GRB 261011A
GCN Circular 45965
Yash Sharma, Amit K. Ror, Shashi B. Pandey (ARIES) report:
We observed the field of GRB 261011A detected by Swift (Cenko et al., GCN 45896) and SVOM (Huang et al., GCN 45895) with the 1.3m Devasthal Fast Optical Telescope (DFOT), located at the Devasthal Observatory of the Aryabhatta Research Institute of Observational Sciences (ARIES), Nainital, India. The observations were started on 2026-10-14 at 18:09:17 UT, i.e., ~ 3.18 days after the Swift/BAT trigger (T0 = 2026-10-11 13:46:41 UT). We obtained multiple frames with an exposure time of 300 s each in the R filter. The images were aligned and stacked.
We do not detect any optical afterglow emission down to the 3-sigma background limit at the optical afterglow position reported by Swift/UVOT (Cenko et al., GCN 45896) and refined by SOAR (Cheng et al., GCN 45922), nor within the 2.9 arcsec error radius of the enhanced Swift-XRT position (Page et al., GCN 45933; Melandri et al., GCN 45934).
We obtain the following 3-sigma upper limit from the stacked image:
Date Start_UT T_start-T0 (days) Filter Exp time (s) Magnitude (3-sigma)
===================================================================================
2026-10-14 18:09:17 ~ 3.18 R 12 x 300 s > 22.0
The non-detection of the optical counterpart is consistent with the rapid fading of the afterglow at z = 2.407 (Pérez-García et al., GCN 45931; Monsalves et al., GCN 45920) and later-epoch optical/NIR upper limits reported by REM (Brivio et al., GCN 45926), SYSU (Wen et al., GCN 45942), and SAO RAS (Moskvitin et al., GCN 45951).
Photometric calibration was performed against secondary standard stars from the Pan-STARRS (PS1) catalog with Zero Point = 4.081 ± 0.015 mag. The reported limiting magnitude is in the AB system and has not been corrected for the Galactic extinction. This circular may be cited.
GCN Circular 45951
A. Moskvitin (SAO), A. Volnova (IKI), V. Goranskij (SAI MSU, SAO),
V. Vlasyuk (SAO), R. Inasaridze (AbAO), N. Pankov (IKI), A. Pozanenko
(IKI),
on behalf of the SAO GRB follow-up team and the IKI-GRB-FuN report.
We observed the field of GRB 261011A (Huang et al., GCN 45895;
Cenko et al., GCN 45896; Ridnaia et al., GCN 45924; Barthelmy et al.,
GCN 45930; Page et al., GCN 45933; Melandri et al., GCN 45934;
Luo et al., GCN 45939) at redshift z = 2.407 (Pérez-García et al.,
GCN 45931; Monsalves et al., GCN 45920) with the SAO RAS 1-m Zeiss-1000,
0.5-m AS-500(2) and AbAO 0.7-m AS-32 telescopes on October 11.
The OT (Cenko et al., GCN 45896; O'Neill et al., GCN 45897; Fu et al.,
GCN 45898; Izzo, GCNs 45899; 45909; Wu et al., GCN 45900; Shi et al.,
GCN 45903; Aryan et al., GCN 45904; Saikia et al., GCN 45907;
Bochenek and Perley, GCN 45914; Li et al., GCN 45915; Zhao et al.,
GCN 45916; Takahashi et al., GCN 45917; Cheng et al., GCN 45922;
also observed in NIR by Huang et al., GCN 45913) is marginally
detected only in the Zeiss-1000 stacked frame.
Details of the observation are the following.
Date UT start t-T0 Exp, Filter Obj Err UL
Site/Telescope
(mid,days) (n*s) (3sigma)
2026-10-11 20:22:07 0.29806 117*30 R n/d 21.6
SAO/AS-500(2)
2026-10-11 20:56:50 0.30510 3*300 Rc 21.9 0.3 22.0
SAO/Zeiss-1000
2026-10-11 21:01:57 0.32050 49*60 R n/d 20.9
AbAO/AS-32
This preliminary photometry (Vega) is based on nearby SDSS stars
(Lupton 2005 transformation) and not corrected for Galactic extinction.
GCN Circular 45942
Lu-Yao Wen, Jian-Hong Cao, Zhong-Nan Dong, Jin-Ji Li, Jia-Qi Lin, Pu Lin, Yun Shi, Hao-Nan Yang, Rui-Chen Gao, Jing-Kai Sun, Hao-Ran Zhang, P H Thomas Tam, Rong-Feng Shen, Bin Ma (Sun Yat-sen University) report on behalf of the SYSU 80cm infrared telescope team:
We carried out further J-band observations of GRB 261011A using the Sun Yat-sen University (SYSU) 80 cm infrared telescope. We observed from 2026 October 12 17:37:44.942 to 19:41:05.309 UT, 27.85–29.91 hours after the Swift/BAT trigger. Our earlier J-band detections were reported in Huang et al. (GCN 45913).
We do not detect the source at the position of the counterpart (Cenko et al., GCN 45896; O'Neill et al., GCN 45897; Fu et al., GCN 45898; Izzo et al., GCN 45899; Wu et al., GCN 45900; Yin et al., GCN 45901; Shi et al., GCN 45903; Aryan et al., GCN 45904; Arya et al., GCN 45907; Izzo et al., GCN 45909; Huang et al., GCN 45913; Bochenek et al., GCN 45914; Li et al., GCN 45915; Zhao et al., GCN 45916; Takahashi et al., GCN 45917; Monsalves et al., GCN 45920; Cheng et al., GCN 45922), down to a 5-sigma limiting magnitude of J > 19.6 mag (Vega).
The limiting magnitude was calibrated against nearby stars from the 2MASS catalog and is reported in the Vega system, without correction for Galactic extinction. The SYSU 80 cm infrared telescope is operated and managed by the Department of Astronomy, Sun Yat-sen University.
GCN Circular 45939
Jin-Ye Luo, Chen-Wei Wang, Yue Wang, Shao-Lin Xiong (IHEP) report on behalf of GECAM team:
GECAM-B was triggered on-ground by GRB 261011A at 2026-10-11T13:49:15.250 UTC (denoted as T0), which is also detected by SVOM/ECLAIRs (Huang et al., GCN #45895), Swift/BAT (Cenko et al., GCN #45896; Barthelmy et al., GCN #45930), and Konus-Wind (Ridnaia et al., GCN #45924).
According to the GECAM-B light curves in about 70-6000 keV, this burst mainly consists of muplti-pulses with a duration (T90) of 40 +21/-9 s.
The GECAM-B light curve can be found here:
https://www.bursthub.cn/gcn/2026/gecambgrb261011A.png
Gravitational wave high-energy Electromagnetic Counterpart All-sky Monitor (GECAM) mission originally consists of two micro-satellites (GECAM-A and GECAM-B) launched in Dec. 2020. As the third member of GECAM constellation, GECAM-C was launched onboard SATech-01 experimental satellite in July 2022. GECAM mission is funded by the Chinese Academy of Sciences (CAS).
GCN Circular 45934
A. Melandri (INAF-OAR), T. Sbarrato (INAF-OAB), P. D'Avanzo (INAF-OAB),
D.N. Burrows (PSU), J.J. DeLaunay (PSU), S. Lanava (PSU), A.P.
Beardmore (U. Leicester), J.P. Osborne (U. Leicester) and P.A. Evans
report on behalf of the Swift-XRT team:
We have analysed 4.2 ks of XRT data for GRB 261011A, from 301 s to 28.0
ks after the trigger. The data comprise 1.2 ks in Windowed Timing
(WT) mode (the first 10 s were taken while Swift was slewing) with the
remainder in Photon Counting (PC) mode. Using 1938 s of PC mode data
and 4 UVOT images, we find an enhanced XRT position (using the XRT-UVOT
alignment and matching UVOT field sources to the USNO-B1 catalogue):
RA, Dec = 21.89722, -21.56052 which is equivalent to:
RA (J2000): 01h 27m 35.33s
Dec(J2000): -21d 33' 37.9"
with an uncertainty of 2.9 arcsec (radius, 90% confidence).
The light curve can be modelled with a series of power-law decays. The
initial decay index is alpha=4.1 (+/-0.6). At T+362 s the decay
flattens to an alpha of 1.68 (+0.11, -0.10) before breaking again at
T+792 s to a final decay with index alpha=1.26 (+0.06, -0.05).
A spectrum formed from the WT mode data can be fitted with an absorbed
power-law with a photon spectral index of 1.80 (+/-0.05). The
best-fitting absorption column is 7.7 (+1.7, -1.6) x 10^20 cm^-2, in
excess of the Galactic value of 0.0 x 10^00 cm^-2 (Willingale et al.
2013). The counts to observed (unabsorbed) 0.3-10 keV flux conversion
factor deduced from this spectrum is 3.6 x 10^-11 (4.1 x 10^-11) erg
cm^-2 count^-1.
A summary of the WT-mode spectrum is thus:
Total column: 7.7 (+1.7, -1.6) x 10^20 cm^-2
Galactic foreground: 1.5 x 10^20 cm^-2
Excess significance: 6.4 sigma
Photon index: 1.80 (+/-0.05)
The results of the XRT-team automatic analysis are available at
https://www.swift.ac.uk/xrt_products/01516664.
This circular is an official product of the Swift-XRT team.
GCN Circular 45933
K.L. Page, P.A. Evans and M.R. Goad (U. Leicester) report
on behalf of the Swift-XRT team:
Using 1938 s of XRT Photon Counting mode data and 4 UVOT images, we find
an astrometrically corrected X-ray position (using the XRT-UVOT alignment
and matching UVOT field sources to the USNO-B1 catalogue): RA, Dec =
21.89722, -21.56052 which is equivalent to:
RA (J2000): 01 27 35.33
Dec (J2000): -21 33 37.9
with an uncertainty of 2.9 arcsec (radius, 90% confidence).
This position may be improved as more data are received. The latest
position can be viewed at https://www.swift.ac.uk/xrt_positions. Position
enhancement is described by Goad et al. (2007, A&A, 476, 1401) and Evans
et al. (2009, MNRAS, 397, 1177).
This circular is an official product of the Swift-XRT team.
GCN Circular 45931
I. Pérez-García (IAA-CSIC), Y.-D. Hu (GXU), A. J. Castro-Tirado (IAA-CSIC), F. J. Aceituno, M.D. Caballero-Garcia, E. Fernandez-Garcia, M. Gritsevich, S. Guziy (IAA-CSIC), D. Garcia-Alvarez, A. Tejero (GRANTECAN, IAC), on behalf of a larger collaboration, report:
We observed the optical afterglow of GRB 261011A detected by SVOM/ECLAIRs (Huang et al. GCN 45895), Swift/BAT (Cenko et al. GCN 45896) and Konus-Wind (Ridnaia et al. GCN 45924), with the 10.4m Gran Telescopio Canarias (equipped with the OSIRIS+ spectrograph) in La Palma (Spain). Long-slit spectra were taken starting on Oct 12, 2026, 00:19 UT (i.e. 10.5 h post burst) with both the R1000R grism (1200 s) and the R1000B grism (600 s), with the slit centred on the optical afterglow position (Cenko et al., GCN 45896; O'Neill et al., GCN 45897; Fu et al., GCN 45898; Izzo et al., GCN 45899; Wu et al., GCN 45900; Yin et al., GCN 45901; Shi et al., GCN 45903; Aryan et al., GCN 45904; Arya et al., GCN 45907; Izzo et al., GCN 45909; Huang et al., GCN 45913; Bochenek et al., GCN 45914; Li et al., GCN 45915; Zhao et al., GCN 45916; Takahashi et al., GCN 45917; Cheng et al., GCN 45922).
A faint continuum of the afterglow is detected across the full range. On top of it, we identify low S/N ratio absorption features consistent with Fe II (2344, 2374, 2382 A), Al II (1670 A) and Al III (1854/1862 A), all at a common redshift z = 2.407 +/- 0.001.
A joint analysis of all the expected lines gives the above mentioned, unique solution, at this redshift over the range 1.5 < z < 4.2. Moreover, we notice that the flux drops strongly below ~4270 A, consistent with the damped Lyman-alpha absorption trough at this redshift.
This confirms the tentative redshift z = 2.405 derived by Monsalves et al. (GCN 45920) from the damped Lyman-alpha trough in the VLT/X-shooter spectrum.
In addition to this, we notice that the Legacy Survey DR10 shows a faint source (r = 25.4 AB), coincident with the afterglow position within 0.1 arcsec, a likely host galaxy candidate.
We thank the staff at GTC for their excellent support.
GCN Circular 45930
S. D. Barthelmy (GSFC), R. Gupta (GSFC), H. A. Krimm (NSF), S. Laha
(GSFC/UMBC), A. Y. Lien (U Tampa), C. B. Markwardt (GSFC), M. J. Moss
(GSFC), D. M. Palmer (LANL), T. Parsotan (GSFC), D. Sadaula (GSFC/UMBC), T.
Sakamoto (AGU) (i.e. the Swift-BAT team):
Using the data set from T-179 to T+723 sec from the recent telemetry
downlink, we report further analysis of BAT GRB 261011A (trigger #1516664)
(Cenko et al., GCN Circ. 45896). The BAT ground-calculated position is
RA, Dec = 21.911, -21.550 deg which is
RA(J2000) = 01h 27m 38.7s
Dec(J2000) = -21d 33' 00.7"
with an uncertainty of 1.0 arcmin, (radius, sys+stat, 90% containment). The
partial coding was 29%.
The mask-weighted light curve shows a multi-peaked structure that starts
~T+100 s and ends at ~T+210 s. T90 (15-350 keV) is 78.90 +- 18.49 sec
(estimated error including systematics). Note that the particularly unusual
light curve mentioned in the original circular (Cenko et al., GCN Circ.
45896) is no longer visible in the ground analysis. Further investigation
shows that there were some noisy detectors producing coincidental
pulse-like structures around the GRB time, and thus those pulses seen in
the raw light curve prior to ~T+100 s are not astrophysical.
The time-averaged spectrum from T+103.61 to T+208.74 sec is best fit by a
simple power-law model. The power law index of the time-averaged spectrum
is 1.50 +- 0.07. The fluence in the 15-150 keV band is 6.3 +- 0.3 x 10^-06
erg/cm2. The 1-sec peak photon flux measured from T+171.74 sec in the
15-150 keV band is 3.0 +- 0.4 ph/cm2/sec. All the quoted errors are at the
90% confidence level.
The results of the batgrbproduct analysis are available at
https://swift.gsfc.nasa.gov/results/batgrbcat/BAT_refined_circular/1516664
GCN Circular 45926
R. Brivio, M. Ferro, P. D'Avanzo, S. Covino, D. Fugazza (INAF-OAB) report on behalf of the REM team:
We observed the field of GRB 261011A, detected by Swift/BAT (Huang et al., GCN 45895; Cenko et al., GCN 45896) and SVOM/ECLAIRs with the REM 60 cm robotic telescope located at the ESO observatory of La Silla (Chile).
The observations were carried out in the g, r, i, z, K bands, started on 2026-10-12 at 01:30:16 UT (i.e. 11.7 hr after the burst) and lasted for about 2.0 hr.
From preliminary photometry, we do not detect the optical/NIR counterpart (Cenko et al., GCN 45896; O'Neill et al., GCN 45897; Fu et al., GCN 45898; Izzo et al., GCN 45899; Wu et al., GCN 45900; Yin et al., GCN 45901; Shi et al., GCN 45903; Aryan et al., GCN 45904; Arya et al., GCN 45907; Izzo et al., GCN 45909; Huang et al., GCN 45913; Bochenek et al., GCN 45914; Li et al., GCN 45915; Zhao et al., GCN 45916; Takahashi et al., GCN 45917; Monsalvel et al., GCN 45920; Cheng et al., GCN 45922) down to the following 3sigma limits:
r > 20.6 (AB; calibrated against the PanSTARRS catalogue),
at a mid-time of 12.1 hr after the trigger;
K > 14.2 (Vega; calibrated against the 2MASS catalogue),
at a mid-time of 11.8 hr after the trigger.
GCN Circular 45924
A. Ridnaia, D. Frederiks, A. Lysenko, V. Panteleeva,
D. Svinkin, A. Tsvetkova, M. Ulanov, and T. Cline,
on behalf of the Konus-Wind team, report:
The long-duration GRB 261011A
(SVOM detection: Huang et al., GCN 45895;
Swift detection: Cenko et al., GCN 45896)
was detected by Konus-Wind (KW) in the waiting mode
at about T0 = T0 (SVOM) = 49747 s UT (13:49:07).
A Bayesian block analysis of the KW waiting mode data
in the 20-400 keV band reveals a ~20 sigma count rate
increase in the interval from T0+1.7 s to T0+66.468 s.
The Konus-Wind light curve of this GRB is available at
http://www.ioffe.ru/LEA/GRBs/GRB261011A/
The total burst fluence is 1.30(-0.21,+0.62)x10^-5 erg/cm^2,
and the 2.944 s peak energy flux, measured from T0+10.532 s,
is 4.63(-4.27,+4.74)x10^-7 erg/cm^2/s.
(both in the 20 keV - 10 MeV energy range).
The time-integrated spectrum of the burst,
measured from T0+1.7 s to T0+66.468 s,
can be described by a power law with exponential cutoff (CPL) model
dN/dE ~ (E^alpha)*exp(-E*(2+alpha)/Ep)
with alpha = -1.8(-0.1,+0.2) and Ep = 198(-67,+869) keV.
All the quoted errors are estimated at the 68% confidence level.
All the presented results are preliminary.
GCN Circular 45922
Cheng Cheng (CASSACA, NAOC), Liping Xin (NAOC), Jia-Sheng Huang (CASSACA, NAOC) report:
We observed the field of GRB 261011A (SVOM/ECLAIRs: Huang et al., GCN 45895; Swift/BAT: Cenko et al., GCN 45896) with the 4.1-m SOAR telescope (GHTS red imager) beginning on 2026-10-12 at 06:45:36 UT, i.e. 17.06 h after the Swift/BAT trigger.
We obtained 3 x 180 s exposures in each of the SDSS g, r and z filters. The frames were trimmed, astrometrically solved, sky-subtracted and median-combined onto a common output grid (0.2894"/pixel), so that the three band images are pixel-aligned. Each stacked image is 1000 x 1000 pixels (4.8' x 4.8'), centred on the target coordinates.
We detect the afterglow at
RA, Dec (J2000) = 01:27:35.40, -21:33:37.7
with an uncertainty of 0.15" (the astrometry is tied to Gaia DR3; a cross-check against LS DR11/DECaLS gives a residual scatter of 0.10"). This position lies 0.52" from the Swift/UVOT position reported by Cenko et al. (GCN 45896), fully consistent with its 1.1" error radius, and refines it.
Photometry was carried out with SExtractor in dual mode, using the r-band image as the detection image and measuring MAG_AUTO magnitudes on the g, r and z images with a local background estimate. Magnitudes were calibrated against LS DR11 (DECaLS) stars and are in the AB system:
g = 23.93 +/- 0.14 (phot) +/- 0.08 (zeropoint)
r = 22.75 +/- 0.08 (phot) +/- 0.09 (zeropoint)
z = 22.43 +/- 0.18 (phot) +/- 0.15 (zeropoint)
The first uncertainty is the photometric error and the second is the zeropoint (calibration) uncertainty, which is systematic across the field and therefore should not be treated as an independent error when combining this measurement with others.
The source is unresolved (FWHM = 1.2"), and no host galaxy is detected at this depth; the LS DR11 source at this position (ls_id_dr11 = 48423370429045300) has r = 25.63 +/- 0.30 AB mag.
We thank the SOAR staff for the rapid execution of these observations.
GCN Circular 45920
Nicolas Monsalves, Yu-Han Yang and Eleonora Troja (U Rome) report on behalf of the ERC BHianca team:
We observed the field of GRB 261011A (Huang et al., GCN 45895; Cenko et al., GCN 45896) with the X-Shooter spectrograph on the ESO VLT UT3 (Melipal). Observations began at T+13.4 hours and obtained a total of 4 x 600 s spectra at an average airmass of about 1.1.
At the position of the optical counterpart (Cenko et al., GCN 45896; O'Neill et al., GCN 45897; Fu et al., GCN 45898; Izzo et al., GCN 45899; Wu et al., GCN 45900; Yin et al., GCN 45901; Shi et al., GCN 45903; Aryan et al., GCN 45904; Arya et al., GCN 45907; Izzo et al., GCN 45909; Huang et al., GCN 45913; Bochenek et al., GCN 45914; Li et al., GCN 45915; Zhao et al., GCN 45916; Takahashi et al., GCN 45917) we detect a faint continuum in all three arms.
In the UVB arm we detect continuum emission down to ~4270 Angstrom, which sets a robust upper limit to the redshift z<3.7. The flux remains consistent with zero between ~4000 and ~4270 Angstrom,with a weak signal reappearing blueward of ~4000 Angstrom. Interpreting this broad feature as a damped Lyman-alpha absorption trough, we infer a tentative redshift of z=2.405.
We thank the staff at the VLT, for the rapid execution of these observations.
GCN Circular 45917
I. Takahashi, M. Sasada, H. Hagio, Y. Kubo, A. Ochi, R. Kato, N. Hosoya, J. Yonamine, Y. Yatsu, N. Kawai (Science Tokyo), and M. Niwano (NAOJ) report on behalf of the MITSuME collaboration:
We observed the field of GRB 261011A detected by Swift (Cenko et al., GCN 45896) and SVOM (Huang et al., GCN 45895) with the optical three-color (g', Rc, and Ic) CCD cameras mounted on the MITSuME 50-cm telescope Akeno.
The observations started at 2026-10-11 13:50:44 UT (243 s after the Swift/BAT trigger). We stacked the images obtained under good observing conditions. We detected an optical afterglow candidate at the position reported by Swift-UVOT (Cenko et al., GCN 45896).
The preliminary photometry of the source is as follows:
T0+[sec] | MID-UT | T-EXP[sec] | Magnitudes
----------------------------------------------------------------------------------------------------
580 | 2026-10-11 13:56:21 | 260 | Rc=16.5+/-0.1, Ic=16.2+/-0.1
----------------------------------------------------------------------------------------------------
T0+ : Elapsed time after the Swift/BAT trigger
T-EXP: Total exposure time
We used the PS1 catalog for flux calibration. The catalog magnitudes in PS1 g, r and i bands were converted to our g', Rc and Ic band magnitudes following Tonry et al. (2012), Table 6. The magnitudes are expressed in the AB system. The images were processed in real-time through the MITSuME GPU reduction pipeline (Niwano et al. 2021, PASJ; https://github.com/MNiwano/Eclaire).
GCN Circular 45916
Jiewei Zhao, Brajesh Kumar, Yuanpei Yang, Guowang Du (SWIFAR, YNU), Kai Liao, Xinyu Wang, Xing Yao, Yang Zeng and Chunlai Zhang (SSO) report:
We performed observations of the GRB 261011A field (Huang et al., GCN 45895; Cenko et al., GCN 45896; T0 at 2026-10-11T13:46:41) with 60cm telescope located at the Sichuan South Observatory (SSO), China. These observation were acquired from 2026-10-11T14:28:48.22 (~0.70 hours after the trigger) and continued ~2.40 hours. Multiple frames were acquired in L band with different exposure time.
The optical counterpart reported by Swift-UVOT (Cenko et al., GCN 45896) and also confirmed by other facilities (O'Neill et al., GCN 45897; Fu et al., GCN 45898; Izzo et al., GCN 45899; Wu et al., GCN 45900; Yin et al., GCN 45901; Shi et al., GCN 45903; Aryan et al., GCN 45904; Arya et al., GCN 45907; Izzo et al., GCN 45909; Huang et al., GCN 45913; Bochenek et al., GCN 45914; Li et al., GCN 45915) was clearly detected in our frames and the preliminary photometry is following:
Start time[MJD], AB Magnitude, Filter
61324.60334, 19.67 +/- 0.19, L
61324.62294, 20.10 +/- 0.14, L
61324.65458, 20.66 +/- 0.20, L
The given magnitudes are not corrected for the expected Galactic extinction.
GCN Circular 45915
R.-Z. Li, B.-T. Wang, F.-F. Song, J. Mao, K.-X. Lu, J.-G. Wang and B. Wang (YNAO, CAS) report:
We observed the field of GRB 261011A (Huang et al., GCN 45895; Cenko et al., GCN 45896; T0 at 2026-10-11T13:46:41) using the GMG-2.4m telescope at the Lijiang Observatory. The observation began at 2026-10-11T16:41:50, about 2.92 hours after the trigger.
The optical counterpart reported by Swift-UVOT (Cenko et al., GCN 45896) and by other facilities (O'Neill et al., GCN 45897; Fu et al., GCN 45898; Izzo et al., GCN 45899; Wu et al., GCN 45900; Yin et al., GCN 45901; Shi et al., GCN 45903; Aryan et al., GCN 45904