the structure of the pulsar magnetosphere via particle simulation shinpei shibata (1), shinya yuki...
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The structure of the pulsar magnetosphere via particle simulation
Shinpei Shibata (1), Shinya Yuki (1), Tohohide Wada (2),Mituhiro Umizaki (1)
(1)Department of Phys. Yamagata University(2)National Astronomical Obvsevatory of Japan
Introduction
Pulsars
Neutron Starabout 1M_sun10km in size
Pulsars:B_d ~ 10^9 – 10^13GP ~ 1.5msec – several seconds
Emf ~ 10^14 Volt rotation powered pulsars
Magnetars: Small subclass of magnetic neutron starsmagnetic active regions with B ~ (maybe)10^15G
Emf ~ 10^14 Volt magnetic powered pulsars
Rotation axis
PulsarWind(relativisticoutflow ofmagnetizedplasmaγ ~ 10^6)
Size of the magnetosphere: c/Ω ~ 4.8×10^4 R_ns
1 ly
Beamed radiationObserved as pulsed radiation
SED(spectral energy density plot)
magnetospheric
Nebula
2. Pulsar Wind Lwind=ηw Lrot
Aharonian, F.A. & Atoyan, A.M., 1998
Unpulsed emission
Pulsed emission
E// + e/p
BB 加熱
E // 加速
IC
sync
RL=c/Ω
Rs=(Lwind/4πPext)^1/2
Vacc=RL*BL=μΩ^2/c^2
Vacc=Rs*Bn with Pext=Bn^2/8π
keVGeV
TeV
垂直衝撃波加速の困難
1. High Energy Pulses1. High Energy Pulses3. Radio Pulses
E// (field-aligned acceleration)
Roation × magnetizationmakes emf charge separation
Unipolar Inductor
E ⊥
If pair creation is suppressed, charged particles are emitted from the neutron star and forms steady clouds.
• Particle Simulation for the screening. (ref. Wada and Shibata 2003)
gap
The gap is unstable against pair creation.
1. EMF and charge separation
Unipolar Induction
Basic properties of the pulsar magnetosphere
Motional field
As compared with required charge separation, plasma source is limited gap E//
Goldreich-Julian model (1969)
In reality, plasma is extracted from the stellar surface by E//: maybe, complete charge separation
Positive space charge
Negative space charge
Corotation speed becomes the light speed
Relativistic
centrifugal wind
Goldreich-Julian model (1969)
Strong charge separation in a rotating magnetosphere makes the gap, non-zero E//
Positive space charge
Negative space charge Null c
harge surfa
ce
Gap formation
Ω B
Dead zone
Null面
Light cylinder
Polar cap
Slot gap
Outer gap
Models based on observatons: PC, SG, OG
Closed field(dead zone)
Open field region
Ω B
Dead zone
Null面
Light cylinder
Polar cap
Slot gap
Outer gapClosed field
(dead zone)
Open field region
γ-ray pulse shape and relation to radio pulses are well explained if γ from OG and radio from PC
Two-pole caustic (TPC) geometry (Dyks & Rudak, 2003)
Radio pulse
Models based on observatons: PC, SG, OG
Particle simulation
part
icle
code
―
acceleration
Gamma-ray―
―
radiation from the starStrong B
Particle codeParticle motion and the electromagnetic fields are solved iteratively for the axis-symmetric steady solution.
Emf is included in the BC
For the EM field
For the particle motion
• Gravitational interaction
• For the electric field • For the magnetic field
We use Grape-6, the special purpose computer for astornonomical N-body problem at NAOJ.
- Particles are emitted from the star if there is E// on the surface.
- On the spot approximation: e+/e- are created if E//>Ec
- Particles are removed through the outer boundary: loss by the puslar wind.
The system settles in a steady state when the system charge becomes constant:seteadily pairs are created in the magnetoschpere and lossed as the wind.
Particle creation and loss
Result
Modificaton of the magnetic field
Light cylinder
Outer gap
The outer gaps steadily create pairs.Gap electric fileld is kept above Ec as to create pairs.
Particle distribution and motion Strength of E//
Pair creation
Not so strong: limitation of particle number
Pola
r cap
current circulation seen
Slot
gap
Outer gap
Outward current
Retun current
Current-neutral dead zone
Dead zone
Light cylinder E/B map
E>BBread down of the ideal-MHD cond.
磁気リコネクション
Summary and Discussion1. The outer gap, which is the candidate place of
the particle acceleration and gamma-ray emission, is proven from the first principles by particle simulation.
2. Due to radiation reaction force, some particles escape through the closed field lines.
3. At the top of the dead zone, we find strong E field larger than B, i.e., break down of the ideal-MHD condition, and in addition PIC simulation indicates possibility of reconnection driven by the centrifugal force.
There are two places in which magnetic reconnection may play an important role.-Close-open boundary near the light cylinder-Termination shock of the pulsar wind
Ω
Magnetic axis
Thick windNeutral sheet
Magnetic reconnection
パルサーオーロラ
Rotation axis
Lig
ht
cylin
der
Outer gap
Polar cap
Slot gap
SED(spectral energy density plot)
magnetospheric
Nebula
2. Pulsar Wind Lwind=ηw Lrot
Aharonian, F.A. & Atoyan, A.M., 1998
Unpulsed emission
Pulsed emission
E// + e/p
BB 加熱
E // 加速
IC
sync
RL=c/Ω
Rs=(Lwind/4πPext)^1/2
Vacc=RL*BL=μΩ^2/c^2
Vacc=Rs*Bn with Pext=Bn^2/8π
keVGeV
TeV
垂直衝撃波加速の困難
1. High Energy Pulses1. High Energy Pulses3. Radio Pulses