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Coherent Emission Mechanisms

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'The whistle on the locomotive' 'We only need to know why pulsars pulse, not how they shine' ... Related to studies of powerful g-ray emission. Important ... – PowerPoint PPT presentation

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Title: Coherent Emission Mechanisms


1
Coherent Emission Mechanisms
  • Roger Blandford
  • KIPAC
  • Stanford

2
Why do we care?
  • The whistle on the locomotive
  • We only need to know why pulsars pulse, not how
    they shine
  • Alternatively,
  • Related to studies of powerful g-ray emission
  • Important sometimes when pulsars are tools
  • Accurate timing eg geodetic precession
  • Scintillation experiments
  • Best laboratory for relativistic plasma physics
  • New light sources
  • Microwave generators
  • Genuinely interesting physics and very good data!

3
Radio Pulses
  • Core cone structure (Rankin)
  • Open flux boundary layer/slot gap/return current
  • Linear, circular polarization swings
  • Propagation, orthogonal mode transitions
  • Millistructure
  • Subpulse drift
  • Microstructure
  • TB 1030 K
  • Nanostructure
  • dn 0.1n
  • Location?
  • H500km in Vela?

4
Magnetosphere
  • GJ density shorts out E
  • Must replenish charge on open flux tube also
    closed flux!
  • Polar gap (Sturrock, Ruderman Sutherland)
  • TeV primary positrons create curvature g-rays if
    W.Bgt0
  • Create 100MeV pairs on field
  • n104 nGJ?? - Wind need much more plasma?
  • Anti-pulsars? Ions?
  • Outer gap/slot gap? (Holloway, Arons)
  • Currents and charges modify magnetosphere
  • TeVltltPeV so force-free probably OK (Spitkovsky)
  • Differential rotation along field?
  • Streaming may be necessary to dissipate
  • Primary beam? j2-r2gt0?, reverse current?

5
General emission mechanisms(cf Goldreich, Pacini
Rees 1972, 1973)
  • Antenna mechanisms
  • Bunched curvature radiation ng3c/R, kTBltNgmc2
  • Lateral coherence?? Frequency structure?
    (Melrose)
  • Orthogonal polarization?
  • Radiation reaction instability? (Goldreich
    Keeley)
  • Plasma turbulence
  • Electrostatic turbulence, solitons, nltltnGJ?
  • Simulations (Weatherall)
  • Attenuation, conversion to EM mode?
  • Maser mechanisms

6
(Anomalous) Cyclotron Resonance
  • Strong absorption in outer magnetosphere?
  • Cooling length 0.1 g B12-2 m gtground state
  • En ( m2c4 pz2c2 2 h ?Gmc2)1/2
  • s2p2recd(w-wG)
  • Anomalous Cyclotron Resonance
  • Kazbegi, Machabeli, Melikhidze Lyutikov
  • ????kz vz - s?G / ?
  • Let n ck/??gt1
  • Can get stimulated emission out of ground state
    if enough parallel momentum is lost by particle
  • Kinetic instability for primary electrons (if
    survive)
  • cf cosmic ray streaming instability

7
Particle distribution function
10
107
104
  • Requires specific distribution function
  • and location
  • O, X-modes excited in outer
  • magnetosphere only
  • Linearly polarized
  • A-modes excited somewhat closer to
  • star but have to mode-convert

Dispersion relation in cold pair plasma
8
Cerenkov Drift Instability
  • Beam/tail particles have curvature drift
  • ud g c2 /wG R
  • ????kz vz kx ud
  • Hydrodynamical instability involving bulk plasma
  • Orthogonal polarization to Rotating Vector Model
  • Outer magnetosphere
  • Saturation
  • Quasilinear diffusion
  • Stimulated Raman, Induced
  • Compton scatttering
  • Machabeli, Melikhidze Lyutikov

9
Emission Sites
10
Phenomenology
  • ACR, CDI gt core, cone (Lyuitkov et al)
  • Only in the outer magnetosphere r n-1/6
  • Not for MSP, young pulsars?
  • Frequency structure, CDI orthogonal polarization

Hankins
11
Challenges
  • Use multi-wavelength studies to describe
    magnetospheric anatomy
  • Locate radio emission cite
  • MSPs rLC 7RNS!
  • Giant pulses (ms), RRATS
  • Global magnetospheric simulations
  • Study and simulate nanostructure
  • Individual emitting elements (c1ft/ns!)
  • High energy density physics experiments
  • New light sources can make pair plasmas scaled
    experiments
  • Relativistic plasma simulations
  • Major challenge to capture dynamic range
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