Diverse Polarimetric Features of AGN Jets from Various Viewing Angles Towards a Unified View

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Citation: Tsunetoe, Y.; Mineshige, S.;
Kawashima, T.; Ohsuga, K.; Akiyama,
K.; Takahashi, H.R. Diverse
Polarimetric Features of AGN Jets
from Various Viewing Angles:
Towards a Unified View. Preprints
2022,10, 103. https://doi.org/
10.3390/galaxies10050103
Academic Editor: Luigina Feretti
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Copyright: © 2022 by the authors.
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Attribution (CC BY) license (https://
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4.0/).
Article
Diverse Polarimetric Features of AGN Jets from Various Viewing
Angles: Towards a Unified View
Yuh Tsunetoe 1,* , Shin Mineshige 1, Tomohisa Kawashima 2, Ken Ohsuga 3, Kazunori Akiyama 4,5,6 and
Hiroyuki R. Takahashi 7
1Department of Astronomy, Kyoto University, Kyoto 606-8501, Japan
2Institute for Cosmic Ray Research, University of Tokyo, Tokyo 113-8654, Japan
3Center for Computational Sciences, University of Tsukuba, Ibaraki 305-8577, Japan
4Haystack Observatory, Massachusetts Institute of Technology, 99 Millstone Road MA 01886, USA
5Black Hole Initiative, Harvard University, 20 Garden Street, Cambridge MA 02138, USA
6National Astronomical Observatory of Japan, 2-21-1 Osawa, Mitaka-shi Tokyo, 181-8588, Japan
7Department of Natural Sciences, Faculty of Arts and Sciences, Komazawa University, Tokyo 154-8525, Japan
*Correspondence: tsunetoe@kusastro.kyoto-u.ac.jp
Abstract:
Here, we demonstrate that polarization properties show a wide diversity depending on viewing
angles. To simulate images of a supermassive black hole and surrounding plasma, we performed a
full-polarimetric general relativistic radiative transfer based on three-dimensional general relativistic
magnetohydrodynamics models with moderate magnetic strengths. Under an assumption of a hot-jet
and cold-disk in the electron temperature prescription, we confirmed a typical scenario where polarized
synchrotron emissions from the funnel jet experience Faraday rotation and conversion in the equatorial
disk. Further, we found that linear polarization vectors are inevitably depolarized for edge-on-like
observers, whereas a portion of vectors survive and reach the observers in face-on-like cases. We also
found that circular polarization components have persistent signs in the face-on cases, and changing
signs in the edge-on cases. It is confirmed that these features are smoothly connected via intermediate
viewing-angle cases. These results are due to Faraday rotation/conversion for different viewing angles,
and suggest that a combination of linear and circular polarimetry can give a constraint on the inclination
between the observer and black hole’s (and/or disk’s) rotating-axis and plasma properties in the jet–disk
structure. These can also lead to a more statistical and unified interpretation for a diversity of emissions
from active galactic nuclei.
Keywords:
black hole physics; accretion disks; active galactic nuclei; radio jets; radiative transfer;
polarimetry
1. Introduction
The direct images of supermassive black holes (SMBH) M87* and Sgr A* by the Event
Horizon Telescope (EHT) have opened a new era of black hole studies [
1
,
2
]. In particular,
the polarimetric images around the black holes have attracted attention as they can reflect
the configuration of magnetic fields around the SMBH [
3
]. It has been established from
theoretical approaches that the magnetic fields should have an important role in the creation
and acceleration of the jets from active galactic nuclei (AGNs) hosting the SMBHs [
4
,
5
]. We can
thus expect to shed new light on the long-standing question of the driving mechanism of AGN
jets through these unprecedented high-resolution observations.
However, one should also note that the polarized synchrotron emissions from a SMBH
can experience Faraday effects on the way to Earth. Observational studies have detected traces
of significant Faraday rotation of the linear polarization (LP) vectors in a range of millimeter
and submillimeter wavelengths for many AGNs with/without jets [
6
9
]. It has been pointed
out by theoretical studies that these should be attributed to internal Faraday rotation; that is,
arXiv:2210.12162v1 [astro-ph.HE] 21 Oct 2022
2 of 11
Figure 1.
A schematic picture of the jet–disk structure (adopted from Tsunetoe et al.
[18]
). In our
model, synchrotron emission is predominantly produced in the funnel jet (green). After the emission,
the polarized lights experience Faraday conversion in the inner hot disk (red) and Faraday rotation in the
outer cold disk (blue) on the way to the observer (eyeball), respectively. See [
18
] for poloidal-slice maps
of typical values of the emissivity and Faraday coefficients.
the Faraday rotation should occur in tandem with the emission near an SMBH, e.g., [
10
12
].
Furthermore, recent calculations have demonstrated that significant Faraday conversion from
LP to circular polarization (CP) can occur near a SMBH [
11
,
13
,
14
]. In such cases, CP components
of the combination between the intrinsic emission and conversion from LP components can be
a good tool for investigating the magnetic field structure.
In this way, it has been established that the unified interpretation of both LP and CP is
essential for understanding the magnetic structure and other plasma properties around an
SMBH. In this context, we have thought of calculating the polarization images theoretically.
To predict images around and near a BH, we must take general relativistic (GR) effects into
account, and, here, perform the GR radiative transfer (GRRT) calculation based on the GR
magnetohydrodynamics (GRMHD) models, e.g., [1517].
In the previous work Tsunetoe et al.
[18]
, we confirmed, on the basis of our moderately
magnetized models with a hot jet and cold disk, a scenario where the polarized emissions
produced in the jet experience the Faraday rotation and conversion effects in the disk. In this
description of the emitting jet and Faraday-thick disk, we found that the LP (or CP) intensities
Parameter Value
BH mass M6.5 ×109M
BH spin parameter a0.9375
Magnetic flux on the horizon φ18 (semi-MAD)
Te-parameter Rlow 1
Te-parameter Rhigh 73
Mass accretion rate onto BH ˙
M6×104Myr1(at the moment of snapshot)
Distance to observer D16.7 Mpc
Observational frequency ν230 GHz
Table 1.
Parameters in our GRMHD and GRRT model, following a fiducial model in [
18
], except the
observer’s inclination angle. Here,
M
is the solar mass.
φΦBH/q˙
Mrgc2
is a strength of dimensionless
magnetic flux on the event horizon of SMBH, where
rgGM/c2
and
ΦBH = (
1
/
2
)R R |Br|
d
Aθφ
.
G
and care the gravitational constant and speed of light, respectively.
3 of 11
Figure 2.
A calculated polarization images at 230 GHz for three viewing angles of
i=
20
(nearly
face-on), 50
(intermediate), and 90
(edge-on), top to bottom. (
Left
) Total intensity (Stokes
I
) image.
Each image consists of 600
×
600 pixels. The forward jet extends upward on the image. (
Center
) LP map.
The LP intensity is shown by the color contour, with LP vectors in electric vector position angle (EVPA)
overwritten. (
Right
) CP image. The CP intensity (Stokes
V
) is shown by the color contour with sign. A
movie of all the images for
i=
0
180
can be found on https://youtu.be/065qAx6Tff0 (accessed on
October 19, 2022).
are mainly distributed in the downstream (upstream) side of the approaching jet for nearly face-
on observers. In this work, we surveyed polarimetric features for different inclination angles
between the black hole’s spin-axis and an observer, to expand and develop the discussions.
Here, we bore in mind observations of a diverse range of AGN jets at 230 GHz by the EHT and
other very long baseline interferometers (VLBIs). Furthermore, we thought of applying them
to the interpretation of the disk precession around SMBHs [19,20].
2. Methods
We followed the model parameters adopted in the fiducial model in [
18
]. Here, we used a
three-dimensional GRMHD model simulated with
UWABAMI
code [
21
,
22
], which is categorized
into the intermediary area between a magnetically arrested disk (MAD; [
23
]) and standard and
normal evolution (SANE; [
24
]), and is thus called semi-MAD. The
Rβ
model was adopted
for the determination of electron temperature, where the proton–electron temperature ratio
摘要:

Citation:Tsunetoe,Y.;Mineshige,S.;Kawashima,T.;Ohsuga,K.;Akiyama,K.;Takahashi,H.R.DiversePolarimetricFeaturesofAGNJetsfromVariousViewingAngles:TowardsaUniedView.Preprints2022,10,103.https://doi.org/10.3390/galaxies10050103AcademicEditor:LuiginaFerettiPublisher'sNote:MDPIstaysneutralwithregardtojuri...

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