REVIEW 3 major objections 5 minor 104 references
Hunting Star-Forming Galaxies in the Gamma-Ray Domain
T0 review · 3 major / 5 minor · reviewed 2026-08-16 · deepseek-v4-flash
Pith's one-line read The paper claims that almost a dozen star-forming galaxies, led by NGC 253, M82, NGC 1068, NGC 4945, and Circinus, may be detectable in the TeV band by the upcoming Cherenkov Telescope Array Observatory.
desk verdict Useful target-selection census for next-gen TeV observatories, but the 'almost a dozen' count rests on a calibration that could be off by a factor of two. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The load-bearing relation is the observationally calibrated correlation between gamma-ray luminosity at 2 GeV and star formation rate, $L_{\gamma,2\,\mathrm{GeV}} = C\,\dot{M}_*^m$, converted into a flux prediction by $F(E) = L_{2\,\mathrm{GeV}}(\mathrm{SFR})/(4\pi d^2) \times (E/2\,\mathrm{GeV})^{2-\alpha} e^{-\tau(E,z)}$ with $\alpha = 2.2$ and EBL optical depth $\tau$. A second channel uses the straight power-law extrapolation of the 4FGL-DR4 spectra. Both are compared with the differential point-source sensitivity of CTAO, LHAASO, and SWGO, computed with the published instrument response functions.
What would settle it
A CTAO campaign reaching the 50-hour sensitivity at the predicted flux on NGC 1068, NGC 4945, and Circinus that finds no source would contradict the paper's central detection claim; likewise, measuring a spectral break in NGC 253 or M82 above roughly 10 TeV would show the unbroken power-law assumption fails and would lower the expected detectability of the ULIRGs.
Extended reading notes
Core claim
The paper claims that the GeV band already contains the raw material for TeV discoveries: extrapolating the Fermi-LAT spectra of the 14 GeV-detected galaxies, or scaling a 2 GeV luminosity to star formation rate, places NGC 253, M82, NGC 1068, NGC 4945, and Circinus above the CTAO 50-hour sensitivity curve, and M83 and M33 at its threshold. A revised correlation $L_{\gamma,2\,\mathrm{GeV}} = C\,\dot{M}_*^m$ with $m = 1.27 \pm 0.10$ (or $m = 1.31 \pm 0.08$ after removing five outliers) provides the normalization for the empirical model. The paper therefore concludes that almost a dozen star-forming galaxies may be detectable by upcoming gamma-ray telescopes, a significant increase over the two known TeV starbursts.
Load-bearing premise
The predictions assume the GeV power law continues unbroken to TeV energies with photon index 2.2, attenuated only by the extragalactic background light, while gamma-ray absorption inside the host galaxy, potentially strong in starbursts and ultraluminous infrared galaxies, is not modeled.
Editorial extensions
If this is right
- If the predictions hold, CTAO will go from two TeV star-forming galaxies (NGC 253 and M82) to roughly a dozen, enabling the first population-level study of TeV emission from star-forming galaxies.
- TeV spectra of these galaxies would constrain cosmic-ray acceleration up to multi-TeV energies in extragalactic environments and test whether hadronic emission dominates outside the GeV band.
- Observations beyond 10 TeV by LHAASO or SWGO would probe internal gamma-ray absorption inside galaxies, turning the predicted cutoff into a diagnostic of the radiation field.
- The outlier galaxies NGC 3424, NGC 4945, Circinus, NGC 2403, and NGC 7059 are candidates for hidden AGN or misassociation, so TeV follow-up would help sort out the origin of their gamma-ray excesses.
Reading between the lines
- A natural extension is to stack the predicted sub-threshold TeV fluxes of the many non-detected galaxies; a stacked signal could test the SFR-gamma-ray correlation in a regime where individual detections remain out of reach.
- If internal absorption is mild, the same scaling law suggests that deeper exposures (e.g., 100 hours) would bring Arp 220, Arp 299, NGC 2403, and NGC 3424 into detectable range, making them interesting targets for a follow-up program.
- The predicted TeV luminosities can be combined with neutrino expectations for star-forming galaxies; a CTAO detection of NGC 1068 would strengthen the case that its reported neutrino signal is hadronic and connected to star formation.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper compiles a sample of 27 star-forming galaxies (14 detected by Fermi-LAT in 4FGL-DR4 and 13 not detected) and assesses their detectability at TeV energies with CTAO, LHAASO, and SWGO. The GeV analysis uses standard Fermipy procedures on roughly 15 years of Fermi-LAT data, yielding upper limits for the non-detected galaxies. The authors update the L_gamma-SFR correlation at 2 GeV using the 4FGL-detected galaxies, then predict TeV fluxes with two models: an empirical SFR-scaled power law of photon index 2.2 (Eq. 1) and a straight extrapolation of the 4FGL power laws, both attenuated by the EBL. These predictions are compared with public CTAO prod5 IRFs, LHAASO, and SWGO sensitivities. The main result is that almost a dozen star-forming galaxies may be detectable by upcoming gamma-ray telescopes, with NGC 253, M82, NGC 1068, NGC 4945, and Circinus above the CTAO 50-hour sensitivity, M83 and M33 at the threshold, and Arp 220, Arp 299, NGC 2403, and NGC 3424 as possible targets with longer exposures.
Significance. If the predictions hold, the paper provides a useful and timely target list for CTAO, LHAASO, and SWGO, extending earlier work by including non-4FGL galaxies and using updated instrument response functions. Strengths include the use of public IRFs, a standard and reproducible Fermi-LAT analysis pipeline, the validation that spectra above the differential sensitivity curves correspond to combined significance above 5 sigma, and the transparent case-by-case discussion of candidates. The main value is in identifying which galaxies deserve dedicated VHE observations and in framing the L_gamma-SFR correlation as a tool for population predictions. However, the central quantitative claim depends on a correlation normalization that is not robust to the treatment of upper limits and excluded outliers, and the 'almost a dozen' count is not tied to a crisp detectability criterion.
major comments (3)
- [Section 2.3, Eq. (1), Fig. 3, Table B.1] The empirical model that places M83 and M33 at the CTAO detection threshold is calibrated with an ODR fit to only 9 of the 14 4FGL-detected galaxies, after excluding NGC 3424, NGC 4945, Circinus, NGC 2403, and NGC 7059, and the fit ignores all 13 upper limits from Table 1. The footnote in Section 2.3 acknowledges that Ambrosone et al. estimate the normalization could shift by a factor of two if non-detected galaxies are properly accounted for, but this systematic uncertainty is not propagated into the detectability claims. A factor-of-two downward shift in the normalization is roughly four times the quoted statistical uncertainty on log C (38.19 +/- 0.08) and would push M83 and M33 below the CTAO sensitivity curve and weaken the 'o' classifications for Arp 220 and Arp 299. Please either perform a censored or mixture regression that includes the upper limits, or explicitly present the candidate list as conditional on the optimistic normalization and show how the list changes under a factor-of-two systematic shift.
- [Abstract, Section 3.2, Table B.1] The headline claim that 'almost a dozen' star-forming galaxies may be detectable is not backed by a well-defined criterion. The paper states that a spectrum above the differential sensitivity curve corresponds to a combined significance above 5 sigma, yet the 'almost a dozen' count appears to include galaxies classified as 'o' (possibility) and '?' (detailed study needed), whose spectra lie below the 50-hour sensitivity curve. Please provide a quantitative definition of 'detectable' (e.g., predicted combined significance, or flux relative to the sensitivity curve integrated over the CTAO band) and state explicitly how many galaxies satisfy that criterion, and how that number changes under the normalization uncertainty discussed above.
- [Section 3.1, Eq. (1)] The paper correctly cautions that internal gamma-ray absorption is not modeled and that results are optimistic beyond 10 TeV, but for the borderline candidates M83 and M33 the CTAO-band fluxes are controlled by sub-TeV emission, so internal absorption is not the dominant uncertainty for those objects. The dominant uncertainty is the normalization of the SFR scaling relation. The manuscript would be strengthened by separating these two caveats and by showing the predicted CTAO-band integrated flux (or significance) with a band that includes both the fit parameter uncertainties and the factor-of-two systematic, rather than only the shaded region based on the best-fit line.
minor comments (5)
- [Throughout] Several figures contain typographical spacing issues in the energy axis label, e.g., 'T eV' instead of 'TeV'; please correct these in the final version.
- [Section 2.3] The sentence 'The figure show that NGC 3424, NGC 4945, Circinus, NGC 2403 and NGC 7059 stand out...' has a subject-verb agreement error; please revise.
- [Eq. (1) and Table 2] The notation L_2GeV(SFR) in Eq. (1) would be clearer if it matched the L_gamma,2GeV notation used in Section 2.3, and if the units of each quantity in Eq. (1) were stated explicitly.
- [Table B.1] The last column header 'LHAASO, SWGO' is ambiguous because each row has a single symbol that may apply to either instrument or both; please clarify the correspondence, for example by splitting the column or defining the convention in the caption.
- [Section 3.1] The statement that a minimum of 5 signal counts per bin and 3 sigma per-bin significance are imposed would benefit from a reference or justification, since these thresholds affect the derived sensitivity curves.
Circularity Check
No significant circularity: the TeV detectability claims rest on independent Fermi-LAT extrapolations and an explicitly calibrated SFR scaling applied to new targets, with admitted non-circular caveats.
full rationale
The paper's central claims are not reductions of their inputs. Section 3.1 defines the empirical model in Eq. (1) as F = L_2GeV(SFR)/(4πd^2) × (E/2 GeV)^{2−α} e^{−τ}, where L_2GeV(SFR) is the ODR fit from Section 2.3 (m=1.31, log C=38.19). For the nine galaxies used in that fit, the empirical model is a re-expression of the fit, but the paper does not use this model as the primary evidence for their detectability: for every 4FGL-detected galaxy the detectability calls in Figs. 2–4 and Table B.1 are based on the extrapolated 4FGL-DR4 power law, an external measurement independent of the fitted correlation. The only non-detected galaxies promoted to 'interesting candidates' by the empirical model are M83 and M33 (Fig. 3), for which the model is an extrapolation of a relation calibrated on other objects, not a fit to their own fluxes; this is genuine prediction, not statistical forcing. The sample selection in Section 2.1 uses SFR/4πd^2 as a pre-filter, but the final assessment is against external CTAO/LHAASO/SWGO response functions, and the paper explicitly reports many selected galaxies as undetectable, so the comparison has content. The admitted limitations are not circular: the Section 2.3 footnote (Ambrosone et al. normalization factor-of-two) and the Section 3.1 caveat that the simple model is optimistic beyond 10 TeV due to unmodeled internal absorption are robustness concerns about a scaling-relation extrapolation and a physical assumption, respectively. No uniqueness theorem, ansatz, or fitted quantity is smuggled in under the name of prediction; the empirical model is explicitly labeled 'simple empirical model normalized to the star formation rate.'
Assumptions & free parameters
free parameters (4)
- slope m of Lgamma-SFR correlation =
1.27 +/- 0.10 (all); 1.31 +/- 0.08 (excluding 5 outliers)
- normalization C of Lgamma-SFR correlation =
log C = 38.28 +/- 0.10 (all); 38.19 +/- 0.08 (fiducial)
- photon index alpha = 2.2 =
2.2
- selection threshold alpha = 1/3.5 relative to NGC 253 =
0.286
assumptions (4)
- domain assumption The GeV-to-TeV gamma-ray emission of star-forming galaxies is dominated by hadronic pion decay and follows a power law with index near 2.2.
- domain assumption The SFR values from FUV, H-alpha, and IR tracers, and the MANGROVE stellar-mass-based SFRs, are reliable proxies for the cosmic-ray injection power.
- domain assumption The Fermi-LAT 4FGL-DR4 associations with SFGs are correct, including the contested association of 4FGL J0737.4+6535 with NGC 2403.
- standard math EBL attenuation follows the Dominguez et al. (2011) model.
Cite this review
Pith. "Pith review of Hunting Star-Forming Galaxies in the Gamma-Ray Domain." pith.science (2026). https://pith.science/paper/JWSFEUWR
@misc{pith2026250417024,
author = {Pith},
title = {Pith review of: Hunting Star-Forming Galaxies in the Gamma-Ray Domain},
year = {2026},
howpublished = {\url{https://pith.science/paper/JWSFEUWR}},
note = {Machine review of arXiv:2504.17024}
}
read the original abstract
Context. Star-forming galaxies emit {\gamma}rays with relatively low luminosity, but the study of their emission is no less captivating. While it is known that their {\gamma}-ray luminosity in the GeV band is strongly linked to their star formation, the origin of their emission at higher energies remains uncertain due to limited observations. Aims. Our aim is to assemble the largest possible sample of star-forming galaxies with potential detectability by the new-generation of Cherenkov telescopes. Methods. To achieve this, we compile a comprehensive sample of galaxies, including those previously detected by Fermi-LAT in the GeV energy range as well as a larger sample of star-forming galaxies in the Local Volume that have been cataloged in the near-infrared band. We estimate their {\gamma}-ray flux assuming a proportional relationship with their star formation rate, and then select the brightest candidates. The predicted spectra in the TeV band are derived using a simple empirical model normalized to the star formation rate and a model based on extrapolating the latest Fermi-LAT data to higher energies. The ground-based detectability of {\gamma}-ray emission from these sources is assessed through a comparison to the most recent instrument response functions. Results. Our investigation reveals that almost a dozen star-forming galaxies may be detectable by upcoming {\gamma}-ray telescopes. Conclusions. The observation of numerous star-forming galaxies in the TeV band is a fundamental piece of the panchromatic puzzle for understanding the physics inside these galaxies. The significant increase in the number of galaxies that can be studied in detail in the near future, particularly with the Cherenkov Telescope Array Observatory, promises a major step forward in the study of the conditions of acceleration and transport of cosmic rays in nearby extragalactic environments.
Figures
Reference graph
Works this paper leans on
-
[1]
A., Ackermann , M., Ajello , M., et al
Abdo , A. A., Ackermann , M., Ajello , M., et al. 2010 a , , 188, 405
2010
-
[2]
A., Ackermann , M., Ajello , M., et al
Abdo , A. A., Ackermann , M., Ajello , M., et al. 2010 b , , 523, L2
2010
-
[3]
2012, , 757, 158
Abramowski , A., Acero , F., Aharonian , F., et al. 2012, , 757, 158
2012
-
[4]
A., Ansoldi , S., Antonelli , L
Acciari , V. A., Ansoldi , S., Antonelli , L. A., et al. 2019, , 883, 135
2019
-
[5]
2023, , 523, 5353
Acharyya , A., Adam , R., Aguasca-Cabot , A., et al. 2023, , 523, 5353
2023
-
[6]
2017, , 836, 208
Ackermann , M., Ajello , M., Albert , A., et al. 2017, , 836, 208
2017
-
[7]
2012, , 755, 164
Ackermann , M., Ajello , M., Allafort , A., et al. 2012, , 755, 164
2012
-
[8]
S., & Garrappa , S
Ajello , M., Di Mauro , M., Paliya , V. S., & Garrappa , S. 2020, , 894, 88
2020
Show all 104 references
-
[9]
2019, arXiv e-prints, arXiv:1902.08429
Albert , A., Alfaro , R., Ashkar , H., et al. 2019, arXiv e-prints, arXiv:1902.08429
2019 arXiv
-
[10]
Ambrosone , A., Chianese , M., Fiorillo , D. F. G., Marinelli , A., & Miele , G. 2021, , 919, L32
2021
-
[11]
2024, , 2024, 040
Ambrosone , A., Chianese , M., & Marinelli , A. 2024, , 2024, 040
2024
-
[12]
Antonucci , R. R. J. & Miller , J. S. 1985, , 297, 621
1985
-
[13]
I., Leer , E., & Skadron , G
Axford , W. I., Leer , E., & Skadron , G. 1977, in International Cosmic Ray Conference, Vol. 11, International Cosmic Ray Conference, 132
1977
-
[14]
H., Lott , B., & The Fermi-LAT collaboration
Ballet , J., Bruel , P., Burnett , T. H., Lott , B., & The Fermi-LAT collaboration . 2023, arXiv e-prints, arXiv:2307.12546
2023 arXiv
-
[15]
Bell , A. R. 1978, , 182, 147
1978
-
[16]
Bell , E. F. 2003, , 586, 794
2003
-
[17]
2021, , 256, 15
Biteau , J. 2021, , 256, 15
2021
-
[18]
& Meyer , M
Biteau , J. & Meyer , M. 2022, Galaxies, 10, 39
2022
-
[19]
J., Paglione , T
Blom , J. J., Paglione , T. A. D., & Carrami \ n ana , A. 1999, , 516, 744
1999
-
[20]
Bouquin , A. Y. K., Gil de Paz , A., Mu \ n oz-Mateos , J. C., et al. 2018, , 234, 18
2018
-
[21]
K., & Taylor , G
Bruzewski , S., Schinzel , F. K., & Taylor , G. B. 2023, , 943, 51
2023
-
[22]
Bykov , A. M. & Fleishman , G. D. 1992, , 255, 269
1992
-
[23]
2019, arXiv e-prints, arXiv:1905.02773
Cao , Z., della Volpe , D., Liu , S., et al. 2019, arXiv e-prints, arXiv:1905.02773
2019
-
[24]
2003, , 115, 763
Chabrier , G. 2003, , 115, 763
2003
-
[25]
2024, , 527, 7915
Chen , X.-B., Liu , R.-Y., Wang , X.-Y., & Chang , X.-C. 2024, , 527, 7915
2024
-
[26]
S., Agudo , I., et al
Cherenkov Telescope Array Consortium , Acharya , B. S., Agudo , I., et al. 2019, Science with the Cherenkov Telescope Array
2019
-
[27]
Condon , J. J. 1992, , 30, 575
1992
-
[28]
2012, , 544, A101
Cortese , L., Boissier , S., Boselli , A., et al. 2012, , 544, A101
2012
-
[29]
2008, , 388, 1595
da Cunha , E., Charlot , S., & Elbaz , D. 2008, , 388, 1595
2008
-
[30]
2021, , 104, 123016
Do , A., Duong , M., McDaniel , A., et al. 2021, , 104, 123016
2021
-
[31]
& Torres , D
Domingo-Santamar \' a , E. & Torres , D. F. 2005, , 444, 403
2005
-
[32]
R., Rosario , D
Dom \' nguez , A., Primack , J. R., Rosario , D. J., et al. 2011, , 410, 2556
2011
-
[33]
2023, , 678, A157
Donath , A., Terrier , R., Remy , Q., et al. 2023, , 678, A157
2023
-
[34]
Dorfi , E. A. & Breitschwerdt , D. 2012, , 540, A77
2012
-
[35]
G., Corre , D., Leroy , N., & Le Floch , E
Ducoin , J. G., Corre , D., Leroy , N., & Le Floch , E. 2020, , 492, 4768
2020
-
[36]
D., et al
Eckner , C., Hou , X., Serpico , P. D., et al. 2018, , 862, 79
2018
-
[37]
L., Andernach , H., et al
Foschini , L., Lister , M. L., Andernach , H., et al. 2022, Universe, 8, 587
2022
-
[38]
2011, , 534, A31
Gavazzi , G., Savorgnan , G., & Fumagalli , M. 2011, , 534, A31
2011
-
[39]
F., et al
Gil de Paz , A., Boissier , S., Madore , B. F., et al. 2007, , 173, 185
2007
-
[40]
Collaboration , Abdalla , H., Aharonian , F., et al
H.E.S.S. Collaboration , Abdalla , H., Aharonian , F., et al. 2018, , 617, A73
2018
- [41]
-
[42]
2022, Science, 378, 538
IceCube Collaboration , Abbasi , R., Ackermann , M., et al. 2022, Science, 378, 538
2022
-
[43]
D., Kaisina , E
Karachentsev , I. D., Kaisina , E. I., & Makarov , D. I. 2018, , 479, 4136
2018
-
[44]
D., Stroh , M
Kaur , A., Falcone , A. D., Stroh , M. D., Kennea , J. A., & Ferrara , E. C. 2019, , 887, 18
2019
-
[45]
1998, , 498, 541
Kennicutt , Robert C., J. 1998, , 498, 541
1998
-
[46]
C., Funes , J
Kennicutt , Robert C., J., Lee , J. C., Funes , J. G., et al. 2008, , 178, 247
2008
-
[47]
Kennicutt , R. C. & Evans , N. J. 2012, , 50, 531
2012
-
[48]
J., del Palacio , S., et al
Kornecki , P., Pellizza , L. J., del Palacio , S., et al. 2020, , 641, A147
2020
-
[49]
Kornecki , P., Peretti , E., del Palacio , S., Benaglia , P., & Pellizza , L. J. 2022, , 657, A49
2022
-
[50]
2023, PoS, Gamma2022, 216
Kornecki, P., Peretti, E., del Palacio, S., Marcowith, A., & Araudo, A. 2023, PoS, Gamma2022, 216
2023
-
[51]
R., Crocker , R
Krumholz , M. R., Crocker , R. M., Xu , S., et al. 2020, , 493, 2817
2020
-
[52]
Lacki , B. C. & Thompson , T. A. 2013, , 762, 29
2013
-
[53]
C., Thompson , T
Lacki , B. C., Thompson , T. A., Quataert , E., Loeb , A., & Waxman , E. 2011, , 734, 107
2011
-
[54]
2019, Astroparticle Physics, 112, 16
Lamastra , A., Tavecchio , F., Romano , P., Landoni , M., & Vercellone , S. 2019, Astroparticle Physics, 112, 16
2019
-
[55]
P., Ricci , C., T \"u rler , M., Dorner , D., & Walter , R
Lenain , J. P., Ricci , C., T \"u rler , M., Dorner , D., & Walter , R. 2010, , 524, A72
2010
-
[56]
& Tingay , S
Lenc , E. & Tingay , S. J. 2009, , 137, 537
2009
-
[57]
2021, arXiv e-prints, arXiv:2101.03508
LHAASO collaboration . 2021, arXiv e-prints, arXiv:2101.03508
2021 arXiv
-
[58]
2012, Astroparticle Physics, 35, 797
Mannheim , K., Els \"a sser , D., & Tibolla , O. 2012, Astroparticle Physics, 35, 797
2012
-
[59]
2014, , 564, A61
Martin , P. 2014, , 564, A61
2014
-
[60]
2019, , 100, 023014
McDaniel , A., Jeltema , T., & Profumo , S. 2019, , 100, 023014
2019
-
[61]
G., de Freitas Pacheco , J
Nasonova , O. G., de Freitas Pacheco , J. A., & Karachentsev , I. D. 2011, , 532, A104
2011
-
[62]
Observatory, C. T. A. & Consortium, C. T. A. 2021, CTAO Instrument Response Functions - prod5 version v0.1
2021
-
[63]
& Hinton , J
Ohm , S. & Hinton , J. A. 2013, , 429, L70
2013
-
[64]
2019, , 487, 168
Peretti , E., Blasi , P., Aharonian , F., & Morlino , G. 2019, , 487, 168
2019
-
[65]
2020, , 493, 5880
Peretti , E., Blasi , P., Aharonian , F., Morlino , G., & Cristofari , P. 2020, , 493, 5880
2020
-
[66]
G., et al
Peretti , E., Lamastra , A., Saturni , F. G., et al. 2023, , 526, 181
2023
-
[67]
2022, , 511, 1336
Peretti , E., Morlino , G., Blasi , P., & Cristofari , P. 2022, , 511, 1336
2022
-
[68]
P., Spoon , H
P \'e rez-Beaupuits , J. P., Spoon , H. W. W., Spaans , M., & Smith , J. D. 2011, , 533, A56
2011
-
[69]
2008, , 486, 143
Persic , M., Rephaeli , Y., & Arieli , Y. 2008, , 486, 143
2008
-
[70]
2024, , 685, A47
Persic , M., Rephaeli , Y., & Rando , R. 2024, , 685, A47
2024
-
[71]
M., & Springel , V
Pfrommer , C., Pakmor , R., Simpson , C. M., & Springel , V. 2017, , 847, L13
2017
-
[72]
2020, , 641, A6
Planck Collaboration , Aghanim , N., Akrami , Y., et al. 2020, , 641, A6
2020
-
[73]
A., Meisenheimer , K., Marco , O., et al
Prieto , M. A., Meisenheimer , K., Marco , O., et al. 2004, , 614, 135
2004
-
[74]
J., Soifer , B
Rice , W., Lonsdale , C. J., Soifer , B. T., et al. 1988, , 68, 91
1988
-
[75]
& Araya , M
Rojas-Bravo , C. & Araya , M. 2016, , 463, 1068
2016
-
[76]
E., M \"u ller , A
Romero , G. E., M \"u ller , A. L., & Roth , M. 2018, , 616, A57
2018
-
[77]
A., Krumholz , M
Roth , M. A., Krumholz , M. R., Crocker , R. M., & Celli , S. 2021, , 597, 341
2021
-
[78]
A., Krumholz , M
Roth , M. A., Krumholz , M. R., Crocker , R. M., & Thompson , T. A. 2023, , 523, 2608
2023
-
[79]
B., Mazzarella , J
Sanders , D. B., Mazzarella , J. M., Kim , D. C., Surace , J. A., & Soifer , B. T. 2003, , 126, 1607
2003
-
[80]
2021, , 506, 6212
Shimono , N., Totani , T., & Sudoh , T. 2021, , 506, 6212
2021
-
[81]
Strickland , D. K. & Heckman , T. M. 2009, , 697, 2030
2009
-
[82]
W., Orlando , E., & Jaffe , T
Strong , A. W., Orlando , E., & Jaffe , T. R. 2011, , 534, A54
2011
-
[83]
2018, , 70, 49
Sudoh , T., Totani , T., & Kawanaka , N. 2018, , 70, 49
2018
-
[84]
N., et al
Tombesi , F., Cappi , M., Reeves , J. N., et al. 2010, , 521, A57
2010
-
[85]
B., Kourkchi , E., Courtois , H
Tully , R. B., Kourkchi , E., Courtois , H. M., et al. 2023, , 944, 94
2023
-
[86]
Vecchiotti , V., Pagliaroli , G., & Villante , F. L. 2022, Communications Physics, 5, 161
2022
-
[87]
2005, , 43, 769
Veilleux , S., Cecil , G., & Bland-Hawthorn , J. 2005, , 43, 769
2005
-
[88]
A., Aliu , E., et al
VERITAS Collaboration , Acciari , V. A., Aliu , E., et al. 2009, , 462, 770
2009
-
[89]
J., Aharonian , F
V \"o lk , H. J., Aharonian , F. A., & Breitschwerdt , D. 1996, , 75, 279
1996
-
[90]
& Fields , B
Wang , X. & Fields , B. D. 2018, , 474, 4073
2018
-
[91]
2021, , 505, 3295
Werhahn , M., Pfrommer , C., Girichidis , P., & Winner , G. 2021, , 505, 3295
2021
-
[92]
& Nied \'z wiecki , A
Wojaczy \'n ski , R. & Nied \'z wiecki , A. 2017, , 849, 97
2017
-
[93]
2017, in International Cosmic Ray Conference, Vol
Wood , M., Caputo , R., Charles , E., et al. 2017, in International Cosmic Ray Conference, Vol. 301, 35th International Cosmic Ray Conference (ICRC2017), 824
2017
-
[94]
L., Eisenhardt , P
Wright , E. L., Eisenhardt , P. R. M., Mainzer , A. K., et al. 2010, , 140, 1868
2010
-
[95]
2020 a , , 896, L33
Xi , S.-Q., Liu , R.-Y., Wang , X.-Y., et al. 2020 a , , 896, L33
2020
-
[96]
2020 b , , 901, 158
Xi , S.-Q., Zhang , H.-M., Liu , R.-Y., & Wang , X.-Y. 2020 b , , 901, 158
2020
-
[97]
2021, Research in Astronomy and Astrophysics, 21, 263
Xiang , Y.-C., Jiang , Z.-J., & Tang , Y.-Y. 2021, Research in Astronomy and Astrophysics, 21, 263
2021
-
[98]
& Wang , Z
Xing , Y. & Wang , Z. 2023, , 952, 112
2023
-
[99]
2023, , 945, L22
Xing , Y., Wang , Z., Zheng , D., & Li , J. 2023, , 945, L22
2023
-
[100]
& Razzaque , S
Yang , L. & Razzaque , S. 2019, , 99, 083007
2019
-
[101]
M., Everett , J
Yoast-Hull , T. M., Everett , J. E., Gallagher , J. S., I., & Zweibel , E. G. 2013, , 768, 53
2013
-
[102]
S., Reddy , N
Yun , M. S., Reddy , N. A., & Condon , J. J. 2001, , 554, 803
2001
-
[103]
, " * write output.state after.block = add.period write newline
ENTRY address archiveprefix author booktitle chapter edition editor howpublished institution eprint journal key month note number organization pages publisher school series title type volume year label extra.label sort.label short.list INTEGERS output.state before.all mid.sent...
-
[104]
write newline
" write newline "" before.all 'output.state := FUNCTION n.dashify 't := "" t empty not t #1 #1 substring "-" = t #1 #2 substring "--" = not "--" * t #2 global.max substring 't := t #1 #1 substring "-" = "-" * t #2 global.max substring 't := while if t #1 #1 substring * t #2 gl...
Reviewed August 16, 2026 · model on record in the stance chip above.
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