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UHECRs and Multiple Shock Acceleration in Active Galactic ... - TAUP

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Diffusive shock acceleration<br />

• Test particle - diffusion - n acceleration shock cycles<br />

E<br />

n ( x + 1) ⋅ E0<br />

• Energy ga<strong>in</strong>: fraction of <strong>in</strong>itial energy<br />

• Average energy ga<strong>in</strong> per collision:<br />

n<br />

=<br />

ΔE<br />

= E − E = x⋅<br />

E<br />

< ΔE<br />

/ E >≅ ( 2V<br />

/ c)<br />

• Lead<strong>in</strong>g to a power-law energy behaviour<br />

∞<br />

i=<br />

n<br />

n(<br />

E)<br />

−σ<br />

( 1−<br />

P ) = ... ∝<br />

N(<br />

> E)<br />

= ∑ E<br />

σ = (r+2)/(r-1), r = V1/V2 = (γ +1) / ( γ -1)<br />

esc<br />

for mono-atomic gas:<br />

γ =5/3 r = 4 E -2<br />

Note: for non-relativistic shocks σ is ‘constant’ ,<br />

<strong>in</strong>dependent of scatter<strong>in</strong>g media or shock <strong>in</strong>cl<strong>in</strong>ation<br />

0<br />

0<br />

Probability of scatter<strong>in</strong>g x av.no. scatter<strong>in</strong>gs x ΔE<br />

Upstream Downstream<br />

(e.g. Krymskii ‘77, Bell ’78, Drury ’83 )

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