Date post: | 22-Dec-2015 |
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Alternative Scenario
Small scale and random B? Length scale
Skin length: lsk~c/wpe wpe is plasma frequency
skll )11.0(
Weibel Instability
Generation of random magnetic field: How to obtain mature B ? Weibel instability ---- plasma velocity anisotropic distribution: initial perturbation (by relativistic shocks) --
electrons/positrons move oppositely -- perturbation current -- B production -- until certain balance
Stochastic Magnetic Field Production
Random magnetic field could be generated by turbulence:
dkkFB )(2
Radiation (I)
Radiation by a single relativistic particle in small scale B (Landau & Lifshitz 1971):
)()2
1()(2 '
42'
2
2'
2
2/1
2'3
2
'
2
dwc
eI
Radiation (II)
Space and temporal Fourier transform of Lorentz force(Fleishman 2006, Mao & Wang 2007):
Particularly, jitter radiation, 1D case
))(()()()2
1())(( 000'
0
2/1
42'
2
2'2
'
'
232
4
2
qqqqKqvqdqdqdcm
eI
2222 / pe )/)(2/( 2222' pe
Radiation Spectral Index
K(q) ~<B^2> spectral index frequency depends on the relation
1 I
2/12222 )2//411( kcck pe
ck2
Magnetic Field of GRB
dkkBk
k
2
11 )/( tsheddy Rlk kk 2/1Pr
GB 6102.1 1
51332
62 )
10()
1()
100()
102.1(102.5
erg
E
s
t
G
BB
Particle Acceleration
Giannios & Spitkosky (2009)
turbulent acceleration (Honda 2005)
sc
U
cm
L
G
B
MeV
Etacc
1110
26
212 )1.0
()100.1
()102.1
()(104.1
sG
Btcool
26
14
8 )102.1
()108.1
(100.3
eVc
U
cm
LE )
1.0()
100.1()
108.1(107.4 2/1
102/1
414
4106.3/ epe mm
Maximum Acceleration
Stochastic acceleration Virtanen & Vainio (2005)
acceleration in random and small scale B field might be very effective
Mizuno et al. numerical simulation
122max 101.1/ mckeB
Preliminary Results
Random & small scale B generated by turbulence
Jitter spectrum index determined by turbulent spectrum: results consistent with BASTE & Fermi
Acceleration is effective
Sironi, Nishikawa, numerical simulation
Small-Scale Turbulent Dynamo
Scale problem: sub-Larmor radius validation ?
B generation? Particle acceleration? Particle energy distribution? ……