Alma Mater Studiorum Universit`a degli Studi di Bologna ... - Inaf
Alma Mater Studiorum Universit`a degli Studi di Bologna ... - Inaf
Alma Mater Studiorum Universit`a degli Studi di Bologna ... - Inaf
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1.2. Non-thermal emission mechanisms of active galaxies 3<br />
fields in astrophysical sources.<br />
Lorentz factorγ(electron energyǫ=γm e c 2 ) is:<br />
dǫ<br />
dt<br />
The synchrotron power emitted by a relativistic electron with<br />
[ erg<br />
]<br />
≃ 1.6×10 −3 (B [µG] sinθ) 2 γ 2 (1.1)<br />
s<br />
where θ is the pitch angle between the electron velocity and the magnetic field <strong>di</strong>rection.<br />
This equation illustrates the degeneracy between particle energy and magnetic field: a given<br />
synchrotron power can be produced by a highly energetic particle in a low magnetic field or vice<br />
versa.<br />
The spectral <strong>di</strong>stribution for a single electron can be assumed to be approximately<br />
monochromatic since it peaks sharply at a frequency:<br />
ν c [GHz]≃4.2×10 −9 γ 2 (B [µG] sinθ). (1.2)<br />
From Eq. 1.2, it is derived that electrons ofγ≃10 4 in magnetic fields of B≃10µG produce<br />
synchrotron ra<strong>di</strong>ation in the ra<strong>di</strong>o band (ν c ∼ 4 GHz), whereas electrons ofγ ≃ 10 7−8 in the<br />
same magnetic field ra<strong>di</strong>ate in the X-rays. A representative example is given by the nearby active<br />
galaxy Pictor A, where the spectrum of the jet from ra<strong>di</strong>o to X-ray wavelengths can be described<br />
as synchrotron emission from a population highly energetic particles with a <strong>di</strong>stribution of Lorentz<br />
factors (Wilson, Young & Shopbell 2001).<br />
For a homogeneous population of electrons with an isotropic pitch-angle <strong>di</strong>stribution and a<br />
power-law energy spectrum with the particle density between energiesǫ andǫ+dǫ given by<br />
N(ǫ)dǫ= N 0 ǫ −δ dǫ, (1.3)<br />
the total intensity spectrum, in optically-thin regions has the functional form:<br />
S (ν)∝ν −α , (1.4)<br />
where the spectral indexα=(δ−1)/2. This spectrum of Eq. 1.4 is described as non-thermal,<br />
since the energy spectrum of the emitting particles is not Maxwellian - i.e. it does not have a<br />
single temperature.<br />
1.2.2 Polarization of synchrotron ra<strong>di</strong>ation<br />
In the optically-thin case, for a homogeneous and isotropic <strong>di</strong>stribution of relativistic particles<br />
whose energy <strong>di</strong>stribution follows the power law of Eq. 1.3 and in a uniform magnetic field, the<br />
3