relativistic particle acceleration in a developing turbulence
DESCRIPTION
Relativistic Particle Acceleration in a Developing Turbulence. Shuichi M ATSUKIYO ESST Kyushu Univ. Collaborator : T. Hada. Outline . Background -- motivation -- acceleration processes in turbulent plasmas -- parametric instability (PI) - PowerPoint PPT PresentationTRANSCRIPT
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Relativistic Particle Acceleration
in a Developing Turbulence
Shuichi MATSUKIYO ESST Kyushu Univ.
Collaborator : T. Hada
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Outline Background -- motivation -- acceleration processes in turbulent
plasmas -- parametric instability (PI) 1D PIC simulation on PIs in a pair plasma Acceleration mechanism : modelling Test particle simulation Summary
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ScholerSN1006Bamba et al. [2003]
Alfven turbulence & particle accelerationBest-known acceleration process in astrophysics : Fermi accelerations1st order Fermi acc. (DSA) 2nd order Fermi acc.
v||
v^
v+v-
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SN1006Bamba et al. [2003]
Alfven turbulence & particle acceleration
● Standard Fermi processes take into account wave-particle interactions in ‘fully-developed’ turbulence.Turbulence observed in space plasma is often coherent and time dependent.
●
Scales of a relaxation process may be rather large !
Best-known acceleration process in astrophysics : Fermi accelerations
How is a particle acceleration process in ‘developing’ turbulence ?
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Parametric decays of large amplitude Alfven waves
w
k
Alfven
acousticP
D1D2
D3
decay inst.
Resonance conditions :wp + w1 = w2,3
kp + k1 = k2,3
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1D PIC sim. on parametric inst. in a pair plasma
x (|| B0)
k
^ )cos()sin(
tkxtkx
Bww
B
RH circularly polarized parent Alfven wave :
3220
2
00
106.1,10
632.0,1
mcT
BB
pw
w
P
Amplitude spectrum of B
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1D PIC sim. on parametric inst. in a pair plasma
Electron energy & momentum dist.
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Acceleration mechanism
trapping by a sharp envelopetrough
tt
kxBkc
tt
kxB
w
w
www
ww
sincos
sin
sincos
cos
w
w
E
B
(w,k)
(w,-k)
Assumption: Two waves with opposite signs of k (same w) locally become dominant.
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Motion of an electron
^
^
^
w
w
w
0||
||
||
||
coscossinsin
sincoscossin
sincos
kxu
kxkcu
kxu
kxkc
u
ucx
kxu
u
w
w
w
cmeB
cmeB
t
cuuu
ww
00
00
||
,,
,sin,cos,
^^
w
vuuwherefixed point
Assumption: u|| , x = const. u||^ = p||^ / m0c
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Trajectory in u^ - space
Nonresonant trapping• Finite amp. is necessary.• Also seen in nonrelativistic limit.
Relativistic trapping• In small amp. limit:
w ~ 0 /
u||
u^
ures- ures+
22||
0||||
1
0
^
uu
vk
w
NR NR
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Trajectory in u^ - space
^
^
^
w
w
w
0||
||
||
||
coscossinsin
sincoscossin
sincos
kxu
kxkcu
kxu
kxkc
u
ucx
kxu
u
w
w
w
2
0max
^ kc
u w
w
Max. u^
65.0,11.0,1
0
00
kcw w
1.18^u
Comparison with sim.
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0t
kc/
0
Log|Bz R/B
0 |
Preferential acc. of high energy particles
0t
e
Time variation ofelectron energy
t
w (k)0/
w 0~ resonance cond.
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Wave amp. spectrum at 0t = 1616
kc/0
|B(k
)|/B
0 -2.0
How essential in particle acc. is the relativistic effects ?
- a
±kK0=0.1 3.0
Bw(k)1
k
w
-3 3
3
3 0
0
0cossin
kc kph
kphw
tvxktvxk
Kk
Bb
awB
Test particle simulation
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Test particle simulation
Non-rel. & Rel. eqs. of motion for 105 particles Initial distribution function: isotropic ring with v^/c = 0.1
Non-relativistic case
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Test particle simulation
Non-rel. & Rel. eqs. of motion for 105 particles Initial distribution function: isotropic ring with v^/c = 0.1
Relativistic case
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Summary
Local sharp envelope troughs of magnetic fields Relativistic perp. acceleration of particles trapped
in the envelope troughs Preferential acceleration of high energy particles
Particle acceleration process through coherent Alfven waves in the course of parametric decay instabilities :1D PIC simulation
Model analysis & test particle simulation Motion of a particle in two oppositely propagating
waves Relativistic resonance with the two waves Maximum attainable energy consistent with the PIC
simulation Test particle simulation reproduced power-law like tail
when the time varying wave spectrum is assumed.