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  • Dawoon E. Kim
  • Laura Di Gesu
  • Ioannis Liodakis
  • Alan P. Marscher
  • Riccardo Middei
  • Herman L. Marshall
  • Luigi Pacciani
  • Ivan Agudo
  • Fabrizio Tavecchio
  • Nicoló Cibrario
  • Stefano Tugliani
  • Raffaella Bonino
  • Michela Negro
  • Simonetta Puccetti
  • Francesco Tombesi
  • Enrico Costa
  • Immacolata Donnarumma
  • Paolo Soffitta
  • Tsunefumi Mizuno
  • Yasushi Fukazawa
  • Koji S. Kawabata
  • Tatsuya Nakaoka
  • Makoto Uemura
  • Ryo Imazawa
  • Mahito Sasada
  • Hiroshi Akitaya
  • Francisco Josè Aceituno
  • Giacomo Bonnoli
  • Vìctor Casanova
  • Ioannis Myserlis
  • Albrecht Sievers
  • Emmanouil Angelakis
  • Alexander Kraus
  • Whee Yeon Cheong
  • Hyeon-Woo Jeong
  • Sincheol Kang
  • Sang-Hyun Kim
  • Sang-Sung Lee
  • Beatriz Agìs-Gonzàlez
  • Alfredo Sota
  • Juan Escudero
  • Mark Gurwell
  • Garrett K. Keating
  • Ramprasad Rao
  • Pouya M. Kouch
  • Elina Lindfors
  • Ioakeim G. Bourbah
  • Sebastian Kiehlmann
  • Evangelos Kontopodis
  • Nikos Mandarakas
  • Stylianos Romanopoulos
  • Raphael Skalidis
  • Anna Vervelaki
  • Lucio A. Antonelli
  • Matteo Bachetti
  • Luca Baldini
  • Wayne H. Baumgartner
  • Ronaldo Bellazzini
  • Stefano Bianchi
  • Stephen D. Bongiorno
  • Alessandro Brez
  • Niccoló Bucciantini
  • Fiamma Capitanio
  • Simone Castellano
  • Elisabetta Cavazzuti
  • Chien-Ting Chen
  • Stefano Ciprini
  • Alessandra De Rosa
  • Ettore Del Monte
  • Niccoló Di Lalla
  • Alessandro Di Marco
  • Victor Doroshenko
  • Michal Dovčiak
  • Steven R. Ehlert
  • Teruaki Enoto
  • Yuri Evangelista
  • Sergio Fabiani
  • Riccardo Ferrazzoli
  • Javier A. Garcia
  • Shuichi Gunji
  • Kiyoshi Hayashida
  • Jeremy Heyl
  • Wataru Iwakiri
  • Philip Kaaret
  • Vladimir Karas
  • Fabian Kislat
  • Takao Kitaguchi
  • Jeffery J. Kolodziejczak
  • Henric Krawczynski
  • Fabio La Monaca
  • Luca Latronico
  • Simone Maldera
  • Alberto Manfreda
  • Frédéric Marin
  • Andrea Marinucci
  • Francesco Massaro
  • Giorgio Matt
  • Ikuyuki Mitsuishi
  • Fabio Muleri
  • C. -Y. Ng
  • Stephen L. O'Dell
  • Nicola Omodei
  • Chiara Oppedisano
  • Alessandro Papitto
  • George G. Pavlov
  • Abel L. Peirson
  • Matteo Perri
  • Melissa Pesce-Rollins
  • Pierre-Olivier Petrucci
  • Maura Pilia
  • Andrea Possenti
  • Juri Poutanen
  • Brian D. Ramsey
  • John Rankin
  • Ajay Ratheesh
  • Oliver Roberts
  • Roger W. Romani
  • Carmelo Sgró
  • Patrick Slane
  • Gloria Spandre
  • Doug Swartz
  • Toru Tamagawa
  • Roberto Taverna
  • Yuzuru Tawara
  • Allyn F. Tennant
  • Nicholas E. Thomas
  • Alessio Trois
  • Sergey S. Tsygankov
  • Roberto Turolla
  • Jacco Vink
  • Martin C. Weisskopf
  • Kinwah Wu
  • Fei Xie
  • Silvia Zane
Aims. We aim to probe the magnetic field geometry and particle acceleration mechanism in the relativistic jets of supermassive black holes. Methods. We conducted a polarimetry campaign from radio to X-ray wavelengths of the high-synchrotron-peak (HSP) blazar Mrk 421, including Imaging X-ray Polarimetry Explorer (IXPE) measurements from 2022 December 6-8. During the IXPE observation, we also monitored Mrk 421 using Swift-XRT and obtained a single observation with XMM-Newton to improve the X-ray spectral analysis. The time-averaged X-ray polarization was determined consistently using the event-by-event Stokes parameter analysis, spectropolarimetric fit, and maximum likelihood methods. We examined the polarization variability over both time and energy, the former via analysis of IXPE data obtained over a time span of 7 months. Results. We detected X-ray polarization of Mrk 421 with a degree of ΠX = 14 ± 1% and an electric-vector position angle ΨX = 107 ± 3 in the 2-8 keV band. From the time variability analysis, we find a significant episodic variation in ΨX. During the 7 months from the first IXPE pointing of Mrk 421 in 2022 May, ΨX varied in the range 0 to 180, while ΠX remained relatively constant within ∼10-15%. Furthermore, a swing in ΨX in 2022 June was accompanied by simultaneous spectral variations. The results of the multiwavelength polarimetry show that ΠX was generally ∼2-3 times greater than Π at longer wavelengths, while Ψfluctuated. Additionally, based on radio, infrared, and optical polarimetry, we find that the rotation of Ψoccurred in the opposite direction with respect to the rotation of ΨX and over longer timescales at similar epochs. Conclusions. The polarization behavior observed across multiple wavelengths is consistent with previous IXPE findings for HSP blazars. This result favors the energy-stratified shock model developed to explain variable emission in relativistic jets. We considered two versions of the model, one with linear and the other with radial stratification geometry, to explain the rotation of ΨX. The accompanying spectral variation during the ΨX rotation can be explained by a fluctuation in the physical conditions, for example in the energy distribution of relativistic electrons. The opposite rotation direction of Ψbetween the X-ray and longer wavelength polarization accentuates the conclusion that the X-ray emitting region is spatially separated from that at longer wavelengths. Moreover, we identify a highly polarized knot of radio emission moving down the parsec-scale jet during the episode of ΨX rotation, although it is unclear whether there is any connection between the two events.
Original languageEnglish
Article numberA12
Number of pages17
JournalAstronomy and Astrophysics
Volume681
DOIs
StatePublished - 1 Jan 2024

    Research areas

  • BL Lacertae objects: individual: HSP, Galaxies: jets, Magnetic fields, Polarization, Relativistic processes

ID: 124379401