Srl. No. | Parameter | Value | Unit |
1 |
![]() |
4 |
![]() |
2 | Distance* | 8.4 | kpc |
3 | Inclination* | 90 | degrees |
4 | r0 | 7 | ![]() |
5 | h0 | 9 | ![]() |
6 | B0 | 147 | Gauss |
7 | n0 | 7 | 104 cm![]() |
8 | ![]() |
7 | 1010 K |
9 | t0 | 5.90 | h UT |
10 | ![]() |
1800 | s |
11 | ![]() |
0.60 | |
12 | ![]() |
0.12 |
The mass (
)
and distance were taken from their latest estimates (see
e.g., Gillessen et al. 2009; Reid et al. 2009). Inclination
of the jet axis to the line of sight was fixed to 90 degrees. The base
of the jet is parametrized by radius of the nozzle (r0), location of
the sonic point (h0), magnetic field strength (B0), number density
(n0), and temperature (
)
of the thermal leptons. The flare
is characterized by its start time (t0), duration (
), density
enhancement fraction (
), and expansion speed of the overdense region (
,
as a fraction of the sound speed). Parameters marked with an asterisk (*) were not varied during fitting.
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