A Helical Magnetic Field in the jet of 3C 273(Session 1:Astrophysical Jets,High-Energy Emission from Accreting Compact Objects,Korea-Japan Seminar)

Both in the Faraday Rotation Measure and the intrinsic polarization angle, new features are revealed to indicate a helical magnetic field operating along the jet of the bright active galactic nucleus 3C 273. The helical field has been suggested to be related to the formation and collimation of jets by magnetohydrodynamic models. The distribution of the rotation measure shows a systematic gradient with respect to the jet axis, which is expected by a helical magnetic field. In addition, the helical field can consistently explain two types in the direction of the projected magnetic field: parallel and perpendicular to the jet axis. Further, if the helical magnetic field is generated by winding up of an initial field by rotation of the accretion disk, we can uniquely determine the direction of the disk rotation, since the jet is approaching us.

[1]  M. H. Edwards Astrophysical Phenomena Revealed by Space VLBI , 2000 .

[2]  D. Meier,et al.  Extraction of Black Hole Rotational Energy by a Magnetic Field and the Formation of Relativistic Jets , 2002, Science.

[3]  A. Lobanov,et al.  A Cosmic Double Helix in the Archetypical Quasar 3C273 , 2001, Science.

[4]  R. Zavala,et al.  Time-Variable Faraday Rotation Measures of 3C 273 and 3C 279 , 2001, astro-ph/0103180.

[5]  D. Meier,et al.  Magnetohydrodynamic production of relativistic jets. , 2001, Science.

[6]  A. Pushkarev,et al.  Analysis of λ = 6 cm VLBI polarization observations of a complete sample of northern BL Lacertae objects , 2000, astro-ph/0307192.

[7]  M. H. Edwards Astrophysical Phenomena Revealed by Space VLBI , 2000 .

[8]  John A. Biretta,et al.  Formation of the radio jet in M87 at 100 Schwarzschild radii from the central black hole , 1999, Nature.

[9]  D. H. Roberts,et al.  Radio Jet-Ambient Medium Interactions on Parsec Scales in the Blazar 1055+018 , 1999, astro-ph/9903330.

[10]  G. Taylor Magnetic Fields in Quasar Cores , 1998 .

[11]  J. Anton Zensus,et al.  PARSEC-SCALE JETS IN EXTRAGALACTIC RADIO SOURCES1 , 1997 .

[12]  W. Sparks,et al.  The Supermassive Black Hole of M87 and the Kinematics of Its Associated Gaseous Disk , 1997, astro-ph/9706252.

[13]  M. Sikora,et al.  Radiation drag in relativistic active galactic nucleus jets , 1996 .

[14]  J. Zensus,et al.  Linear Polarization Imaging with Very Long Baseline Interferometry at High Frequencies , 1995 .

[15]  Naomasa Nakai,et al.  Evidence for a black hole from high rotation velocities in a sub-parsec region of NGC4258 , 1995, Nature.

[16]  H. Ford,et al.  HST FOS spectroscopy of M87: Evidence for a disk of ionized gas around a massive black hole , 1994 .

[17]  H. Ford,et al.  Narrowband HST images of M87: Evidence for a disk of ionized gas around a massive black hole , 1994 .

[18]  D. H. Roberts,et al.  A survey of the milliarcsecond polarization properties of BL Lacertae objects at 5 GHz , 1992 .

[19]  D. H. Roberts,et al.  Milliarcsecond polarization structure of the superluminal quasar 3C 273 , 1990 .

[20]  D. H. Roberts,et al.  The milliarcsecond polarization structure of six BL Lacertae objects , 1989 .

[21]  T. Kuzhir,et al.  Modification of chemical mutagenesis by antioxidants (AOs) in germ and somatic cells , 1989 .

[22]  K. Shibata,et al.  Magnetodynamical acceleration of cosmic jets: sweeping-magnetic-twist mechanism , 1986 .

[23]  T. Jones,et al.  Rotation measures for compact variable radio sources , 1983 .

[24]  R. Blandford,et al.  Hydromagnetic flows from accretion discs and the production of radio jets , 1982 .

[25]  V. Icke Gas flow above an alpha disk , 1980 .

[26]  G. Benford Current-carrying beams in astrophysics: models for double radio sources and jets , 1978 .

[27]  W. Cannon,et al.  The small-scale structure of radio galaxies and quasi-stellar sources at 3.8 centimeters. , 1971 .