• James F. Steiner
  • Edward Nathan
  • Kun Hu
  • Henric Krawczynski
  • Michal Dovčiak
  • Alexandra Veledina
  • Fabio Muleri
  • Jiri Svoboda
  • Kevin Alabarta
  • Maxime Parra
  • Yash Bhargava
  • Giorgio Matt
  • Juri Poutanen
  • Pierre-Olivier Petrucci
  • Allyn F. Tennant
  • M. Cristina Baglio
  • Luca Baldini
  • Samuel Barnier
  • Sudip Bhattacharyya
  • Stefano Bianchi
  • Maimouna Brigitte
  • Mauricio Cabezas
  • Floriane Cangemi
  • Fiamma Capitanio
  • Jacob Casey
  • Nicole Rodriguez Cavero
  • Simone Castellano
  • Elisabetta Cavazzuti
  • Sohee Chun
  • Eugene Churazov
  • Enrico Costa
  • Niccolò Di Lalla
  • Alessandro Di Marco
  • Elise Egron
  • Melissa Ewing
  • Sergio Fabiani
  • Javier A. García
  • David A. Green
  • Victoria Grinberg
  • Petr Hadrava
  • Adam Ingram
  • Philip Kaaret
  • Fabian Kislat
  • Takao Kitaguchi
  • Brankica Kubátová
  • Fabio La Monaca
  • Luca Latronico
  • Christian Malacaria
  • Frédéric Marin
  • Andrea Marinucci
  • Olga Maryeva
  • Guglielmo Mastroserio
  • Tsunefumi Mizuno
  • Michela Negro
  • Nicola Omodei
  • Jakub Podgorný
  • John Rankin
  • Ajay Ratheesh
  • Lauren Rhodes
  • David M. Russell
  • Miroslav Šlechta
  • Paolo Soffitta
  • Sean Spooner
  • Valery Suleimanov
  • Francesco Tombesi
  • Sergei A. Trushkin
  • Martin C. Weisskopf
  • Silvia Zane
  • Andrzej A. Zdziarski
  • Sixuan Zhang
  • Wenda Zhang
  • Menglei Zhou
  • Iván Agudo
  • Lucio A. Antonelli
  • Matteo Bachetti
  • Wayne H. Baumgartner
  • Ronaldo Bellazzini
  • Stephen D. Bongiorno
  • Raffaella Bonino
  • Alessandro Brez
  • Niccolò Bucciantini
  • Chien-Ting Chen
  • Stefano Ciprini
  • Alessandra De Rosa
  • Ettore Del Monte
  • Laura Di Gesu
  • Immacolata Donnarumma
  • Victor Doroshenko
  • Steven R. Ehlert
  • Teruaki Enoto
  • Yuri Evangelista
  • Riccardo Ferrazzoli
  • Shuichi Gunji
  • Kiyoshi Hayashida
  • Jeremy Heyl
  • Wataru Iwakiri
  • Vladimir Karas
  • Jeffery J. Kolodziejczak
  • Ioannis Liodakis
  • Simone Maldera
  • Alberto Manfreda
  • Alan P. Marscher
  • Herman L. Marshall
  • Francesco Massaro
  • Ikuyuki Mitsuishi
  • Chi-Yung Ng
  • Stephen L. O'Dell
  • Chiara Oppedisano
  • Alessandro Papitto
  • George G. Pavlov
  • Abel L. Peirson
  • Matteo Perri
  • Melissa Pesce-Rollins
  • Maura Pilia
  • Andrea Possenti
  • Simonetta Puccetti
  • Brian D. Ramsey
  • Oliver J. Roberts
  • Roger W. Romani
  • Carmelo Sgrò
  • Patrick Slane
  • Gloria Spandre
  • Douglas A. Swartz
  • Toru Tamagawa
  • Fabrizio Tavecchio
  • Roberto Taverna
  • Yuzuru Tawara
  • Nicholas E. Thomas
  • Alessio Trois
  • Sergey S. Tsygankov
  • Roberto Turolla
  • Jacco Vink
  • Kinwah Wu
  • Fei Xie
We present the first X-ray spectropolarimetric results for Cygnus X-1 in its soft state from a campaign of five IXPE observations conducted during 2023 May–June. Companion multiwavelength data during the campaign are likewise shown. The 2–8 keV X-rays exhibit a net polarization degree PD = 1.99% ± 0.13% (68% confidence). The polarization signal is found to increase with energy across the Imaging X-ray Polarimetry Explorer's (IXPE) 2–8 keV bandpass. The polarized X-rays exhibit an energy-independent polarization angle of PA = ‑25.°7 ± 1.°8 east of north (68% confidence). This is consistent with being aligned to Cyg X-1's au-scale compact radio jet and its parsec-scale radio lobes. In comparison to earlier hard-state observations, the soft state exhibits a factor of 2 lower polarization degree but a similar trend with energy and a similar (also energy-independent) position angle. When scaling by the natural unit of the disk temperature, we find the appearance of a consistent trend line in the polarization degree between the soft and hard states. Our favored polarimetric model indicates that Cyg X-1's spin is likely high (a * ≳ 0.96). The substantial X-ray polarization in Cyg X-1's soft state is most readily explained as resulting from a large portion of X-rays emitted from the disk returning and reflecting off the disk surface, generating a high polarization degree and a polarization direction parallel to the black hole spin axis and radio jet. In IXPE's bandpass, the polarization signal is dominated by the returning reflection emission. This constitutes polarimetric evidence for strong gravitational lensing of X-rays close to the black hole.
Original languageEnglish
Article numberL30
JournalThe Astrophysical Journal
Volume969
Issue number2
DOIs
StatePublished - 1 Jul 2024

ID: 125280729