The modeling of the Vela pulsar pulses - - from op5cal to hard - - PowerPoint PPT Presentation

the modeling of the vela pulsar pulses
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The modeling of the Vela pulsar pulses - - from op5cal to hard - - PowerPoint PPT Presentation

The modeling of the Vela pulsar pulses - - from op5cal to hard gamma-rays Bronek Rudak in collabora5on with J. Dyks Nicolaus Copernicus Astronomical Center (CAMK) Poland ICRC 2017, Busan, Korea In the talk 1) 3D Outer-Gap model of


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The modeling of the Vela pulsar pulses -

  • from op5cal to hard gamma-rays

Bronek Rudak

in collabora5on with J. Dyks Nicolaus Copernicus Astronomical Center (CAMK) Poland

ICRC 2017, Busan, Korea

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In the talk

1) 3D Outer-Gap model of Very-High-Energy emission expected from Vela-like pulsars: − the origin of the VHE component, − its temporal (pulses) and spectral proper5es. 2) A case for coexistence of the outer gap and an inner gap in the magnetosphere of the Vela pulsar: − the forma5on of core-like pulses in op5cal, UV and in hard X-rays, aligned in phase with the core-like radio pulse (as observed)

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CTA ?

The many faces of the Vela pulsar

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Picture from Benoit CeruW

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Outer gap: primary pairs with ϒ > 107, curvature photons in gamma

Not to scale drawing

Secondary pairs layer: ϒ ~ 100 – 1000, synchrotron photons in op5cal-IR

Hot surface, TBB = 106 K

μB

Inner-Gap pairs, ϒ ~ 100 - 1000 Core emission in coherent radio

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  • 1. Primary OG pairs + op5cal-IR photons

(synchrotron photons)

  • 2. Inner Gap pairs + op5cal-IR photons

(synchrotron photons)

  • 3. Inner Gap pairs + thermal X-ray photons

Processes Results

pulsed VHE component pulsed core op5cal comp. pulsed core hard X-rays comp.

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The first step: determine α − inclina5on angle (between Ω and μ ) and ζ − viewing angle (between Ω and kobserver ) by reconstruc5ng simultaneously the shapes and phases of the observed main peaks in op5cal and gamma using the „geometrical” version of the OG model. The next step: use α and ζ in the physical OG model.

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Gouiffes 1998 Abdo+ 2010

Two main pulses from Vela in op5cal and gamma rays and their reconstruc5on in a uniform-emissivity version of the OG model,

  • btained for

inclina5on angle α = 70o, viewing angle ζ = 79o

P1 P2 P1 P2 P3

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The OG model - ICS component in VHE α = 70o

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CTA South 50h

Phase-averaged gamma-ray SED in OG model of Vela

Curvature radia5on component ICS component: con5nuous – sok photon field

  • p5cal to far-IR

dashed – sok photon field

  • p5cal to near-IR

α = 70o, ζ = 79o

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  • 1.0 -0.5 0.0 0.5 1.0

α = 70o The ICS core component in op5cal-UV

P3

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The ICS core component in hard X-rays α = 70o

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Summary

1) The VHE domain

− Forma5on of pulsed VHE-spectral component is possible in the Vela pulsar in the case of high inclina5on angle, − its lightcurve consists of two pulses at phases ~0.2 and ~0.6, − its expected phase-averaged flux may be of interest to CTA South (for > 50h).

2) The opFcal-UV and the hard X-rays domains

If an inner gap with e--e+ pairs coexists with outer gaps, then

− core-like pulses can form in op5cal, UV and hard X-rays, − they are in phase with the core-like radio pulse (as observed in Vela).

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Back-up slides

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The OG model - Curvature Radia5on component at HE α = 70o