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Bibliographic Details
Main Authors: Wang, Y. L., Zelati, F. Coti, Parent, E., Marino, A., Rea, N., Dhillon, V. S., Blanco-Pozo, J., Ribas, I., Littlefair, S. P., Yang, Z. H., Zhang, G. B., Guillot, S., Ni, K. R., Wu, J. H., Patruno, A., Cavecchi, Y., Illiano, G., Papitto, A., Ambrosino, F., Liu, B. F., Cheng, H. Q., Feng, H., Hu, J. W., Jin, C. C., Sun, H., Tao, L., Xu, Y. J., Yang, H. N., Yuan, W., Zhao, Q. C.
Format: Preprint
Published: 2026
Subjects:
Online Access:https://arxiv.org/abs/2601.11784
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Table of Contents:
  • EP J171159.4-333253 is a new neutron-star low-mass X-ray binary discovered in outburst by the Einstein Probe (EP) on 2025 June 23, exhibiting clocked type-I X-ray bursts, eclipses and dips. In this paper, we report on the results of the X-ray spectral and timing analyses for EP J171159.4-333253 using data collected by EP and NuSTAR during the first 21 days of the outburst. The X-ray burst recurrence time can be characterized over a subset of nine bursts spanning 1.6 days around the NuSTAR observation, and the result is $t_{\rm rec}=8196 \pm 177\,$s with indications of a possible decreasing trend. From the X-ray eclipse events, the binary orbital period and the eclipse duration are estimated to be $P_{\rm orb}=6.48301 \pm 0.00003\,$hr and $D_{\star,X} = 1245.5^{+6.9}_{-6.5}\,$s, respectively. These enable an estimate of the mass and radius of the companion star and the binary inclination, which are $M_2\approx0.6-0.8\,M_\odot$, $R_2\approx0.7-0.8\,R_\odot$ and $i\approx73-75^\circ$, respectively. We also report on joint ULTRACAM and EP observations on 2025 July 21--22, detecting the source optical counterpart and covering an eclipse in both X-ray and optical bands. The optical eclipse is wavelength-dependent and broader than in X-rays, indicating that part of the optical emission arises from an extended region in the accretion flow. Despite a moderate variation in the source flux, the properties of the persistent X-ray emission are typical of a hard spectral state. We further evaluated the ratio of the accretion energy to the thermonuclear energy to be 120--130, implying helium bursts with the accreted hydrogen being depleted in-between bursts.