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Particle Acceleration in Kinetic Plasma Processes

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Title: Particle Acceleration in Kinetic Plasma Processes


1
Particle Acceleration in Kinetic Plasma Processes
  • Masahiro HOSHINO
  • University of Tokyo

Collaboration with S. Zenitani, K. Nagata, C.
Jaroschek
2
Cosmic Ray Accelerator
  • Relativistic Shock and Reconnection in
    Astrophysics
  • Pulsars Winds (g 106-7)
  • Extragalactic radio source (g 10)
  • Gamma ray bursts (g gt 100)
  • Sources for UHE CR?

3
Open Issues in Particle Acceleration
  • Structure of Collisionless Shock Reconnection
  • Acceleration Mechanisms
  • Fermi acceleration (slow process)
  • Injection Problem Particles need
    pre-acceleration to leave the thermal pool and
    enter Fermi acceleration engine.This mechanism
    remains unknown.
  • Acceleration Efficiency How large fraction of
    the accelerated particles?
  • This fraction remains unknown.
  • Something else in kinetic plasma process
  • (fast process) ?
  • There are many possible mechanisms, but they
    remains unknown.
  • Efficiency of Nonthermal Particles

4
Shock Numerical Experiment
Modeling on Collisionless Shock
Particle-in-Cell (PIC) Simulation
Bz
z
Ey
wall
y
e,e-
x
injection
reflection
108 particles
5
Shock Heating for s0.1
shock front
injection
relativistic Maxwellian
wall
upstream
downstream
EM waves are strong No nonthermal Acceleration
Langdon et al. PRL 1988, Gallant et al. ApJ 1992
6
How are nonthermal particles generated?
  • (1) Low s Shock with Surfing Acceleration,
  • (2) Pair plasmas ion Shock,
  • (3) Striped Wind Shock.

7
Shock Acceleration for s10-4
relativistic Maxwellian
injection
shock front
wall
upstream
downstream
nonthermal particles
  • EM waves are very strong
  • Strong Acceleration occurs at the shock front

8
s dependence
s10-1
s10-2
s10-4
s10-3
Nonthermal
slt 10-3 ? strong non-thermal acceleration s
10-2 ? marginal
9
Shock Surfing Acceleration
z
Sagdeev and Shapiro (1973), Katsouleas and
Dawson (1983)
y
Bz
Ey
? charge
Current Sheet Shock Surfing
? charged particles
?
Near the Shock Front
x
? -charge
shock surface
This can provide unlimited acceleration
Hoshino PTP 2001, Nagata 2005
10
Weibel Instability in 3D Shocks
  • Magnetic Fields by Weibel Instability

Weibel 1959
Hededal et al. ApJ 2004
11
Perpendicular shock
Parallel shock
upstream
upstream
downstream
downstream
magnetic field
magnetic field
Fermi acceleration
Surfing acceleration, ..
12
Surfing Acceleration with Turbulent Fields
Kolmogolov Turbulence Test Particle
Simulation
This Talk
Electrostatic Potential (particle trapping
force)
Trajectory around Shock
Niemiec and Ostrowski, ApJ 2004
13
Fermi Surfing Accelerationin Oblique Shock
Fermi
Fermi Surfing
along shock
N(cos q)
N(cos q)
cos j
cos j
14
How are nonthermal particles generated?
  • (1) Low s Shock with Surfing Acceleration,
  • (2) Pair plasmas ion Shock,
  • (3) Striped Wind Shock.

15
Composition pair ion plasmas
(Upstream) Kinetic energy of p dominates
(Downstream) Strong turbulence by p
synchrotron maser inst.? energy transfer to e
shock front
Ion synchrotron maser instability
Hoshino et al. ApJ 1992
16
Efficiency of pairion Shock
Nonthermal Efficiency
Power-Law Index
17
How are nonthermal particles generated?
  • (1) Low s Shock with Surfing Acceleration,
  • (2) Pair plasmas ion Shock,
  • (3) Striped Wind Shock.

18
Striped Wind
neutron star
Equatorial plane
Meridional plane
equator
Coroniti, ApJ 1990 Kirk et al. PRL 2003
rotation axis
magnetic axis
19
1D Relativistic Shock Simulation
Vx
Vx,ele
Vy
Shock-Current Sheet Interaction
Vy,ele
Energy
Eele
Ey
Ey/E0
Current Sheet
s1 ?10
Bz
Bz/B0
Upstream
Downstream
X
20
Bz
BEFORE
TD (Current Sheet)
FS (Shock)
upstream
downstream
X
Bz
AFTER
upstream
downstream
X
TD (Current Sheet)
FS (Shock)
21
Bz
BEFORE
TD (Current Sheet)
FS (Shock)
upstream
downstream
X
FW (Magnetosonic Wave)
Bz
AFTER
upstream
downstream
Thick CS
X
TD (Current Sheet)
FS (Shock)
22
Multi-Current Sheet Interaction with Shock
Vx,ele
Vx,ele
Vy,ele
Vy,ele
Multi-current sheets
Bz/B0
nonthermal particles
Bz/B0
Ey/E0
Ey/E0
Upstream
Downstream
23
How are nonthermal particles generated?
  • (1) Low s Shock with Surfing Acceleration,
  • (2) Pair plasmas ion Shock,
  • (3) Striped Wind Shock,
  • (4) Magnetic Reconnection

24
Flares
Magnetic Reconnection
Solar Stellar Flares, Magnetosphere, Accretion
Disks, Pulsar Wind-Nebula,
YOHKOH, SOHO, Trace, RHESSI
25
Relativistic Magnetic Reconnection(Particle-in-Ce
ll simulation)
Zenitani Hoshino, ApJ 2001
26
Nonthermal Acceleration in MRX
Jaroschek et al. ApJ 2004
27
Power-Law Spectrum in Reconnection
  • Acceleration rate
  • Loss rate
  • Energy Spectrum

28
3D Reconnection with Guide Field
t/tc 160
t/tc 160
t/tc 200
t/tc 200
Zenitani Hoshino, PRL 2005
29
Summary
Direct Acceleration
  • Surfing Acceleration (low s),
  • Pair Ion Shock/Synchrotron Inst. (low s),
  • Surfing Fermi Acceleration (low s),
  • Striped Wind Shock (medium s),
  • Reconnection (high s).

30
Acceleration Mechanisms
31
Acceleration Mechanisms
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