Quasi-periodic Faraday-rotation fluctuations of the polarization plane during radio sounding of the circumsolar plasma

2013 ◽  
Vol 58 (9) ◽  
pp. 901-910 ◽  
Author(s):  
A. I. Efimov ◽  
L. A. Lukanina ◽  
A. I. Rogashkova ◽  
L. N. Samoznaev ◽  
I. V. Chashei ◽  
...  
2015 ◽  
Vol 59 (4) ◽  
pp. 313-326 ◽  
Author(s):  
A. I. Efimov ◽  
L. A. Lukanina ◽  
A. I. Rogashkova ◽  
L. N. Samoznaev ◽  
I. V. Chashei ◽  
...  

2009 ◽  
Vol 53 (3) ◽  
pp. 252-261 ◽  
Author(s):  
T. V. Smirnova ◽  
I. V. Chashei ◽  
V. I. Shishov

2020 ◽  
Vol 498 (4) ◽  
pp. 5468-5488
Author(s):  
Angelo Ricarte ◽  
Ben S Prather ◽  
George N Wong ◽  
Ramesh Narayan ◽  
Charles Gammie ◽  
...  

ABSTRACT Faraday rotation has been seen at millimeter wavelengths in several low-luminosity active galactic nuclei, including Event Horizon Telescope (EHT) targets M87* and Sgr A*. The observed rotation measure (RM) probes the density, magnetic field, and temperature of material integrated along the line of sight. To better understand how accretion disc conditions are reflected in the RM, we perform polarized radiative transfer calculations using a set of general relativistic magnetohydrodynamic (GRMHD) simulations appropriate for M87*. We find that in spatially resolved millimetre wavelength images on event horizon scales, the RM can vary by orders of magnitude and even flip sign. The observational consequences of this spatial structure include significant time-variability, sign-flips, and non-λ2 evolution of the polarization plane. For some models, we find that internal RM can cause significant bandwidth depolarization even across the relatively narrow fractional bandwidths observed by the EHT. We decompose the linearly polarized emission in these models based on their RM and find that emission in front of the mid-plane can exhibit orders of magnitude less Faraday rotation than emission originating from behind the mid-plane or within the photon ring. We confirm that the spatially unresolved (i.e. image integrated) RM is a poor predictor of the accretion rate, with substantial scatter stemming from time variability and inclination effects. Models can be constrained with repeated observations to characterize time variability and the degree of non-λ2 evolution of the polarization plane.


2013 ◽  
Vol 58 (5) ◽  
pp. 429-439 ◽  
Author(s):  
A. I. Efimov ◽  
L. A. Lukanina ◽  
A. I. Rogashkova ◽  
L. N. Samozhaev ◽  
I. V. Chashei ◽  
...  

2013 ◽  
Vol 51 (1) ◽  
pp. 13-22 ◽  
Author(s):  
A. I. Efimov ◽  
L. A. Lukanina ◽  
V. K. Rudash ◽  
L. N. Samoznaev ◽  
I. V. Chashei ◽  
...  

2011 ◽  
Vol 56 (12) ◽  
pp. 1407-1416 ◽  
Author(s):  
A. I. Efimov ◽  
L. A. Lukanina ◽  
A. I. Rogashkova ◽  
L. N. Samoznaev ◽  
I. V. Chashei ◽  
...  

2020 ◽  
Vol 637 ◽  
pp. L6
Author(s):  
E. Kravchenko ◽  
M. Giroletti ◽  
K. Hada ◽  
D. L. Meier ◽  
M. Nakamura ◽  
...  

We report on high angular resolution polarimetric observations of the nearby radio galaxy M87 using the Very Long Baseline Array at 24 GHz (λ = 1.3 cm) and 43 GHz (λ = 7 mm) in 2017–2018. New images of the linear polarization substructure in the nuclear region are presented, characterized by a two-component pattern of polarized intensity and smooth rotation of the polarization plane around the 43 GHz core. From a comparison with an analogous dataset from 2007, we find that this global polarization pattern remains stable on a time interval of 11 yr, while showing smaller month-scale variability. We discuss the possible Faraday rotation toward the M87 nucleus at centimeter to millimeter wavelengths. These results can be interpreted in a scenario where the observed polarimetric pattern is associated with the magnetic structure in the confining magnetohydrodynamic wind, which also serves as the source of the observed Faraday rotation.


1988 ◽  
Vol 126 ◽  
pp. 689-690
Author(s):  
Yu. N. Gnedin ◽  
T. M. Natsvlishvili

Two new methods for the detection of hot gas in globular clusters are proposed: 1. measurement of the position change of a radio source due to refraction and 2. determination of the concentration of hot gas using the Faraday rotation of the polarization plane of the background radio source radiation.


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