TITLE: GCN CIRCULAR NUMBER: 31187 SUBJECT: Chandra observation of GW170817 at ~1573 days since merger (Epoch 1 of 4) DATE: 21/12/08 14:05:45 GMT FROM: Aprajita Hajela at Northwestern U A. Hajela (Northwestern U.), R. Margutti (UC Berkeley), K. D. Alexander (Northwestern U.), T. Laskar (Radboud U.), R. Chornock (UC Berkeley), E. Berger (Harvard), V. Ashley Villar (PSU) report: We have acquired X-ray observations of GW170817 with the Chandra X-ray Observatory (CXO) at t ~ 1573 days (~ 4.3 years) after the binary neutron star merger. We report here the preliminary results from the first epoch (ObsID 23869; PI Margutti; program 22510329), for a total exposure time of 28.5 ks (out of a total of 100 ks requested; we will report on the results from the complete data set in the next few days). After aligning the images to a common astrometric solution as described in Hajela et al., 2021, we find evidence for X-ray emission at the location of GW170817 with a statistical significance of 3.8 sigma (Gaussian equivalent) corresponding to a net count-rate of (1.31 +/- 0.72)e-04 c/s (0.5 - 8 keV). Assuming a simple absorbed power-law spectral model with a photon index Gamma ~ 1.6, no intrinsic absorption (NH,int = 0 cm-2 as found in e.g. Hajela et al. 2019) and Galactic neutral hydrogen column density NH,gal = 7.8e+20 cm-2 (Kalberla et al., 2005), we derive an unabsorbed flux of ~ 1.7e-15 erg/cm2/s (0.3-10 keV), corresponding to a luminosity of ~3.4e+38 erg/s at the distance of 40.7 Mpc (Cantiello et al., 2018). Based on the extrapolation of the jet afterglow models calculated with JetFit (gammaB=12) and the universal post jet break models with start time tstart=196 days as calculated in Hajela et al., 2021, and the observed background, the expected number of photons within a 1” region at the location of GW170817 is ~0.55 (0.5-8 keV, exposure time of 28.5 ks). The observed number of counts after Xspec filtering corresponds to a ~10% chance fluctuation probability for universal post jet break models (~12% for JetFit). For this choice of tstart and gammaB, the total probability of observing at least as many counts as those collected for GW170817 at t>900 days based on jet afterglow models as a result of a chance fluctuation is ~6e-5 (~ 4.0 sigma Gaussian equivalent, for the universal post jet break model) and ~3e-5 (~ 4.2 sigma Gaussian equivalent for JetFit). The remaining ~75 ks of planned CXO observations will further constrain the statistical evidence of an excess of X-ray emission in GW170817 with respect to jet afterglow models as reported in Hajela et al., 2021. We thank the entire Chandra team for scheduling and executing these observations.