A 4200-hour HyperFlash and \'ECLAT campaign on the hyperactive FRB 20240114A: constraining energetics with the most brilliant bursts
Pith reviewed 2026-05-20 09:12 UTC · model grok-4.3
The pith
Highest-energy bursts from FRB 20240114A release twice the total radio energy of thousands of weaker bursts.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The 4200-hour HyperFlash and ECLAT campaign detected 178 bursts with energies from 10 to the 40 to 10 to the 42 erg, for a cumulative radio energy of 4.4 times 10 to the 42 erg assuming isotropic emission and 1-GHz bandwidth. This cumulative energy is about twice that of roughly 11,000 lower-energy bursts detected with FAST. The single most brilliant burst, termed the STROOP, contributes roughly one-third of the total energy and reaches the maximum energy seen across studies of both repeating and apparently one-off FRBs.
What carries the argument
The cumulative radio-energy sum of the 178 high-energy bursts compared against the much larger sample of lower-energy bursts, which demonstrates the dominant contribution of the rarest events to overall energy depletion.
If this is right
- The rarest, highest-energy bursts play the main role in depleting the central engine's stored energy.
- The burst energy distribution shows a clear break near 2 times 10 to the 40 erg.
- Dispersion measure rises linearly by 0.96 plus or minus 0.06 pc cm to the minus 3 over 318 days.
- The measured energetics can be compared directly to intermediate and giant flares from Galactic magnetars.
Where Pith is reading between the lines
- If the energy-distribution break appears in other repeaters, it may mark a shared physical cutoff in the emission mechanism.
- Longer monitoring could check whether single-burst dominance of the energy budget is common among hyperactive sources.
- The observed DM increase offers a measurable probe of evolving local plasma that future observations can track for changes in rate or direction.
Load-bearing premise
Absolute energies are calculated assuming isotropic emission and a 1-GHz emission bandwidth; if either assumption fails, all energy values and comparisons to other FRBs scale by an unknown factor.
What would settle it
A future campaign that measures more total energy from the numerous lower-energy bursts than from the high-energy sample under identical assumptions, or records a burst whose energy clearly exceeds the current observed maximum.
Figures
read the original abstract
Hyperactive repeaters provide a unique window into the evolving environments and energy budgets of fast radio burst (FRB) sources, though they may not be representative of the FRB population in general. High-cadence observations are key to capturing the rarest and most energetic bursts, which occur only once per hundreds to thousands of hours. Here we present an unprecedented $4{,}200$-hour observing campaign targeting FRB 20240114A as part of the HyperFlash and \'ECLAT FRB monitoring programs. Over $806$ days, we detected $178$ high-energy ($\sim$$10^{40-42}$ erg) bursts with HyperFlash, which together amount to $4.4 \times 10^{42}$ erg of released radio energy (assuming isotropic emission and 1-GHz emission bandwidth). The cumulative energy of the HyperFlash bursts is about twice that of $\sim$$11{,}000$ lower-energy bursts detected with FAST, emphasising the significant role that the highest-energy bursts play in depleting the central engine's stored energy. In fact, the single most brilliant burst from our sample, which we term the STROOP, contributes roughly $1/3$ of all the energy we measure, and is at the maximum energy seen in studies of both repeating and apparently one-off FRBs alike. We also find a break in the burst energy distribution at $\sim$$2\times10^{40}$ erg and a linear dispersion measure (DM) increase of $+0.96 \pm 0.06$ pc cm$^{-3}$ over a period of $318$ days. We discuss these findings in the context of a magnetar source model and highlight comparisons with the energetics of intermediate and giant X-ray/$\gamma$-ray flares from Galactic sources.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This paper presents findings from an extensive 4,200-hour radio observation campaign targeting the hyperactive repeating fast radio burst FRB 20240114A, conducted under the HyperFlash and ECLAT programs. The authors report detecting 178 high-energy bursts (~10^40-42 erg) over 806 days, with a cumulative radio energy release of 4.4 × 10^42 erg assuming isotropic emission and a 1 GHz bandwidth. This total is claimed to be approximately twice the energy from ~11,000 lower-energy bursts observed by FAST, underscoring the importance of the most energetic events. A standout burst termed the 'STROOP' is said to account for roughly one-third of the measured energy and matches the highest energies seen in both repeating and apparently non-repeating FRBs. Additional results include a break in the burst energy distribution around 2 × 10^40 erg and a linear dispersion measure (DM) increase of +0.96 ± 0.06 pc cm^{-3} over 318 days. These are interpreted within a magnetar central engine framework, with comparisons to X-ray and gamma-ray flares from Galactic sources.
Significance. Should the energy calculations prove accurate with proper error analysis and completeness, this study significantly advances understanding of FRB energy budgets by demonstrating that infrequent, high-energy bursts can dominate the total energy output, potentially depleting the source's reservoir more efficiently than numerous low-energy events. The long-term monitoring provides a valuable dataset for tracking environmental changes via the DM trend. The work merits credit for its high-cadence, long-duration observations that captured these rare events and for placing the results in the context of magnetar flare energetics, offering a bridge between repeating FRBs and other high-energy astrophysical phenomena.
major comments (2)
- Abstract and §4 (Results on energetics): The total energy of 4.4 × 10^{42} erg is presented without error bars, uncertainty propagation, or discussion of detection thresholds and completeness corrections for the 178 bursts. This is load-bearing for the central claim that the HyperFlash cumulative energy is twice the FAST sample and that the highest-energy bursts dominate depletion of the central engine.
- §3 (Energy and distance conversion): The manuscript does not specify the luminosity distance, redshift, or host galaxy assumptions used to convert observed quantities to erg, nor does it propagate uncertainties from these into the reported totals or the STROOP fraction. This directly affects the absolute scale needed for comparisons to other FRB studies and Galactic magnetar flares.
minor comments (2)
- The acronym 'STROOP' for the brightest burst should be defined on first use in the abstract and introduction with a brief note on its fluence or peak flux.
- Figure showing the energy distribution (presumably in §4) should explicitly mark the reported break at ~2×10^{40} erg and include the fitted parameters with uncertainties.
Simulated Author's Rebuttal
We thank the referee for their careful reading of the manuscript and for highlighting the importance of rigorous error analysis and clear assumptions in our energy calculations. We address each major comment below and will revise the manuscript to strengthen these aspects of the presentation.
read point-by-point responses
-
Referee: Abstract and §4 (Results on energetics): The total energy of 4.4 × 10^{42} erg is presented without error bars, uncertainty propagation, or discussion of detection thresholds and completeness corrections for the 178 bursts. This is load-bearing for the central claim that the HyperFlash cumulative energy is twice the FAST sample and that the highest-energy bursts dominate depletion of the central engine.
Authors: We agree that the total energy estimate requires explicit uncertainty treatment to support the central claims. In the revised manuscript we will add error bars to the cumulative radio energy, describe the propagation of fluence uncertainties for the 178 bursts, and include a dedicated discussion of detection thresholds and completeness corrections above the relevant energy range. We will also clarify the comparison to the FAST sample by noting differences in sensitivity and energy coverage, thereby reinforcing that the highest-energy events dominate the observed energy release. revision: yes
-
Referee: §3 (Energy and distance conversion): The manuscript does not specify the luminosity distance, redshift, or host galaxy assumptions used to convert observed quantities to erg, nor does it propagate uncertainties from these into the reported totals or the STROOP fraction. This directly affects the absolute scale needed for comparisons to other FRB studies and Galactic magnetar flares.
Authors: We thank the referee for noting this omission. In the revised §3 we will explicitly state the luminosity distance, redshift, and host-galaxy association adopted for FRB 20240114A, together with the cosmological parameters used. We will propagate the associated uncertainties into the total energy, the STROOP fraction, and all derived energetics so that absolute scales and comparisons to other FRB and magnetar-flare studies are placed on a transparent footing. revision: yes
Circularity Check
No circularity: energies and comparisons derived directly from new observations under explicit assumptions
full rationale
The paper reports burst detections and energy sums from a new 4200-hour campaign on FRB 20240114A. Cumulative radio energy (4.4e42 erg) is obtained by summing individual burst fluences converted under the stated isotropic + 1 GHz assumptions; the factor-of-two comparison to the external FAST sample and the 1/3 contribution of the brightest burst follow arithmetically from those sums. No equations, fits, or self-citations are invoked that reduce the reported totals or ratios back to the inputs by construction. The assumptions are flagged as such and affect absolute scale uniformly, but do not create definitional or fitted-input circularity within the derivation chain.
Axiom & Free-Parameter Ledger
free parameters (2)
- 1-GHz emission bandwidth
- isotropic emission
axioms (1)
- domain assumption The redshift or luminosity distance to FRB 20240114A is known and can be used to convert observed flux to isotropic-equivalent energy.
Lean theorems connected to this paper
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
assuming isotropic emission and 1-GHz emission bandwidth... cumulative energy of the HyperFlash bursts is about twice that of ~11,000 lower-energy bursts... break in the burst energy distribution at ~2×10^40 erg
-
IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
discuss these findings in the context of a magnetar source model and highlight comparisons with the energetics of intermediate and giant X-ray/γ-ray flares
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
Abbott T. C., et al., 2025, @doi [ ] 10.3847/1538-3881/ad9451 , https://ui.adsabs.harvard.edu/abs/2025AJ....169...39A 169, 39
-
[2]
Radio Monitoring Campaign of Active Repeater FRB 20220912A with CHIME
Abbott T. C., et al., 2026, @doi [arXiv e-prints] 10.48550/arXiv.2604.09098 , https://ui.adsabs.harvard.edu/abs/2026arXiv260409098A p. arXiv:2604.09098
work page internal anchor Pith review Pith/arXiv arXiv doi:10.48550/arxiv.2604.09098 2026
-
[3]
Agarwal D., Aggarwal K., Burke-Spolaor S., Lorimer D. R., Garver-Daniels N., 2020, @doi [ ] 10.1093/mnras/staa1856 , https://ui.adsabs.harvard.edu/abs/2020MNRAS.497.1661A 497, 1661
-
[4]
Alstott J., Bullmore E., Plenz D., 2014, @doi [PLoS ONE] 10.1371/journal.pone.0085777 , https://ui.adsabs.harvard.edu/abs/2014PLoSO...985777A 9, e85777
-
[5]
Anna-Thomas R., et al., 2023, @doi [Science] 10.1126/science.abo6526 , https://ui.adsabs.harvard.edu/abs/2023Sci...380..599A 380, 599
-
[6]
Aschwanden M. J., et al., 2016, @doi [ ] 10.1007/s11214-014-0054-6 , https://ui.adsabs.harvard.edu/abs/2016SSRv..198...47A 198, 47
-
[7]
Astropy Collaboration et al., 2013, @doi [ ] 10.1051/0004-6361/201322068 , http://adsabs.harvard.edu/abs/2013A\
-
[8]
Astropy Collaboration et al., 2018, @doi [ ] 10.3847/1538-3881/aabc4f , https://ui.adsabs.harvard.edu/abs/2018AJ....156..123A 156, 123
-
[9]
Astropy Collaboration et al., 2022, @doi [ ] 10.3847/1538-4357/ac7c74 , https://ui.adsabs.harvard.edu/abs/2022ApJ...935..167A 935, 167
work page internal anchor Pith review doi:10.3847/1538-4357/ac7c74 2022
-
[10]
Bak P., Tang C., Wiesenfeld K., 1987, @doi [ ] 10.1103/PhysRevLett.59.381 , https://ui.adsabs.harvard.edu/abs/1987PhRvL..59..381B 59, 381
-
[11]
Barr E. D., et al., 2013, @doi [Monthly Notices of the Royal Astronomical Society] 10.1093/mnras/stt1440 , 435, 2234
-
[12]
Barsdell B. R., Bailes M., Barnes D. G., Fluke C. J., 2012, @doi [ ] 10.1111/j.1365-2966.2012.20622.x , https://ui.adsabs.harvard.edu/abs/2012MNRAS.422..379B 422, 379
-
[13]
Beniamini P., Kumar P., 2025, @doi [ ] 10.3847/1538-4357/adb8e6 , https://ui.adsabs.harvard.edu/abs/2025ApJ...982...45B 982, 45
-
[14]
Beniamini P., Wadiasingh Z., Trigg A., Chirenti C., Burns E., Younes G., Negro M., Granot J., 2025, @doi [ ] 10.3847/1538-4357/ada947 , https://ui.adsabs.harvard.edu/abs/2025ApJ...980..211B 980, 211
-
[15]
Bhardwaj M., et al., 2025, @doi [ ] 10.3847/2041-8213/ae0b68 , https://ui.adsabs.harvard.edu/abs/2025ApJ...992L..35B 992, L35
-
[16]
Bochenek C. D., Ravi V., Belov K. V., Hallinan G., Kocz J., Kulkarni S. R., McKenna D. L., 2020, @doi [ ] 10.1038/s41586-020-2872-x , https://ui.adsabs.harvard.edu/abs/2020Natur.587...59B 587, 59
-
[17]
Bransgrove A., Beloborodov A. M., Levin Y., 2026, @doi [ ] 10.3847/2041-8213/ae50f2 , https://ui.adsabs.harvard.edu/abs/2026ApJ..1001L..13B 1001, L13
-
[18]
Burns E., et al., 2021, @doi [ ] 10.3847/2041-8213/abd8c8 , https://ui.adsabs.harvard.edu/abs/2021ApJ...907L..28B 907, L28
-
[19]
CHIME/FRB Collaboration et al., 2018, @doi [ ] 10.3847/1538-4357/aad188 , https://ui.adsabs.harvard.edu/abs/2018ApJ...863...48C 863, 48
-
[20]
CHIME/FRB Collaboration et al., 2020, @doi [ ] 10.1038/s41586-020-2863-y , https://ui.adsabs.harvard.edu/abs/2020Natur.587...54C 587, 54
-
[21]
CHIME/FRB Collaboration et al., 2026, @doi [ ] 10.3847/1538-4365/ae3828 , https://ui.adsabs.harvard.edu/abs/2026ApJS..283...34C 283, 34
-
[22]
Caleb M., et al., 2025, @doi [arXiv e-prints] 10.48550/arXiv.2508.01648 , https://ui.adsabs.harvard.edu/abs/2025arXiv250801648C p. arXiv:2508.01648
-
[23]
, year = 1996, month = aug, volume =
Cheng B., Epstein R. I., Guyer R. A., Young A. C., 1996, @doi [ ] 10.1038/382518a0 , https://ui.adsabs.harvard.edu/abs/1996Natur.382..518C 382, 518
-
[24]
Cook A. M., et al., 2026, arXiv e-prints, https://ui.adsabs.harvard.edu/abs/2026arXiv260508410C p. arXiv:2605.08410
work page internal anchor Pith review Pith/arXiv arXiv 2026
-
[25]
Cooper A. J., Wijers R. A. M. J., 2021, @doi [ ] 10.1093/mnrasl/slab099 , https://ui.adsabs.harvard.edu/abs/2021MNRAS.508L..32C 508, L32
-
[26]
, year = 1970, month = nov, volume =
Crawford D. F., Jauncey D. L., Murdoch H. S., 1970, @doi [ ] 10.1086/150672 , https://ui.adsabs.harvard.edu/abs/1970ApJ...162..405C 162, 405
-
[27]
Eppel F., et al., 2025, @doi [ ] 10.1051/0004-6361/202453563 , https://ui.adsabs.harvard.edu/abs/2025A&A...695L..10E 695, L10
-
[28]
Ester M., Kriegel H.-P., Sander J., Xu X., 1996, in Proceedings of the Second International Conference on Knowledge Discovery and Data Mining. KDD'96. AAAI Press, p. 226–231
work page 1996
-
[29]
G \"o tz D., et al., 2006, @doi [ ] 10.1051/0004-6361:20053648 , https://ui.adsabs.harvard.edu/abs/2006A&A...445..313G 445, 313
-
[30]
Gourdji K., Michilli D., Spitler L. G., Hessels J. W. T., Seymour A., Cordes J. M., Chatterjee S., 2019, @doi [ ] 10.3847/2041-8213/ab1f8a , https://ui.adsabs.harvard.edu/abs/2019ApJ...877L..19G 877, L19
-
[31]
M., Kouveliotou C., van Paradijs J., Briggs M
G \"o g \"u s E., Woods P. M., Kouveliotou C., van Paradijs J., Briggs M. S., Duncan R. C., Thompson C., 1999, @doi [ ] 10.1086/312380 , https://ui.adsabs.harvard.edu/abs/1999ApJ...526L..93G 526, L93
-
[32]
M., Kouveliotou C., van Paradijs J., Briggs M
G \"o g \"u s E., Woods P. M., Kouveliotou C., van Paradijs J., Briggs M. S., Duncan R. C., Thompson C., 2000, @doi [ ] 10.1086/312583 , https://ui.adsabs.harvard.edu/abs/2000ApJ...532L.121G 532, L121
-
[33]
Gupta V., et al., 2021, @doi [ ] 10.1093/mnras/staa3683 , https://ui.adsabs.harvard.edu/abs/2021MNRAS.501.2316G 501, 2316
-
[34]
Harris C. R., et al., 2020, @doi [Nature] 10.1038/s41586-020-2649-2 , 585, 357
-
[35]
Hewitt D. M., et al., 2022, @doi [ ] 10.1093/mnras/stac1960 , https://ui.adsabs.harvard.edu/abs/2022MNRAS.515.3577H 515, 3577
-
[36]
Hewitt D. M., et al., 2023, @doi [ ] 10.1093/mnras/stad2847 , https://ui.adsabs.harvard.edu/abs/2023MNRAS.526.2039H 526, 2039
-
[37]
Hewitt D. M., Huang J., Hessels J. W. T., Cognard I., Guillemot L., Ould-Boukattine O. S., Snelders M. P., Kirsten F., 2024, The Astronomer's Telegram, https://ui.adsabs.harvard.edu/abs/2024ATel16597....1H 16597, 1
work page 2024
-
[38]
Huang Y.-X., et al., 2025, @doi [Research in Astronomy and Astrophysics] 10.1088/1674-4527/ade34e , https://ui.adsabs.harvard.edu/abs/2025RAA....25h5009H 25, 085009
-
[39]
Matplotlib: A 2D Graphics Environment
Hunter J. D., 2007, @doi [Computing in Science & Engineering] 10.1109/MCSE.2007.55 , 9, 90
-
[40]
Hurley K., et al., 1999, @doi [ ] 10.1038/16199 , https://ui.adsabs.harvard.edu/abs/1999Natur.397...41H 397, 41
-
[41]
Ibrahim A. I., et al., 2001, @doi [ ] 10.1086/322248 , https://ui.adsabs.harvard.edu/abs/2001ApJ...558..237I 558, 237
-
[42]
James C. W., Ekers R. D., Macquart J. P., Bannister K. W., Shannon R. M., 2019, @doi [ ] 10.1093/mnras/sty3031 , https://ui.adsabs.harvard.edu/abs/2019MNRAS.483.1342J 483, 1342
-
[43]
Kaspi V. M., Beloborodov A. M., 2017, @doi [ ] 10.1146/annurev-astro-081915-023329 , https://ui.adsabs.harvard.edu/abs/2017ARA&A..55..261K 55, 261
-
[44]
Keimpema A., et al., 2015, @doi [Experimental Astronomy] 10.1007/s10686-015-9446-1 , https://ui.adsabs.harvard.edu/abs/2015ExA....39..259K 39, 259
-
[45]
Kirsten F., Snelders M. P., Jenkins M., Nimmo K., van den Eijnden J., Hessels J. W. T., Gawro \'n ski M. P., Yang J., 2021, @doi [Nature Astronomy] 10.1038/s41550-020-01246-3 , https://ui.adsabs.harvard.edu/abs/2021NatAs...5..414K 5, 414
-
[46]
Kirsten F., et al., 2024, @doi [Nature Astronomy] 10.1038/s41550-023-02153-z , https://ui.adsabs.harvard.edu/abs/2024NatAs...8..337K 8, 337
- [47]
-
[48]
Konijn D. C., et al., 2024, @doi [ ] 10.1093/mnras/stae2296 , https://ui.adsabs.harvard.edu/abs/2024MNRAS.534.3331K 534, 3331
-
[49]
Lander S. K., Gourgouliatos K. N., Wadiasingh Z., Antonopoulou D., 2026, @doi [ ] 10.3847/2041-8213/ae31f5 , https://ui.adsabs.harvard.edu/abs/2026ApJ...997L...7L 997, L7
-
[50]
Li C. K., et al., 2021a, @doi [Nature Astronomy] 10.1038/s41550-021-01302-6 , https://ui.adsabs.harvard.edu/abs/2021NatAs...5..378L 5, 378
-
[51]
Li D., et al., 2021b, @doi [ ] 10.1038/s41586-021-03878-5 , https://ui.adsabs.harvard.edu/abs/2021Natur.598..267L 598, 267
-
[52]
Limaye P., Spitler L. G., Manaswini N., Ben \'a c ek J., Eppel F., Kadler M., Nicotera L., Wongphechauxsorn J., 2025, @doi [arXiv e-prints] 10.48550/arXiv.2510.08367 , https://ui.adsabs.harvard.edu/abs/2025arXiv251008367L p. arXiv:2510.08367
work page internal anchor Pith review Pith/arXiv arXiv doi:10.48550/arxiv.2510.08367 2025
-
[53]
Lu W., Kumar P., 2019, @doi [ ] 10.1093/mnrasl/sly200 , https://ui.adsabs.harvard.edu/abs/2019MNRAS.483L..93L 483, L93
-
[54]
Luo J.-W., et al., 2025, @doi [ ] 10.3847/1538-4357/ade0b9 , https://ui.adsabs.harvard.edu/abs/2025ApJ...988...62L 988, 62
-
[55]
Lyubarsky Y., 2014, @doi [ ] 10.1093/mnrasl/slu046 , https://ui.adsabs.harvard.edu/abs/2014MNRAS.442L...9L 442, L9
-
[56]
Macquart J. P., Ekers R., 2018, @doi [ ] 10.1093/mnras/sty2083 , https://ui.adsabs.harvard.edu/abs/2018MNRAS.480.4211M 480, 4211
-
[57]
Manaswini N., et al., 2026, arXiv e-prints
work page 2026
-
[58]
Marcote B., Kirsten F., Hessels J., Nimmo K., Paragi Z., Project P., 2022, in European VLBI Network Mini-Symposium and Users' Meeting 2021. p. 35 ( @eprint arXiv 2202.11644 ), @doi 10.22323/1.399.0035
-
[59]
Margalit B., Beniamini P., Sridhar N., Metzger B. D., 2020, @doi [ ] 10.3847/2041-8213/abac57 , https://ui.adsabs.harvard.edu/abs/2020ApJ...899L..27M 899, L27
-
[60]
Mazets E. P., Golentskii S. V., Ilinskii V. N., Aptekar R. L., Guryan I. A., 1979, @doi [ ] 10.1038/282587a0 , https://ui.adsabs.harvard.edu/abs/1979Natur.282..587M 282, 587
-
[61]
Mckinven R., et al., 2023, @doi [ ] 10.3847/1538-4357/acc65f , https://ui.adsabs.harvard.edu/abs/2023ApJ...950...12M 950, 12
-
[62]
Mereghetti S., et al., 2020, @doi [ ] 10.3847/2041-8213/aba2cf , https://ui.adsabs.harvard.edu/abs/2020ApJ...898L..29M 898, L29
-
[63]
Metzger B. D., Margalit B., Sironi L., 2019, @doi [ ] 10.1093/mnras/stz700 , https://ui.adsabs.harvard.edu/abs/2019MNRAS.485.4091M 485, 4091
-
[64]
Michilli D., et al., 2018, @doi [ ] 10.1038/nature25149 , https://ui.adsabs.harvard.edu/abs/2018Natur.553..182M 553, 182
-
[65]
Moroianu A. M., et al., 2026, @doi [ ] 10.3847/2041-8213/ae28c7 , https://ui.adsabs.harvard.edu/abs/2026ApJ...996L..16M 996, L16
-
[66]
Nimmo K., et al., 2021, @doi [Nature Astronomy] 10.1038/s41550-021-01321-3 , https://ui.adsabs.harvard.edu/abs/2021NatAs...5..594N 5, 594
-
[67]
Nimmo K., et al., 2023, @doi [ ] 10.1093/mnras/stad269 , https://ui.adsabs.harvard.edu/abs/2023MNRAS.520.2281N 520, 2281
-
[68]
Ould-Boukattine O. S., et al., 2024, The Astronomer's Telegram, https://ui.adsabs.harvard.edu/abs/2024ATel16432....1O 16432, 1
work page 2024
-
[69]
Ould-Boukattine O. S., et al., 2025, The Astronomer's Telegram, https://ui.adsabs.harvard.edu/abs/2025ATel16967....1O 16967, 1
work page 2025
-
[70]
Ould-Boukattine O. S., et al., 2026a, @doi [ ] 10.1093/mnras/staf1937 , https://ui.adsabs.harvard.edu/abs/2026MNRAS.545f1937O 545, staf1937
-
[71]
Ould-Boukattine O. S., et al., 2026b, @doi [ ] 10.1093/mnras/stag090 , https://ui.adsabs.harvard.edu/abs/2026MNRAS.546ag090O 546, stag090
-
[72]
Palmer D. M., et al., 2005, @doi [ ] 10.1038/nature03525 , https://ui.adsabs.harvard.edu/abs/2005Natur.434.1107P 434, 1107
-
[73]
Panda U., Roy J., Bhattacharyya S., Dudeja C., Kudale S., 2025, @doi [ ] 10.3847/1538-4357/adeb74 , https://ui.adsabs.harvard.edu/abs/2025ApJ...989...15P 989, 15
-
[74]
Pandhi A., et al., 2026, @doi [ ] 10.3847/2041-8213/ae52f8 , https://ui.adsabs.harvard.edu/abs/2026ApJ..1000L..53P 1000, L53
-
[75]
Pelliciari D., Geminardi A., Bernardi G., Pilia M., Esposito P., Naldi G., 2024, The Astronomer's Telegram, https://ui.adsabs.harvard.edu/abs/2024ATel16434....1P 16434, 1
work page 2024
-
[76]
Perez F., Granger B. E., 2007, @doi [Computing in Science and Engineering] 10.1109/MCSE.2007.53 , https://ui.adsabs.harvard.edu/abs/2007CSE.....9c..21P 9, 21
-
[77]
Petroff E., Hessels J. W. T., Lorimer D. R., 2022, @doi [ ] 10.1007/s00159-022-00139-w , https://ui.adsabs.harvard.edu/abs/2022A&ARv..30....2P 30, 2
-
[78]
Pleunis Z., et al., 2021, @doi [ ] 10.3847/1538-4357/ac33ac , https://ui.adsabs.harvard.edu/abs/2021ApJ...923....1P 923, 1
-
[79]
Hyperflares of SGRs as an engine for millisecond extragalactic radio bursts
Popov S. B., Postnov K. A., 2010, in Harutyunian H. A., Mickaelian A. M., Terzian Y., eds, Evolution of Cosmic Objects through their Physical Activity. pp 129--132 ( @eprint arXiv 0710.2006 ), @doi 10.48550/arXiv.0710.2006
work page internal anchor Pith review Pith/arXiv arXiv doi:10.48550/arxiv.0710.2006 2010
-
[80]
Ransom S., 2011, PRESTO: PulsaR Exploration and Search TOolkit , Astrophysics Source Code Library, record ascl:1107.017 ( @eprint ascl 1107.017 )
work page 2011
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.