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Cycle Variation in the Occurrence of Great Soft X-ray Solar Flares

Solar and Stellar Astrophysics · Submitted 8 Sep 2026 · Published version · 171 references

Pith's verdict: Interesting pattern in flare phase distribution, but a clear numerical inconsistency undermines trust in the analysis.

T0 · AI review

How this review was made: An AI referee (deepseek/deepseek-v4-flash) read the paper on September 10, 2026 and answered a fixed list of questions about it. T0 is the starting level every paper gets. The levels describe how deeply Pith has checked the paper, never the authors.

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  4. T3 Formal statement The claims written out in a formal math language a computer can read.
  5. T4 Proof Those claims proved, and the proof checked by computer.

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arXiv ID2609.09435 (version 1)
Pith ID5GO5Q2FK, Pith's permanent record of this paper and its review
CitationD.D. Sokoloff, M.M. Katsova, V.N. Obridko. "Cycle Variation in the Occurrence of Great Soft X-ray Solar Flares." arXiv:2609.09435 (2026). https://pith.science/paper/5GO5Q2FK
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Claim paper

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Referee report
The paper

The paper claims

The paper establishes that extreme solar soft X-ray flares (X10 and above) are not randomly distributed across the solar cycle but are strongly concentrated in the maximum and decline phases, while virtually absent during the growth phase…

The reading

By analyzing the latitude-time distribution of X-class flares observed by GOES over four full solar cycles (21–24), the authors show that the most powerful flares (X10+) avoid the early rise of the cycle. Instead, they first appear 1–2 years before sunspot maximum at a specific location where two activity waves collide—one moving equatorward and one poleward. That collision point, which the paper calls the burning point or overlapping point (OLP), is identified via a superposed-epoch analysis and coincides with a signature enhancement in the fifth harmonic of the large-scale magnetic field. The pattern suggests that extreme flare energy release requires the interaction of local active-region fields with global open-field structures (coronal holes), which become abundant only after the maximum. If correct, this work refines space-weather forecasting by specifying a narrow window and a magnetic-field marker for the most dangerous events.

What carries the argument

The central analytical tool is superposed epoch analysis, which normalizes each cycle to unit length and aligns flares relative to the cycle maximum, producing a synthetic time-latitude diagram. The key explanatory mechanism is the overlapping point (OLP) or burning point: the location on the butterfly diagram where three activity waves coexist (the main equatorward wave of the current cycle, a poleward wave of the same cycle, and a poleward wave of the next cycle), identified via the amplification of the fifth harmonic of the large-scale magnetic field. This point marks where the probability of complicated magnetic structures and extreme flares is highest because local bipolar fields interact with open field lines of coronal holes.

Extended reading notes

Core claim

The paper claims that the occurrence of the largest soft X-ray solar flares (≥X10) follows a strict cycle-phase dependence: they are virtually absent during the growth phase, begin to erupt about 1–2 years before the sunspot maximum at the overlapping point (OLP) where equatorward and poleward activity waves meet, and continue through the maximum and especially the decline phase of the cycle. This pattern is extracted by applying superposed epoch analysis to 37 X10+ flares over cycles 21–24, collapsing them onto a normalized phase axis. The OLP is independently defined from the magnetic field harmonic decomposition (enhanced l=5 harmonic) and is shown to coincide in time and latitude with the first appearance of weak X4-7 flares and the initiation of X10+ flares. The paper concludes that the largest flares require a global activity complex—a configuration combining an active region with an adjacent coronal hole—which becomes most frequent after solar maximum.

Load-bearing premise

The statistical pattern rests on only 37 X10+ flares gathered from four solar cycles, and the coincidence of the burning point with the previously defined overlapping point (OLP) is derived from the same magnetic field data without independent observational verification.

Editorial extensions

If this is right

  • Space-weather hazard forecasts for extreme flares can be refined: the most dangerous events are unlikely before the phase corresponding to the overlapping point, about 1–2 years pre-maximum, and become increasingly probable through the decline phase.
  • A specific large-scale magnetic field signature—enhanced l=5 harmonic—can serve as a proxy for the OLP and thus as a trigger for heightened flare monitoring.
  • The dependence of extreme flare occurrence on global magnetic topology implies that flare prediction models must incorporate both local active-region properties and the surrounding coronal hole configuration.
  • For stellar astrophysics, the result implies that superflares on Sun-like stars are not uniformly distributed in activity cycles; they should be concentrated in the analogous decline phase, offering a testable prediction for stellar flare surveys.

Reading between the lines

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

  • The claimed phase dependence can be tested on data from cycle 25, which the paper already begins to include: if the pattern holds, X10+ flares should continue through the late decline of cycle 24 and into the decline of cycle 25, with no such flares appearing before mid-2024.
  • Because the sample is limited to four cycles and 37 events, a statistical coincidence cannot be ruled out; extending the analysis to earlier GOES data or to X8-X9 flares (which are more numerous) would test whether the phase lock scales with flare energy.
  • The paper implicitly suggests that the overlapping point is a universal feature of solar-type dynamos. If so, observations of other G-type stars could look for a magnetic harmonic signature (a peak in l=5-like component) before the occurrence of extreme stellar flares.
  • The link to coronal holes implies that extreme flare activity may be anti-correlated with the strength of the axial dipole moment, because the equatorial dipole (which produces low-latitude coronal holes) dominates in the decline phase.
Original abstract

Powerful nonstationary processes such as flares and coronal mass ejections are detected mainly near the solar cycle maxima. However, the analysis of the great flares since 1975, when the GOES monitoring started, leads us to more precise conclusions. We have traced the latitudinal distribution of X-class flares and their dependence on the phase of the cycle throughout four cycles. Besides, we compared directly their positions with the magnetic field structure. It was found that the relatively weak X4--7 flares occur at relatively high latitudes (15 -- 20 degrees), where two waves of activity converge, one moving toward the equator and the other, the wave of the following cycle, directed poleward. Such events are observed almost constantly 1 -- 2 years before the cycle maximum. At the same time, the number of the powerful X-ray flares increases sharply during the maximum phase, but the greatest X10 flares are observed at the beginning of the decline phase, where wave interactions still persist, and throughout the decline phase. Note that they are virtually absent during the cycle growth phase. Thus, we conclude that the greatest X-ray flares begin to appear 1 -- 2 years before the maximum number of sunspots in the overlapping phase, when different kinds of activity waves coexist on the Sun at relatively high latitudes, and, then, continue to appear at the boundary, which separates the wave of local fields and the poleward wave of the following cycle.

The compiled record

The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-23: 1 request, 7,009 input tokens.

What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.12 · human participants 0.02 · controlled comparison 0.06 · randomized assignment 0.01 · states quantitative result 0.94 · compares with prior results 0.32 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

Powerful nonstationary processes such as flares and coronal mass ejections are detected mainly near the solar cycle maxima. However, the analysis of the great flares since 1975, when the GOES monitoring started, leads us to more precise conclusions. We have traced the latitudinal distribution of X-class flares and their dependence on the phase of the cycle throughout four cycles. Besides, we compared directly their positions with the magnetic field structure. It was found that the relatively weak X4--7 flares occur at relatively high latitudes (15 -- 20 degrees), where two waves of activity converge, one moving toward the equator and the other, the wave of the following cycle, directed poleward. Such events are observed almost constantly 1 -- 2 years before the cycle maximum. At the same time, the number of the powerful X-ray flares increases sharply during the maximum phase, but the greatest X10 flares are observed at the beginning of the decline phase, where wave interactions still persist, and throughout the decline phase. Note that they are virtually absent during the cycle growth phase. Thus, we conclude that the greatest X-ray flares begin to appear 1 -- 2 years before the maximum number of sunspots in the overlapping phase, when different kinds of activity waves coexist on the Sun at relatively high latitudes, and, then, continue to appear at the boundary, which separates the wave of local fields and the poleward wave of the following cycle.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 Powerful nonstationary processes such as flares and coronal mass ejections are detected mainly near the solar cycle maxima. background 1.00 0.11 0.04 asserted 1.00
s1 However, the analysis of the great flares since 1975, when the GOES monitoring started, leads us to more precise conclusions. contribution 0.56 0.75 0.02 asserted 0.89
s2 We have traced the latitudinal distribution of X-class flares and their dependence on the phase of the cycle throughout four cycles. contribution 0.77 0.96 0.03 asserted 0.96
s3 Besides, we compared directly their positions with the magnetic field structure. method 0.75 0.92 0.02 asserted 0.88
s4 It was found that the relatively weak X4--7 flares occur at relatively high latitudes (15 -- 20 degrees), where two waves of activity converge, one moving toward the equator and the other, the wave of the following cycle, directed poleward. result 1.00 0.92 0.09 asserted 1.00
s5 Such events are observed almost constantly 1 -- 2 years before the cycle maximum. result 1.00 0.84 0.04 asserted 1.00
s6 At the same time, the number of the powerful X-ray flares increases sharply during the maximum phase, but the greatest X10 flares are observed at the beginning of the decline phase, where wave interactions still persist, and throughout the decline phase. result 1.00 0.90 0.12 asserted 1.00
s7 Note that they are virtually absent during the cycle growth phase. result 1.00 0.83 0.04 asserted 1.00
s8 Thus, we conclude that the greatest X-ray flares begin to appear 1 -- 2 years before the maximum number of sunspots in the overlapping phase, when different kinds of activity waves coexist on the Sun at relatively high latitudes, and, then, continue to appear at the boundary, which separates the wave of local fields and the poleward wave of the following cycle. interpretation 0.76 0.92 0.96 asserted 1.00

What kind of paper the classifier reports this is: empirical study 1.00 · evidence from analysis of existing data 0.99.

What was examined, and what was not

sources read
  • arXiv listing abstract v1
not examined
  • full text
  • figures and tables
  • references and citing sentences
  • relations to other papers
levels run
  • P abstract
not run
  • S sections
  • T body sentences
  • C citations
  • R cross-paper relations

Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

Figures
Figure 1. Latitude-time distribution of the largest X-ray solar flares against the background of the surface magnetic field butterfly diagram shown with thin solid lines (upper panel) in comparison with the SSN cyclic variation (lower panel). The red points correspond to the flares of magnitude larger than X10, the blue ones, to the flares of magnitudes between X4 and X10
Figure 2. Time-latitude diagram for the flares under investigation
Figure 3. Synthetic time-latitude diagram for the greatest X-ray flares. Top – beginning of the cycles are identified, both kinds of lares are given as black points. Bottom – the cycles maxima are identified, vertical black line corresponds to the cycles maxima, the vertical gray strip shows the phase of maximum, red points are for the flares with magnitudes larger then X10, blue ones stand for the magnitudes between X4 and X10
Figure 4. A burning point of the wave of flares (the white ellipse on the top panel) against the surface magnetic field. On the top panel, this position is compared with space-time distribution of the surface magnetic field from Hathaway (2015)(shown in colors). The red lines mark the dates of the cycle maxima. On the lower panel, the location of the burning point is compared with the evolution of 5th harmonics of the surface solar magnetic field. 1-2 years before the maximum, relatively weak flares of magnitude X4-X7 appear, and subsequently, such flares occur throughout all phases of the…
Figure 5. Relation between the SXR class and the phase of the activity cycle. The vertical line shows the cycle maximum, the gray vertical strip stands for the phase of maximum. The dots indicate flares
Figure 6. Solar activity on October 29, 2003. Left - the magnetogram; right - the image in λ284A. Consider as an example the situation in october-november 2003. AR 10486 produced a large number of powerful flares (“halloween” series). The region passed through the central meridian on 29.10.2003 at the latitude S19. In the vicinity of the main active region, a few other large AR and an equatorial hole (see Fig.6) were observed to form a single activity complex. This structure is characteristic of global complexes of activity. The concept has been discussed by different authors for nearly 90…

Figures reproduced from arXiv:2609.09435 by the authors.

References

Discussion

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