

  7. [15]

    2012, Research in Astronomy and Astrophysics, 12, 1197

    Cui, X.-Q., Zhao, Y.-H., Chu, Y.-Q., et al. 2012, Research in Astronomy and Astrophysics, 12, 1197

  8. [16]

    D., De Rosa, G., Croxall, K., et al

    Denney, K. D., De Rosa, G., Croxall, K., et al. 2014, ApJ, 796, 134 DESI Collaboration, Aghamousa, A., Aguilar, J., et al. 2016, arXiv e-prints, arXiv:1611.00036

  9. [17]

    Dexter, J., & Begelman, M. C. 2019, MNRAS, 483, L17

  10. [18]

    2025a, arXiv e-prints, arXiv:2510.18445

    Dong, Q., Zhang, Z.-X., Gu, W.-M., et al. 2025a, arXiv e-prints, arXiv:2510.18445

  11. [19]

    J., Djorgovski, S

    Drake, A. J., Djorgovski, S. G., Mahabal, A., et al. 2009, ApJ, 696, 870

  12. [20]

    2012, ApJL, 747, L33

    Elitzur, M. 2012, ApJL, 747, L33

  13. [21]

    Elitzur, M., & Ho, L. C. 2009, ApJL, 701, L91

  14. [22]

    C., & Trump, J

    Elitzur, M., Ho, L. C., & Trump, J. R. 2014, MNRAS, 438, 3340

  15. [23]

    Eracleous, M., & Halpern, J. P. 2001, ApJ, 554, 240

  16. [24]

    J., et al

    Frederick, S., Gezari, S., Graham, M. J., et al. 2019, ApJ, 883, 31

  17. [25]

    2021, QSOFITMORE: a python package for fitting UV-optical spectra of quasars, v.v1.1.0, Zenodo, doi:10.5281/zenodo.5810042

    Fu, Y. 2021, QSOFITMORE: a python package for fitting UV-optical spectra of quasars, v.v1.1.0, Zenodo, doi:10.5281/zenodo.5810042

  18. [26]

    2022, ApJS, 261, 32

    Fu, Y., Wu, X.-B., Jiang, L., et al. 2022, ApJS, 261, 32

  19. [27]

    B., et al

    Gezari, S., Hung, T., Cenko, S. B., et al. 2017, ApJ, 835, 144

  20. [28]

    J., Duffy, L., et al

    Gilbert, O., Ruan, J. J., Duffy, L., et al. 2025, arXiv e-prints, arXiv:2508.01933

  21. [29]

    R., & Korista, K

    Goad, M. R., & Korista, K. T. 2014, MNRAS, 444, 43

  22. [30]

    J., Ross, N

    Graham, M. J., Ross, N. P., Stern, D., et al. 2020, MNRAS, 491, 4925

  23. [31]

    J., Pulgarin-Duque, L., Anderson, S

    Green, P. J., Pulgarin-Duque, L., Anderson, S. F., et al. 2022, ApJ, 933, 180

  24. [32]

    E., & Ho, L

    Greene, J. E., & Ho, L. C. 2005, ApJ, 630, 122

  25. [33]

    2018, PyQSOFit: Python code to fit the spectrum of quasars, Astrophysics Source Code Library, record ascl:1809.008, , , ascl:1809.008

    Guo, H., Shen, Y., & Wang, S. 2018, PyQSOFit: Python code to fit the spectrum of quasars, Astrophysics Source Code Library, record ascl:1809.008, , , ascl:1809.008

  26. [34]

    2026, Research in Astronomy and Astrophysics, 26, 095026

    Guo, W.-J., Chen, Z.-Q., Wang, S., Zhang, Z.-X., & Cheng, C. 2026, Research in Astronomy and Astrophysics, 26, 095026

  27. [35]

    A., et al

    Guo, W.-J., Zou, H., Fawcett, V. A., et al. 2024, ApJS, 270, 26

  28. [36]

    2026, Research in Astronomy and Astrophysics, 26, 095001

    Han, P., Lu, H., Lyu, B., Wu, J., & Wu, Q. 2026, Research in Astronomy and Astrophysics, 26, 095001

  29. [37]

    Hawkins, M. R. S. 2004, A&A, 424, 519

  30. [38]

    2026, arXiv e-prints, arXiv:2606.06802

    He, H., You, B., ´Sniegowska, M., & Czerny, B. 2026, arXiv e-prints, arXiv:2606.06802

  31. [39]

    Huber, P. J. 1964, The Annals of Mathematical Statistics, 35, 73

  32. [40]

    J., et al

    Jana, A., Ricci, C., Temple, M. J., et al. 2025, A&A, 693, A35

  33. [41]

    2025, arXiv e-prints, arXiv:2511.09626

    Kaaz, N., Liska, M., Ward, C., & Davelaar, J. 2025, arXiv e-prints, arXiv:2511.09626

  34. [42]

    2026, A&A, 707, A46

    Kollatschny, W., Grupe, D., Winkler, H., et al. 2026, A&A, 707, A46

  35. [43]

    2026, Advances in Space Research, 77, 4041

    Komossa, S., Grupe, D., Marziani, P., et al. 2026, Advances in Space Research, 77, 4041

  36. [44]

    T., & Goad, M

    Korista, K. T., & Goad, M. R. 2004, ApJ, 606, 749

  37. [45]

    2014, ApJ, 788, 159

    Koshida, S., Minezaki, T., Yoshii, Y., et al. 2014, ApJ, 788, 159

  38. [46]

    2026, arXiv e-prints, arXiv:2606.23564

    Kovacevic, N., Dai, X., Yuk, H., et al. 2026, arXiv e-prints, arXiv:2606.23564

  39. [47]

    M., Yaqoob, T., Ptak, A

    LaMassa, S. M., Yaqoob, T., Ptak, A. F., et al. 2014, ApJ, 787, 61 22

  40. [48]

    M., Cales, S., Moran, E

    LaMassa, S. M., Cales, S., Moran, E. C., et al. 2015, ApJ, 800, 144

  41. [49]

    1987, PASP, 99, 309 —

    Lawrence, A. 1987, PASP, 99, 309 —. 2018, Nature Astronomy, 2, 102

  42. [50]

    2025, ApJ, 994, 216

    Layek, N., Nandi, P., Naik, S., et al. 2025, ApJ, 994, 216

  43. [51]

    M., et al

    Liu, C., Kong, F., Cooper, E. M., et al. 2026, ApJS, 284, 12 liu, H., Wu, Q., Lyu, B., & Yan, Z. 2019, arXiv e-prints, arXiv:1912.03972 L´ opez-Navas, E., Mart ´ ınez-Aldama, M. L., Bernal, S., et al. 2022, MNRAS, 513, L57 L´ opez-Navas, E., S´ anchez-S´ aez, P., Ar´ evalo, P....

  44. [52]

    2025, A&A, 693, A173

    Lyu, B., Wu, X.-B., Pang, Y., et al. 2025, A&A, 693, A173

  45. [53]

    L., Ross, N

    MacLeod, C. L., Ross, N. P., Lawrence, A., et al. 2016, MNRAS, 457, 389

  46. [54]

    2011, ApJ, 731, 53

    Mainzer, A., Bauer, J., Grav, T., et al. 2011, ApJ, 731, 53

  47. [55]

    2012, The Astrophysical Journal Letters, 757, L24

    Nixon, C., King, A., Price, D., & Frank, J. 2012, The Astrophysical Journal Letters, 757, L24

  48. [56]

    2018, MNRAS, 480, 3898

    Noda, H., & Done, C. 2018, MNRAS, 480, 3898

  49. [57]

    2019, arXiv e-prints, arXiv:1902.05857

    Mahto, M. 2019, arXiv e-prints, arXiv:1902.05857

  50. [58]

    J., Bianchi, S., et al

    Panessa, F., Carrera, F. J., Bianchi, S., et al. 2009, MNRAS, 398, 1951

  51. [59]

    2023, A&A, 669, A140

    Petrushevska, T., Leloudas, G., Ili´ c, D., et al. 2023, A&A, 669, A140

  52. [60]

    2022, ApJ, 925, 50

    Ren, W., Wang, J., Cai, Z., & Guo, H. 2022, ApJ, 925, 50

  53. [61]

    2026, arXiv e-prints, arXiv:2606.12511

    Ricci, C. 2026, arXiv e-prints, arXiv:2606.12511

  54. [62]

    J., et al

    Ricci, C., Trakhtenbrot, B., Koss, M. J., et al. 2017, Nature, 549, 488

  55. [63]

    T., Lacy, M., Storrie-Lombardi, L

    Richards, G. T., Lacy, M., Storrie-Lombardi, L. J., et al. 2006, ApJS, 166, 470

  56. [64]

    P., Ford, K

    Ross, N. P., Ford, K. E. S., Graham, M., et al. 2018, MNRAS, 480, 4468

  57. [65]

    J., Anderson, S

    Ruan, J. J., Anderson, S. F., Eracleous, M., et al. 2019, ApJ, 883, 76

  58. [66]

    J., Anderson, S

    Ruan, J. J., Anderson, S. F., Cales, S. L., et al. 2016, ApJ, 826, 188

  59. [67]

    2018, ApJ, 854, 160

    Rumbaugh, N., Shen, Y., Morganson, E., et al. 2018, ApJ, 854, 160

  60. [68]

    C., Cales, S., Ruan, J

    Runnoe, J. C., Cales, S., Ruan, J. J., et al. 2016, MNRAS, 455, 1691

  61. [69]

    C., & Dexter, J

    Scepi, N., Begelman, M. C., & Dexter, J. 2021, Monthly Notices of the Royal Astronomical Society: Letters, 502, L50

  62. [70]

    J., Prieto, J

    Shappee, B. J., Prieto, J. L., Grupe, D., et al. 2014, ApJ, 788, 48

  63. [71]

    2017, ApJL, 846, L7 —

    Sheng, Z., Wang, T., Jiang, N., et al. 2017, ApJL, 846, L7 —. 2020, ApJ, 889, 46

  64. [72]

    2020, A&A, 641, A167

    Sniegowska, M., Czerny, B., Bon, E., & Bon, N. 2020, A&A, 641, A167

  65. [73]

    A., & Wilson, A

    Storchi-Bergmann, T., Baldwin, J. A., & Wilson, A. S. 1993, ApJL, 410, L11

  66. [74]

    2008, NewAR, 52, 227

    Tadhunter, C. 2008, NewAR, 52, 227

  67. [75]

    E., & Osterbrock, D

    Tohline, J. E., & Osterbrock, D. E. 1976, ApJL, 210, L117

  68. [76]

    L., Denneau, L., Heinze, A

    Tonry, J. L., Denneau, L., Heinze, A. N., et al. 2018, PASP, 130, 064505

  69. [77]

    L., et al

    Trakhtenbrot, B., Arcavi, I., MacLeod, C. L., et al. 2019, ApJ, 883, 94

  70. [78]

    R., Impey, C

    Trump, J. R., Impey, C. D., Kelly, B. C., et al. 2011, ApJ, 733, 60

  71. [79]

    M., & Padovani, P

    Urry, C. M., & Padovani, P. 1995, PASP, 107, 803

  72. [80]

    Vestergaard, M., & Osmer, P. S. 2009, ApJ, 699, 800

  73. [81]

    Vestergaard, M., & Peterson, B. M. 2006, ApJ, 641, 689

  74. [82]

    2019, Research in Astronomy and Astrophysics, 19, 149

    Wang, C.-J., Bai, J.-M., Fan, Y.-F., et al. 2019, Research in Astronomy and Astrophysics, 19, 149

  75. [83]

    2025a, arXiv e-prints, arXiv:2511.10217

    Wang, H., Wu, X.-B., Yao, N., et al. 2025a, arXiv e-prints, arXiv:2511.10217

  76. [84]

    K., Brink, T

    Wang, J., Zheng, W. K., Brink, T. G., et al. 2023, ApJ, 956, 137

  77. [85]

    K., Xu, D

    Wang, J., Zheng, W. K., Xu, D. W., et al. 2022, Research in Astronomy and Astrophysics, 22, 015011

  78. [86]

    2025b, ApJ, 981, 129 —

    Wang, S., Woo, J.-H., Gallo, E., et al. 2025b, ApJ, 981, 129 —. 2024, ApJ, 966, 128 WISE Team. 2020, NEOWISE 2-Band Post-Cryo Single Exposure (L1b) Source Table, IPAC, doi:10.26131/IRSA124

  79. [87]

    L., Eisenhardt, P

    Wright, E. L., Eisenhardt, P. R. M., Mainzer, A. K., et al. 2010, AJ, 140, 1868

  80. [88]

    2018, ApJ, 862, 109

    Yang, Q., Wu, X.-B., Fan, X., et al. 2018, ApJ, 862, 109

  81. [89]

    J., MacLeod, C

    Yang, Q., Green, P. J., MacLeod, C. L., et al. 2023, ApJ, 953, 61

  82. [90]

    2024, ApJ, 966, 85

    Zeltyn, G., Trakhtenbrot, B., Eracleous, M., et al. 2024, ApJ, 966, 85

  83. [91]

    C., et al

    Zhu, L., Wang, Z., Gupta, A. C., et al. 2026, arXiv e-prints, arXiv:2605.25689

  84. [92]

    2024, MNRAS, 530, 3538

    Zhu, L.-T., Li, J., Wang, Z., & Zhang, J.-J. 2024, MNRAS, 530, 3538

  85. [93]

    U., et al

    Zhu, L.-T., Wang, Z., Devanand, P. U., et al. 2025, MNRAS, 536, 2715

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