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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3.7. The magnetic field power spectrum 37<br />
Figure 3.6: Comparison of theσ RM profiles obtained from simulations of a Gaussian and random<br />
magnetic field (solid line) and the expectations from the analytical model of Eq. 3.9 by assuming<br />
three <strong>di</strong>fferentΛ c :Λ min =6 kpc,Λ B =Λ Bz = 16 kpc,Λ RM =69 kpc (dashed and dotted lines). The<br />
best agreement is given byΛ c =Λ B . The simulated magnetic field power spectrum has slope n=2.<br />
The source is assumed to be halfway through the cluster and the magnetic field strength and gas<br />
density have the same ra<strong>di</strong>al profiles in both the simulations and the analytical formulation. Taken<br />
from Murgia et al. (2004).<br />
be identical and the approximationΛ c =Λ RM has been used in the single-scale model (Eq. 3.9),<br />
lea<strong>di</strong>ng to underestimates of the magnetic field strength. Murgia et al. (2004) have shown thatΛ B<br />
is a good approximation forΛ c in Eq. 3.9 and therefore that this length must be used to compare<br />
the analytical pre<strong>di</strong>ctions from the single-scale model with RM analyses assuming a multi-scale<br />
field (Fig. 3.6). SinceΛ B depends on the underlying magnetic field power spectrum (Eq. 3.10), the<br />
latter must be estimated first.<br />
Multiple <strong>di</strong>fferent estimators of spatial statistics of the RM <strong>di</strong>stributions such as structure and<br />
auto-correlation functions or a multi-scale statistic have been used to derive the field strength, its<br />
relation to the gas density and its power spectrum (Murgia et al. 2004; Govoni et al. 2006; Guidetti<br />
et al. 2008; Laing et al. 2008). The technique of Bayesian maximum likelihood has also been used<br />
for this purpose (Enßlin & Vogt 2005; Kuchar & Enßlin 2009). These stu<strong>di</strong>es have shown that the<br />
magnetic field power spectrum is well approximated by a power-law<br />
ŵ( f )∝ f −q (3.11)<br />
over a range of spatial frequencies, correspon<strong>di</strong>ng respectively to the outer and inner fluctuation<br />
scales of the magnetic field 2 . Although the theory of intergalactic magnetic field fluctuations is<br />
still debated, a power-law functional form is expected if the turbulence is mostly hydrodynamic,<br />
2 Spatial frequency and scale are related in the sense: f= 1/Λ<br />
37