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Table 5

Order of magnitude for physical parameters in astrophysical environments.

Objects with ion-electron plasmas (with also pairs) B (G) ne (cm-3) Te (K)

Microquasar coronae, X-ray emitting regiona 105107 10131016 109 10-1105 0.003–1
AGN coronae, X-ray emitting regionb 109 1.7–180 0.03–0.3
Giant radio galaxy lobesc 10-610-5 3 × 10-6 106 0.8–80 0.02–0.2
Extragalactic jet, γ-ray emitting region (<0.05 pc)d 12 80 2 × 105 ~1
Extragalactic jet, radio emitting region (kpc scales)e 1–3 × 10-5 0.8–5 × 10-8 500–2500 ~1
GRB jet, at radius of fast reconnectionf 7 × 108 1010 108 5 × 1012 0.9

Objects with pair plasmas B (G) ne (cm-3) Te (K)

At the termination shock of pulsar windsg 104 0.1–10 1013 ~1
In a pulsar wind nebulaeh 5 × 10-3 5 to 103 γ ~ 10109 <0.5 0.6

Notes.

(c)

Observations, Kronberg et al. (2004).

(d)

Analytical model assuming , Giannios et al. (2009). See also Giroletti et al. (2004) for magnetic field measurements (0.2 G, but on larger scales).

(f)

Analytical model, McKinney & Uzdensky (2012). Pairs are also present, with npair ~ 10ne.

(g)

Analytical model and observations, Bucciantini et al. (2011); Sironi & Spitkovsky (2011a).

(h)

Analytical model and observations, Atoyan & Aharonian (1996); Meyer et al. (2010); Uzdensky et al. (2011); Cerutti et al. (2013). The plasma distribution function is a broken power law with Lorentz factors γ in the indicated range. We note that Cerutti et al. (2013) considers only the high-energy electron population, so have higher magnetizations.

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