LIGO/Virgo/KAGRA S251112cm
GCN Circular 42867
Mankeun Jeong, Myungshin Im, Seo-Won Chang, Hyeonho Choi (SNU/SNU ARC), Gregory S.-H. Paek (IfA), and Chung-Uk Lee (KASI), on behalf of the GECKO team
We observed the S251112cm sky localization region (Updated; GCN 42690) following the LIGO/Virgo/KAGRA trigger. Optical imaging was obtained with the three 1.6-m Korea Microlensing Telescope Network (KMTNet) telescopes at CTIO, SAAO, and SSO, with most of the data taken from SSO.
We surveyed the southern portion (decl. < -10 deg) of the S251112cm 90% localization region, covering ~1,012 deg^2 from 2025-11-13 to 2025-11-27. During the first three nights, we obtained R and I imaging with 480 sec total exposure per field (four dithered 120 sec exposures) over ~180 deg^2. For the remainder of the run, observations were conducted in R-band only with the same 480 sec per-field exposure.
A fraction of the surveyed area overlaps with regions having KMTNet Synoptic Survey of the Southern Sky (KS4) reference images. Difference image analysis has been completed for ~60 deg^2, with additional processing ongoing.
Below we list transient candidates re-identified from TNS and new GECKO sources detected in our imaging. Redshifts are adopted from the GLADE+ host-galaxy associations.
| Name | RA (deg) | Dec (deg) | R (AB mag) | I (AB mag) | Date-Obs (UTC) | Redshift |
|---|---|---|---|---|---|---|
| AT2025aebs | 354.16948 | -33.01666 | 20.42 ± 0.05 | 20.66 ± 0.07 | 2025-11-16T12:24:50 | 0.1642 |
| AT2025adbw | 3.31215 | -36.40843 | 19.07 ± 0.02 | — | 2025-11-14T14:23:37 | — |
| AT2025abnc | 7.50565 | -34.96515 | 19.95 ± 0.05 | 20.54 ± 0.08 | 2025-11-14T12:40:10 | 0.1067 |
| GECKO25dryb | 1.69517 | -33.38614 | 18.95 ± 0.01 | 19.05 ± 0.05 | 2025-11-14T13:39:42 | 0.2094 |
| GECKO25drxk | 1.53192 | -35.03043 | 18.89 ± 0.01 | 18.86 ± 0.03 | 2025-11-14T13:39:42 | 0.2408 |
| GECKO25dulp | 358.59508 | -35.91373 | 19.58 ± 0.06 | 18.65 ± 0.03 | 2025-11-16T13:40:59 | 0.0859 |
| GECKO25dukb | 356.10091 | -34.07094 | 18.37 ± 0.01 | 18.13 ± 0.01 | 2025-11-16T12:24:50 | 0.1269 |
All newly identified GECKO candidates lie close to the center of the host galaxy, whose redshifts exceed the estimated distance of S251112cm, indicating they are unrelated to the GW event's physical origin.
Further difference imaging and transient vetting across the remaining fields are underway.
The GECKO network (Im et al. 2023; Paek et al. 2024) operates 0.5–1 m class telescopes worldwide for EM follow-up of gravitational-wave events. KMTNet is operated by the Korea Astronomy and Space Science Institute. We thank the KMTNet staff for their support during these observations.
GCN Circular 42825
J. H. Gillanders (Oxford), A. Aryan, T.-W. Chen, Y.-H. Lee, C.-S. Lin (all NCU), A. K. H. Kong (NTHU), S. J. Smartt (Oxford), Y. J. Yang (NYUAD), A. Sankar.K, Y.-C. Pan, C.-C. Ngeow, M.-H. Lee, C.-H. Lai, W.-J. Hou, H.-C. Lin, H.-Y. Hsiao, J.-K. Guo (all NCU), S. Yang, Z. N. Wang, L. L. Fan, G. H. Sun (all HNAS), H.-W. Lin (UMich), H. F. Stevance, S. Srivastav, L. Rhodes (all Oxford), M. Nicholl, M. Fulton, T. Moore, K. W. Smith, C. Angus, A. Aamer (all QUB), A. Schultz and M. Huber (both IfA, Hawaii) report:
Here we report follow-up observations of the candidate optical counterpart AT 2025adht (first reported by Franz et al., GCN 42675; see also Anand et al., GCN 42677; Burkhonov et al., GCN 42798) to the LIGO-Virgo-KAGRA (LVK) gravitational-wave event S251112cm (LVK Collaboration, GCN 42650).
We observed AT 2025adht utilizing the 1m LOT at Lulin Observatory in Taiwan, as part of the Kinder collaboration (Chen & Yang et al. 2025, ApJ, 983, 86, doi:10.3847/1538-4357/adb428). The first LOT epoch of observations began at 20:31 UTC on November 21, 2025 (MJD 61000.855), 9.225 days after the GW trigger. The second LOT epoch began at 20:16 UTC, or MJD 61001.845, 10.207 days after the GW trigger.
We utilized the astroalign (Beroiz et al. 2020, A&C, 32, 100384) and astropy (Astropy Collaboration et al. 2022, ApJ, 935, 167) packages to align and stack the individual frames. We utilized the Python-based package AutoPhOT (Brennan & Fraser 2022, A&A, 667, A62) to perform template subtraction with the DESI Legacy Survey (Dey et al. 2019, AJ 157, 168) DR10 images using the 'hotpants' (Becker 2015, ascl.soft. ascl:1504.004) algorithm.
Moreover, we further utilized AutoPhOT to perform PSF photometry. The details of the observations and the measured magnitudes (in the AB system) are as follows:
Telescope | Filter | MJD (start) | t - t0 (d) | Exposure (s) | Magnitude | avg. Seeing | med. Airmass
LOT | r | 61000.855 | 9.225 | 300 * 6 | 21.83 +/- 0.06 | 1".2 | 1.41
LOT | r | 61001.845 | 10.207 | 300 * 6 | 21.86 +/- 0.08 | 1".2 | 1.46
Burkhonov et al. (GCN 42698) report a (PS1-equivalent) r-band magnitude of 21.64 +/- 0.1 on MJD 60994.009 (2.37 days post-GW trigger). Our observations indicate that AT 2025adht has faded only slightly in the ~week since detection. The slow evolution indicates that AT 2025adht is not some rapidly declining kilonova-like transient; we instead suspect that AT 2025adht is a background supernova near peak, hence the slow evolution. This interpretation is supported by the Legacy Survey's host galaxy phot-z estimate (0.139 +/- 0.033; see also Anand et al., GCN 42677).
The presented magnitudes are calibrated using field stars from the ATLAS-RefCat2 catalog from MAST (Tonry et al. 2018, ApJ, 867, 105) and are not corrected for the expected Galactic foreground extinction of A_r = 0.06 mag in the direction of the transient (Schlafly & Finkbeiner 2011). The methodology and details on the capabilities of Lulin observatory telescopes can be found in Aryan et al. 2025, ApJS, 281, 20. doi:10.3847/1538-4365/adfc69.
GCN Circular 42796
Hemanth Bommireddy (U de Chile), Regis Cartier (UA), Felipe Olivares (U Hawaii), reporting on behalf of the Dark Energy Survey Gravitational Wave (DESGW) spectroscopy team:
We report spectroscopic observations of the transients AT2025adgp, AT2025adhf, and AT2025adhs obtained with the SOAR telescope on 2025-11-14 at 04:10:05 UTC (PI: Bommireddy). For each source, we obtained an exposure of approximately 900s. The spectra were preliminarily reduced and classified using the NGSF spectral classification software (Goldwasser et al. 2022). Based on the reported redshifts (GCN 42675), the top 3 template fits for each event are listed below.
| event | SN type/event/instrument (χ²/dof) |
|---|---|
| AT2025adgp | II/2013fs/KAST (~0.83), Ic-BL/1998bw/DFOSC (~0.82), IIn/2010jl/KAST (~0.88) |
| AT2025adhf | Ic-BL/1998bw/DFOSC (~1.96), Ic-BL/1998bw/EFOSC2-3.6 (~1.99), Ic-BL/1998bw/DFOSC (~2.06) |
| AT2025adhs | SLSN-I/PTF10aagc/LRIS (~1.57), Ia-pec/2000cx/KAST (~1.61), SLSN-I/PTF12dam/DBSP (~1.62) |
We thank the SOAR staff for their support during these observations.
GCN Circular 42777
Y. N. Ma, L. P. Xin, Z. H. Yao, Y. L. Qiu, C. Wu, H. L. Li, X. H. Han, Y. Xu, J. Wang, P. P. Zhang, W. J. Xie, Y. J. Xiao, H. B. Cai, L. Lan, J. S. Deng, J. Y. Wei (NAOC), J. Palmerio (CEA) report on behalf of the SVOM/VT team.
SVOM/VT performed the Target of Opportunity observations of 3 candidates of S251112cm reported by LIGO/Virgo/KAGRA (GCN 42650, GCN 42690). SVOM/VT began observing the field at 2025-11-17, in the VT_B (400nm-650nm) and VT_R (650nm-1000nm) channels simultaneously.
We observed AT2025adhf (GCN 42675, GCN 42724), AT2025adkl (GCN 42691), and AT2025addc (GCN 42658), which were reported by the Vera C. Rubin Observatory (GCN 42707). We found that AT2025adhf is located within a galaxy, while AT2025adkl is situated at a galaxy's edge. Here we provide the total magnitudes of the supernovae and the galaxies (using the galactic nuclei as the photometric center), since we do not have the templates for this sources. AT2025addc is an isolated source, and we also provide its magnitude. The magnitudes are:
Name |Observation Date(UTC) |VT_B(AB_mag) |VT_R(AB_mag)
----------------------|----------------------|-------------|-------------
AT2025adhf(+galaxy) |2025-11-17 |17.19+-0.01 |16.41+-0.01
AT2025adkl(+galaxy) |2025-11-18 |20.14+-0.05 |19.50+-0.04
AT2025addc |2025-11-17 |20.45+-0.04 |20.75+-0.07
Our photometry was not corrected for Galactic extinction.
Further analysis of these candidates is ongoing.
The Space Variable Objects Monitor (SVOM) is a China-France joint mission led by the Chinese National Space Administration (CNSA, China), National Center for Space Studies (CNES, France) and the Chinese Academy of Sciences (CAS, China), which is dedicated to observing gamma-ray bursts and other transient phenomena in the energetic universe. VT was jointly developed by Xi'an Institute of Optics and Precision Mechanics (XIOPM), CAS and National astronomical observatories (NAOC), CAS.
GCN Circular 42746
M. Kerr, C.C. Cheung, R. Woolf, J.E. Grove (NRL), A. Goldstein (USRA), C.A. Wilson-Hodge, D. Kocevski (MSFC), and M.S. Briggs (UAH) report:
The compact binary merger candidate S251112cm (event time, T0 = 2025-11-12T15:19:22.360 UTC) was identified in LIGO Hanford Observatory (H1), LIGO Livingston Observatory (L1), and Virgo Observatory (V1) data (GCN 42690).
The Glowbug gamma-ray instrument [1,2,3] observed much of the sky to which a high probability for the candidate origin was assigned. Glowbug has an all-sky field-of-view limited only by earth occultation and large-scale structures on the International Space Station (ISS). At T0, the Glowbug boresight was pointed towards R.A., Dec. = 92, 22 deg. We examined three high-probability regions in the contours with positions R.A., Dec. = 346, -13 deg; 173, 43 deg; and 149, 6.5 deg, which were at zenith angles of 110 deg., 68 deg., and 57 deg., respectively, all nominally above the limb of the earth. Positions at lower zenith angles, however, are more likely to be obstructed by ISS structure.
Using 50-2000 keV data and two representative (normal and hard spectrum) GRB templates from [4], we searched for transient gamma-ray signals using maximum likelihood methods and found no plausible counterpart up to 30s before or after T0. We determined 3-sigma upper limits on the flux for a GRB at the three trial positions by selecting data centered on T0 and integrating the posterior probability to determine the flux beyond which the tail probability is 0.27%. For various timescales and the two GRB spectral templates, the range of limits (over the three positions) in units of 1e-7 erg/cm2/s are:
Timescale Normal Hard
------------------------------------
0.128 s: 1.4-2.8 3.0-6.0
1.024 s: 0.8-1.0 1.5-2.0
8.192 s: 0.2-0.4 0.4-1.0
These results do not account for scattering or occultation by structures on the ISS. We do not report results for an assumed soft spectrum due to a likely increase in the low-energy threshold of Glowbug due to accumulated radiation exposure.
The Glowbug sky coverage is complementary to that obtained by Fermi/GBM (GCN 42655).
Glowbug is a NASA-funded technology demonstrator for sensitive, low-cost gamma-ray transient telescopes developed, built, and operated by the U.S. Naval Research Laboratory (NRL) with support from the University of Alabama in Huntsville, USRA, and NASA MSFC. It was launched on 2023 March 15 aboard the Department of Defense Space Test Program’s STP-H9 to the ISS and operated until 2024 April when it was put in safe storage on orbit. Glowbug was removed from storage and resumed operation on 2025 September 12.
[1] Grove, J.E. et al. 2020, Proc. Yamada Conf. LXXI, arXiv:2009.11959
[2] Woolf, R.S. et al. 2022, Proc. SPIE, 12181, id. 121811O
[3] Woolf, R.S. et al. 2024, Proc. SPIE, 13151, id. 1315108
[4] Goldstein, A. et al. 2020, ApJ 895, 40, arXiv:1909.03006
Distribution Statement A: Approved for public release. Distribution is unlimited.
GCN Circular 42725
Kenta Taguchi, Miho Kawabata (Kyoto U.); Ryosuke Itoh (Ibara City); Hiroshi Akitaya, Tomoki Morokuma (ARC/Chiba Tech); Jun Takahashi, Satoshi Honda, Miyako Tozuka, Shigeru Takahashi (Univ. of Hyogo/NHAO); Koji Kawabata, Tatsuya Nakaoka (Hiroshima U.); Haruna Hagio, Ryotaro Kato, Atsuya Ochi, Mahito Sasada, Ichiro Takahashi (Science Tokyo); Nozomu Tominaga, Yousuke Utsumi, Michitoshi Yoshida, Haibin Zhang, Masafumi Niwano, Mitsuru Kokubo, Yuhei Iwata (NAOJ); Masaomi Tanaka (Tohoku University); Yuu Niino, Taiga Sasaoka (U. of Tokyo); Yumiko Oasa, Takahiro Kanai (Saitama Univ.); Yuichiro Sekiguchi (Toho University) on behalf of the J-GEM collaboration
We report imaging follow-up observations for the gravitational-wave event S251112cm (GCN 42650).
Our observations started at 2025-11-12 19:09:29 UT (MJD=60991.80), approximately 3.8 hours after the event, and ended at 2025-11-17 10:18:47 UT (MJD=60996.43).
We conducted galaxy-targeted observations of 135 galaxies (see the table below), selected from the GLADE catalog (v2.4; Dalya et al. 2018) within the probability skymap of S251112cm, using the telescopes and instruments listed below.
After screening out known minor planets, we did not find any apparent transient candidates in these galaxies down to the 5-sigma limiting magnitudes in the AB magnitude system summarized below.
galid ra dec dist g r R i I z J H Ks NoFilt obsid
--------------- -------- -------- ------ ---- ---- ---- ---- ---- ---- ---- ---- ---- ------ -------
GL000835-335128 2.1441 -33.8578 97.4 -- -- 17.2 -- -- -- -- -- -- -- 1
GL094621+030417 146.5879 3.0713 86.9 19.6 18.6 -- 18.8 -- -- -- -- -- 18.3 2,3
GL095807+102135 149.5288 10.3598 77.8 20.4 19.9 19.8 19.8 18.0 -- -- 15.8 -- -- 4,5,2
GL102235+195314 155.6440 19.8871 82.7 19.9 19.6 18.7 19.6 18.0 -- -- -- -- 19.0 5,2,3
GL094620+030244 146.5848 3.0455 87.3 19.6 18.6 -- 18.8 -- -- -- -- -- 18.3 2,3
GL094604+042412 146.5148 4.4033 71.9 18.0 17.1 -- 17.2 -- -- -- -- -- 18.5 2,3
GL093427-023015 143.6119 -2.5041 78.1 19.6 18.6 20.1 18.9 -- -- -- 16.8 -- 14.9 2,3,4
GL100140+104523 150.4186 10.7564 78.3 19.9 19.5 18.6 19.5 17.9 -- -- -- -- 18.6 5,2,3
GL103939+251921 159.9126 25.3226 75.2 19.8 -- 19.9 19.1 -- -- -- 15.8 -- 18.9 2,3,4
GL092022-075250 140.0914 -7.8807 49.6 19.2 18.4 19.6 18.6 -- -- -- 17.2 -- 18.5 2,4,3
GL224424-000943 341.1015 -0.1620 70.1 -- -- 18.2 -- -- -- -- 18.8 -- 19.4 1,3,6
GL094909+022851 147.2866 2.4808 88.5 20.4 19.6 15.3 19.3 15.1 -- -- -- -- 14.5 5,2,3
GL094559+030843 146.4950 3.1453 85.8 19.7 19.0 -- 18.8 -- -- -- -- -- 18.2 2,3
GL102905+221246 157.2692 22.2128 92.9 20.0 19.4 -- 19.2 -- -- -- -- -- 19.1 2,3
GL230311-085921 345.7959 -8.9890 104.2 20.4 19.6 -- 19.8 -- -- -- -- 17.6 19.2 2,3,6
GL094036+033437 145.1516 3.5769 73.2 18.3 17.3 -- 17.5 -- 16.5 -- -- -- -- 7,2
GL234745-280828 356.9380 -28.1410 124.7 18.3 17.6 -- 23.8 -- -- -- -- -- -- 2
GL234045-244137 355.1890 -24.6937 98.5 -- 18.5 -- 19.2 -- -- -- -- -- 18.9 3,2
GL230344-071330 345.9325 -7.2250 74.5 20.2 19.7 18.6 19.9 18.2 18.2 -- -- -- 19.0 2,7,3,5
GL103958+240528 159.9915 24.0912 91.6 19.7 18.8 -- 18.8 -- -- -- -- -- -- 2
GL093941-001406 144.9204 -0.2351 72.2 17.1 16.5 -- 16.4 -- -- -- -- -- 17.8 2,3
GL103130+245210 157.8750 24.8693 90.7 19.6 18.6 -- 18.4 -- -- -- -- -- 18.7 2,3
GL110800+365220 166.9981 36.8722 116.9 20.2 19.4 -- 19.4 -- -- -- -- -- 19.0 2,3
GL234729-280634 356.8690 -28.1093 120.3 18.3 17.6 -- 23.8 -- -- -- -- -- -- 2
GL235137-282154 357.9030 -28.3651 121.0 18.4 18.0 -- -- -- -- -- -- -- 18.6 3,2
GL101229+122237 153.1220 12.3771 79.2 19.7 19.3 -- 19.2 -- -- -- -- -- 18.7 2,3
GL093411+001431 143.5443 0.2420 70.9 20.2 19.7 18.6 19.7 17.9 -- -- 17.8 -- 17.7 5,2,3,4
GL225651-085803 344.2120 -8.9674 72.7 -- -- -- -- -- -- 17.9 17.9 -- 19.0 3,6
GL225542-052943 343.9238 -5.4953 43.8 19.2 -- -- 18.2 -- -- -- -- -- 19.4 2,3
GL104801+281447 162.0045 28.2464 92.0 21.6 21.2 -- 21.2 -- -- -- -- -- 21.1 2,3
GL092514-064300 141.3074 -6.7166 88.7 20.0 19.4 -- 19.4 -- -- -- -- -- 18.9 2,3
GL104437+261054 161.1539 26.1816 90.8 -- -- -- -- -- -- -- -- -- 18.9 3
GL232431-190333 351.1310 -19.0591 110.5 19.9 18.8 -- 18.9 -- -- -- 18.1 18.1 19.0 2,3,6
GL000254-341408 0.7269 -34.2357 98.9 -- -- 16.7 -- 17.2 -- -- -- -- -- 5
GL091049-085331 137.7050 -8.8919 27.7 20.0 19.3 -- 19.4 -- -- -- -- -- 18.7 2,3
GL223407+053413 338.5282 5.5703 65.5 19.9 18.9 -- 19.6 -- -- 17.4 17.9 17.5 -- 2,6
GL235624-312111 359.0995 -31.3532 125.1 -- -- -- -- -- -- -- -- -- 17.9 3
GL104703+263235 161.7609 26.5430 91.8 19.7 -- -- 19.0 -- -- -- -- -- 18.7 2,3
GL225138-053326 342.9087 -5.5573 53.2 19.9 19.4 -- 19.8 -- -- -- -- -- 19.2 2,3
GL225641-072245 344.1724 -7.3790 64.2 19.2 18.1 -- 18.5 -- -- -- -- -- -- 2
GL095230+020916 148.1235 2.1544 72.2 19.6 19.0 -- 18.7 -- -- -- -- -- 18.6 2,3
GL095730+080729 149.3742 8.1246 94.6 -- -- -- -- -- -- -- -- -- 19.0 3
GL103617+265744 159.0691 26.9623 92.1 19.5 19.1 -- 19.0 -- -- -- -- -- 19.1 2,3
GL234743-280838 356.9300 -28.1439 117.6 18.3 17.6 -- 23.8 -- -- -- -- -- -- 2
GL093635+010700 144.1473 1.1165 71.3 19.5 18.6 20.6 18.8 -- -- -- 16.2 -- -- 2,4
GL092056-094336 140.2319 -9.7268 56.4 -- -- -- -- -- -- -- -- -- 18.7 3
GL094617+054231 146.5710 5.7087 44.7 19.4 18.8 19.9 18.7 -- 17.1 -- 15.3 -- -- 7,2,4
GL094541+045631 146.4228 4.9419 54.0 19.9 19.2 -- 19.3 -- 17.9 -- -- -- -- 7,2
GL104245+265038 160.6860 26.8438 87.9 20.1 19.6 -- 19.4 -- -- -- -- -- 18.8 2,3
GL110427+381232 166.1138 38.2089 135.9 -- 18.2 -- 17.9 -- 18.1 -- -- -- 18.5 7,3
GL094901+041811 147.2530 4.3030 88.8 -- -- -- -- -- -- -- -- -- 18.6 3
GL094410+022437 146.0433 2.4103 86.7 20.1 19.3 -- -- -- -- -- -- -- -- 2
GL232149-164309 350.4551 -16.7192 85.6 18.6 17.6 -- 18.0 -- -- -- -- -- 19.0 2,3
GL230658-091710 346.7422 -9.2861 103.7 19.8 18.9 -- 19.1 -- -- -- 17.7 -- 18.8 2,3,6
GL101301+170203 153.2554 17.0342 95.9 19.3 19.0 20.6 18.9 17.2 -- -- 16.0 -- 18.6 5,2,4,3
GL093434+000522 143.6430 0.0894 68.4 19.9 19.5 18.6 19.7 17.9 -- -- -- -- 17.6 5,2,3
GL104827+263502 162.1140 26.5838 88.5 27.3 27.3 -- 27.3 -- -- -- -- -- 27.0 2,3
GL110558+362425 166.4920 36.4070 108.1 20.2 19.8 -- 19.5 -- -- -- -- -- 18.6 2,3
GL225544-062712 343.9352 -6.4533 104.7 19.9 19.2 -- 19.5 -- -- -- -- -- -- 2
GL100135+124554 150.3962 12.7649 91.2 19.8 19.3 -- 19.2 -- -- -- -- -- 18.8 2,3
GL235754-314854 359.4764 -31.8151 126.6 -- -- -- -- -- -- -- -- -- 18.0 3
GL100430+144608 151.1230 14.7690 101.5 19.3 18.6 20.0 18.4 -- -- -- 18.0 -- 14.3 4,2,3
GL100545+101636 151.4356 10.2767 104.9 -- -- -- -- -- -- -- -- -- 18.7 3
GL095757+102556 149.4862 10.4323 76.5 20.3 19.8 19.8 19.7 18.0 -- -- 15.8 -- -- 4,5,2
GL095905+102140 149.7714 10.3611 77.6 18.0 16.7 18.6 -- 18.0 -- -- -- -- -- 5,2
GL110759+352748 166.9957 35.4633 125.8 19.7 19.0 -- 19.0 -- -- -- -- -- 18.4 2,3
GL104739+261746 161.9130 26.2961 91.8 19.1 18.0 -- 18.3 -- -- -- -- -- 18.4 2,3
GL095351+085241 148.4630 8.8781 92.4 19.6 18.7 18.4 18.5 17.6 -- -- -- -- 18.8 2,3,5
GL232338-190035 350.9101 -19.0097 112.2 19.7 18.5 -- 19.1 -- -- -- -- -- 19.2 2,3
GL233923-222956 354.8438 -22.4989 112.9 19.2 18.9 -- 19.2 -- -- -- -- -- -- 2
GL120532+513017 181.3840 51.5047 124.3 20.4 19.7 -- 19.4 -- -- -- -- -- 18.8 2,3
GL110916+360116 167.3172 36.0212 92.7 19.9 19.1 -- 19.3 -- -- -- -- -- 18.1 2,3
GL230009-083953 345.0359 -8.6647 107.0 20.2 19.6 -- 19.6 -- -- -- -- -- -- 2
GL110505+352157 166.2693 35.3657 108.9 20.1 19.4 -- 19.1 -- -- -- -- -- 18.1 2,3
GL104552+255705 161.4677 25.9515 90.5 19.6 18.9 -- 18.5 -- -- -- -- -- 18.2 2,3
GL110955+365648 167.4810 36.9465 132.5 20.6 20.0 -- 19.7 -- -- -- -- -- 19.1 2,3
GL094900+022748 147.2477 2.4633 82.6 -- -- -- -- -- -- -- -- -- 14.5 3
GL102626+173038 156.6065 17.5105 80.7 -- -- -- -- -- -- -- -- -- 18.8 3
GL104607+255417 161.5305 25.9049 92.1 19.6 18.9 -- 18.5 -- -- -- -- -- 18.2 2,3
GL234615-280557 356.5627 -28.0990 121.6 -- 18.5 -- 18.8 -- -- -- -- -- -- 2
GL103139+255902 157.9119 25.9840 91.5 18.9 18.6 -- 18.2 -- 18.0 -- -- -- 19.1 7,2,3
GL102241+205133 155.6709 20.8590 107.4 -- -- -- -- -- -- -- -- -- 19.2 3
GL113253+433054 173.2190 43.5150 106.2 23.4 23.1 -- 19.6 -- -- -- -- -- 21.3 2,3
GL095106+090031 147.7751 9.0085 75.2 20.4 19.8 20.0 19.6 18.1 -- -- 17.7 -- 18.9 5,4,2,3
GL093744+024542 144.4330 2.7616 97.9 20.4 19.5 20.7 19.7 -- -- -- -- -- -- 2,4
GL091711-044508 139.2939 -4.7521 51.0 19.6 19.1 19.6 18.8 -- -- -- 17.4 -- 18.0 2,3,4
GL104642+255554 161.6770 25.9317 89.6 20.0 19.4 -- 19.0 -- -- -- -- -- 18.6 2,3
GL102917+260557 157.3200 26.0991 73.6 17.7 -- -- -- -- -- -- -- -- -- 2
GL110958+370810 167.4932 37.1360 113.7 20.2 -- -- 19.4 -- -- -- -- -- -- 2
GL111208+352707 168.0335 35.4520 108.8 20.2 18.8 -- 19.5 -- -- -- -- -- 17.9 2,3
GL094955+090949 147.4781 9.1637 75.6 18.2 17.3 19.7 17.1 15.5 -- -- 17.8 -- -- 5,2,4
GL100836+181353 152.1515 18.2313 73.9 -- -- 20.0 -- -- -- -- 18.2 -- -- 4
GL093411+001430 143.5440 0.2417 66.7 20.2 19.7 17.4 19.7 17.0 -- -- 17.2 -- 13.9 5,2,3,4
GL130847+621618 197.1938 62.2716 118.2 19.8 19.1 -- 18.8 -- -- -- -- -- 18.0 2,3
GL121329+504429 183.3722 50.7415 134.9 19.7 19.2 -- 19.0 -- -- -- -- -- -- 2
GL110542+350704 166.4263 35.1178 125.8 -- -- -- -- -- -- -- -- -- 17.9 3
GL233707-202747 354.2789 -20.4631 115.3 19.0 17.8 -- 18.2 -- -- -- -- -- -- 2
GL225223+010533 343.0941 1.0926 71.3 20.2 18.9 -- 19.2 -- -- -- -- -- -- 2
GL123208+562816 188.0340 56.4711 66.5 20.4 19.9 -- 22.2 -- -- -- -- -- 19.8 2,3
GL123221+563923 188.0891 56.6564 66.6 -- -- -- -- -- -- -- -- -- 17.9 3
GL120251+483811 180.7111 48.6363 49.4 20.1 19.7 -- 19.8 -- -- -- -- -- 18.2 2,3
GL110841+360940 167.1716 36.1610 121.1 -- -- -- -- -- -- -- -- -- 12.3 3
GL092046-080322 140.1927 -8.0562 85.6 -- -- -- -- -- -- -- -- -- 18.5 3
GL231645-185257 349.1889 -18.8825 109.5 19.2 -- -- 18.4 -- -- -- -- -- -- 2
GL130737+621258 196.9038 62.2160 121.1 20.2 19.7 -- 19.6 -- -- -- -- -- 17.9 2,3
GL104827+263501 162.1137 26.5837 91.4 27.3 27.3 -- 27.3 -- -- -- -- -- -- 2
GL120945+563125 182.4386 56.5235 115.1 -- -- -- -- -- -- -- -- -- 17.8 3
GL231022-084119 347.5910 -8.6886 103.0 18.3 17.2 -- 17.4 -- -- -- -- -- -- 2
GL091906-064215 139.7744 -6.7042 87.6 -- -- -- -- -- -- -- -- -- 17.6 3
GL113906+431450 174.7746 43.2473 106.3 20.4 19.9 -- 19.7 -- -- -- -- -- -- 2
GL123600+541315 189.0006 54.2208 77.6 20.2 19.4 -- 19.6 -- -- -- -- -- -- 2
GL111118+352308 167.8252 35.3855 108.8 20.1 19.3 -- 19.9 -- -- -- -- -- 18.1 2,3
GL225716-105700 344.3147 -10.9499 105.2 19.7 18.4 -- 18.9 -- -- -- -- -- -- 2
GL094953+090545 147.4705 9.0959 81.5 15.9 -- 19.7 -- 15.5 -- -- -- -- -- 5,4
GL114916+460713 177.3185 46.1203 94.5 -- -- -- -- -- -- -- -- -- 18.3 3
GL230009-124828 345.0368 -12.8079 50.6 20.1 19.1 -- 19.3 -- -- -- -- -- -- 2
GL114803+461028 177.0139 46.1746 108.5 -- -- -- -- -- -- -- -- -- 18.3 3
GL111451+353008 168.7137 35.5022 93.5 19.9 19.1 -- 19.2 -- -- -- -- -- 17.9 2,3
GL093745+024450 144.4378 2.7473 101.6 20.4 19.5 -- 19.7 -- -- -- -- -- -- 2
GL104532+240900 161.3845 24.1501 88.9 20.2 19.5 -- 19.0 -- -- -- -- -- -- 2
GL120446+491112 181.1925 49.1865 104.5 -- -- -- -- -- -- -- -- -- 17.9 3
GL111522+353007 168.8413 35.5020 92.4 19.9 19.1 -- 19.2 -- -- -- -- -- 17.9 2,3
GL111507+363224 168.7802 36.5401 107.1 20.2 19.3 -- 19.2 -- -- -- -- -- 18.2 2,3
GL103546+210253 158.9420 21.0481 102.5 17.5 -- 18.8 -- 18.0 -- -- -- -- 18.8 5,3
GL111535+363033 168.8966 36.5092 108.8 20.2 19.3 -- 19.2 -- -- -- -- -- 17.9 2,3
GL232235-130539 350.6470 -13.0941 102.5 19.9 18.9 -- 19.0 -- -- -- -- -- -- 2
GL112646+391558 171.6918 39.2662 90.6 -- -- -- -- -- -- -- -- -- 17.8 3
GL111734+360351 169.3902 36.0641 112.8 19.9 19.3 17.8 19.2 16.9 -- -- -- -- 17.8 2,3,5
GL094937+090019 147.4041 9.0053 75.4 18.9 18.1 15.9 17.8 15.5 -- -- 18.1 -- -- 5,2,4
GL111703+360828 169.2646 36.1411 110.5 20.3 19.6 17.8 19.6 16.9 -- -- -- -- -- 2,5
GL112719+383952 171.8290 38.6645 93.8 20.3 -- -- 19.2 -- -- -- -- -- 17.7 2,3
GL122635+525934 186.6451 52.9929 94.6 -- -- -- -- -- -- -- -- -- 18.2 3
GL112001+360603 170.0025 36.1007 110.3 20.5 19.6 -- 19.5 -- -- -- -- -- -- 2
GL113009+383713 172.5390 38.6204 93.3 -- -- -- -- -- -- -- -- -- 17.8 3
GL232407-115139 351.0290 -11.8607 108.1 19.7 18.6 -- 19.1 -- -- -- -- -- -- 2
References for obsid:
1: BAO101cm: 101 cm telescope at Bisei Astronomical Observatory and CCD optical camera (B, V, Rc, Ic)
2: Seimei-TriCCS: 380 cm Seimei telescope (g, r, i)
3: Kiso Schmidt: 105 cm Schmidt telescope at Kiso Observatory and Tomo-e Gozen 20 deg2 fov camera (no filter)
4: Kanata-HONIR: 150 cm Kanata telescope at Higashi-Hiroshima Observatory and HONIR -- a 2 channel imager (Rc and H or J) (Akitaya et al. 2014, Proc. SPIE 9147, 91474O)
5: MITSuME-Akeno: 50 cm MITSuME telescope at Akeno Observatory and a 3 color imager (g, Rc, Ic); The images were processed in real-time through the MITSuME GPU reduction pipeline (Niwano et al. 2021, PASJ, 73, 1, 4-24; https://github.com/MNiwano/Eclaire).
6: Nayuta-NIC: 200 cm Nayuta telescope at Nishi-Harima Astronomical Observatory and Nishiharima Infrared Camera, NIC (J, H, Ks)
7: SaCRA-MuSaSHI: 55 cm SaCRA telescope at Saitama University and MuSaSHI (r, i, z) (Oasa et al., 2020, proc. SPIE, 11447, 114475Z)
GCN Circular 42724
A. Santos (CBPF), C. D. Kilpatrick (Northwestern), C. R. Bom (CBPF), L. Santana-Silva (CBPF), P. Darc (CBPF), Gabriel Teixeira (CBPF), C. Mendes de Oliveira (IAG-USP) report on behalf of the STEP-GW collaboration
Following the subsolar-mass gravitational-wave candidate S251112cm (GCN 42650, 42690), we conducted optical spectroscopic follow-up of four transients: 2025adiw, 2025adim, 2025adhf, and 2025adjf using the Goodman High-Throughput Spectrograph on the SOAR 4.1 m telescope at Cerro Pachón, Chile. Observations were performed on UT 2025 Nov 17 with the 400 l/mm M1 grating, 2×2 binning. For each source we obtained two 900 s exposures and coadded them for analysis. Each target was submitted for spectrum acquisition using the AEON queue. We classified 2025adim, 2025adiw, and 2025adhf as Type Ia supernovae based on SNID-SAGE spectral matches and identifiable SN Ia features. For 2025adjf, the spectra were heavily contaminated by host-galaxy light, preventing a definitive classification, and we instead report the host galaxy redshift based on nebular emission lines in the extracted spectrum. Our classification and redshift estimates are listed as follows:
| AT Name | Classification | redshift |
|---|---|---|
| 2025adim | SN Ia | 0.091 |
| 2025adiw | SN Ia | 0.165 |
| 2025adhf | SN Ia | 0.098 |
| 2025adjf | - | 0.124 |
All classified events are best matched to templates of normal or 91T-like SNe Ia at redshifts inconsistent with the expected distance for S251112cm, and thus are unlikely to be associated with the GW candidate. These results are based on observations obtained through the Astronomical Event Observatory Network (AEON), a joint endeavor of Las Cumbres Observatory and NSF NOIRLab, which is managed by the Association of Universities for Research in Astronomy (AURA) under a cooperative agreement with the U.S. National Science Foundation.
GCN Circular 42722
Z. Y. Liu, W. Zhao, J.-A. Jiang, Z. L. Xu, D. Z. Meng, M. X. Cai, T. G. Wang, X. Kong, Z. G. Dai, L. L. Fan (USTC), Z. P. Jin, Y. Z. Fan (PMO) report on behalf of the WFST Collaboration:
Following the detection of the sub-solar mass merger candidate S251112cm (the LIGO-Virgo-Kagra Collaboration, GCN 42650), we conducted follow-up observations focused on the northern region of the initial bayestar skymap (GCN 42650) using the newly deployed 2.5-meter Wide Field Survey Telescope (WFST Collaboration; Wang et al., 2023) at the Lenghu Astronomical Observation Base (Qinghai province, China). Observations began at UTC 2025-11-13T11:29:36, corresponding to ~20.2 hours after the merger event (UTC 2025-11-12T15:18:45). The follow-ups lasted for three nights until UTC 2025-11-15T23:16:16. We observed in WFST g, r, and i bands with exposure times of 45-90 seconds. A total area of about 727.4 square degrees of the 90% skymap (GCN 42650) was observed, covering ~64% of the event localization. Additionally, ~7.5% skymap was covered in 30s g- and r-band exposures through the WFST wide-field survey (WFS) 6.35 hours after the merger event.
The follow-up observation data were processed using the WFST pipeline. For images localized in WFS, image subtraction was performed using the WFST stacking images taken berfore the event as templates. The search for the counterpart of S251112cm was performed mainly through visual inspection based on the locations of nearby galaxies, considering the distance estimate of 93 +/- 27 Mpc (redshift ~ 0.02; the LIGO-Virgo-Kagra Collaboration, GCN 42690) and the uncertainty of the potential electromagnetic counterpart. All extragalactic transient candidates detected by WFST during follow-ups were reported to the IAU Transient Name Server (TNS).
After excluding sources with pre-merger detections reported in TNS, only one candidate was found to be located near a galaxy with spectroscopic redshift below 0.045: AT2025aebp was first detected at 60992.93 (+1.3 days post-merger) with 21.5 +/- 0.1 mag in r-band, and the spectroscopic redshift of its possible host galaxy SDSS J103703.20+231142.2 is 0.043. Additionally, we report three other sources without pre-merger detections. These sources have possible host galaxies with SDSS DR16 photometric redshift (Csabai et al., 2007; Ahumada et al., 2019) less than 0.1:
| AT Name | MJD | RA | Dec | Filter | Mag | Host | photoZ |
|---|---|---|---|---|---|---|---|
| AT2025aebk | 60992.86 | 156.5043 | 24.9277 | g | 21.8 ± 0.1 | SDSS J102601.47+245542.1 | 0.06 ± 0.02 |
| AT2025aebl | 60992.92 | 152.3554 | 18.2025 | r | 21.4 ± 0.1 | SDSS J100925.32+181207.3 | 0.09 ± 0.03 |
| AT2025aebq | 60992.94 | 172.3128 | 36.6438 | r | 21.4 ± 0.1 | SDSS J112914.78+363832.0 | 0.09 ± 0.03 |
We also checked the aforementioned candidates reported through TNS and GCN Circulars (GCN 42658, GCN 42666, GCN 42677, GCN 42691, GCN 42707