Observations of particle acceleration in the blast waves of GRB - - PowerPoint PPT Presentation

observations of particle acceleration in the blast waves
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Observations of particle acceleration in the blast waves of GRB - - PowerPoint PPT Presentation

Observations of particle acceleration in the blast waves of GRB afterglows Peter A. Curran with Phil Evans, Alexander van der Horst, Rhaana Starling, Mat Page Laboratoire AIM, Irfu /Service d'Astrophysique CEA Saclay, France GRB afterglows


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Observations of particle acceleration in the blast waves

  • f GRB afterglows

with Phil Evans, Alexander van der Horst, Rhaana Starling, Mat Page

Peter A. Curran

Laboratoire AIM, Irfu /Service d'Astrophysique CEA Saclay, France

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GRB afterglows

(Piran 2003)

External shocks: X-ray, optical, radio

Electrons are accelerated by shock… emit synchrotron radiation

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GRB Synchrotron spectra

(Sari et al. 1998)

Optical X-ray Electrons are accelerated by shock… emit synchrotron radiation (Slow cooling, adiabatic expansion) Cooling break freq.

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Electron energy distribution

N(E) ∝ E-p

Fermi acceleration of electrons

Number of electrons with Energy, E Energy, E

Electrons are accelerated by shock… to a certain distribution (value of p dependent on the underlying plasma physics)

p – electron energy distribution index

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Fermi acceleration of electrons

Single, discrete value of p? Or a distribution? What distribution? How does measured value compare to theory/ simulations? Universal value or variation between sources*?

* GRB (p~2-3), Cosmic Rays (p≈2.5-2.7), X-ray binaries (p≈2.6, σ≈0.4), AGN (p~3)

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X-ray spectra ➝ p(βX,NH) ⇒ multiple options ⇒ synchrotron cooling frequency above/below

Derivation of p

Compare predictions of p to light curves (optical & X-ray: small sample) to decide which value of p is correct

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Distribution of p

BeppoSAX & Swift (16 GRBs)

(Starling et al. 2008; Curran et al. 2009)

Not consistent with single, discrete value

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Cooling frequency: (free parameter) > X-ray < X-ray

0.5

Transform p to β

Probability distributions

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(data from Evans et al. 2009)

X-ray spectral index, βX

Swift X-ray Telescope (XRT) (~300 bursts)

i) Assume underlying p distribution ii) Find most-likely parameters iii) Test hypothesis (via Monte Carlo)

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Monte Carlo hypothesis test

~105 synthetic data sets

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Distribution of spectral index, βX

Swift XRT (~300 bursts)

(Curran et al. 2010)

Single discrete value of p?

synthetic data

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Distribution of spectral index, βX

Swift XRT (~300 bursts) Not consistent with single, discrete value

(Curran et al. 2010)

synthetic data

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Distribution of spectral index, βX

Swift XRT (~300 bursts)

(Curran et al. 2010)

Gaussian distribution of p? (p=2.39, σ=0.6)

synthetic data

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Distribution of spectral index, βX

Swift XRT (~300 bursts) Consistent with a Gaussian distribution p=2.39, σ=0.6

(Curran et al. 2010)

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X-ray spectra ➝ p(βX,NH) ⇒ multiple options X-ray light curves ➝ p(indices, density structure, accretion) & accuracy of fit, model dependent ⇒ multiple options

Distribution of p via temporal indices

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(Evans et al. in preparation, using model of Van Eerten & Wijers 2009)

Distribution of p via temporal indices

Preliminary (~180 bursts)

p≈2.36, σ≈0.36

Totally independent method, with different data!

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Fermi acceleration of electrons

Electron energy distribution

Number of electrons with Energy, E Energy, E

Q: Single value of p? Distribution of p? What distribution? A: Gaussian distribution at p=2.39 and standard deviation, σ=0.6

N(E) ∝ E-p

Q: Single value of p? Distribution of p? What distribution? A: Gaussian distribution at p=2.39 and standard deviation, σ=0.6

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Only 1 spectral peak?

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Only 1 spectral peak?

Swift XRT (~300 bursts)

?

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(Curran et al. submitted)

~94%: cooling frequency below

>94% with cooling frequency < X-ray ≤6% with cooling frequency > X-ray

3σ limit

Fraction of GRBs with νc < X-ray Number of trials

Only 1 spectral peak?

94% 6%

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Other explanations?

 Bimodal distribution of p, with mode of p drawn from correlated with position of cooling break? Highly convoluted!  Wide distribution blurs out double peaks? Requires distribution far wider than observed  Not 2 βX(p) relationships?

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Synchrotron spectra?

Smoothly broken curves ⇒ continuous range of relationships

(Granot & Sari 2002)

Breaks evolve in time ⇒ spectral & temporal changes (inconsistent with observations)

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Other explanations?

 Bimodal distribution of p, with mode of p drawn from correlated with position of cooling break? Highly convoluted!  Wide distribution blurs out double peaks? Requires distribution far wider than observed  Not 2 βX(p) relationships? Inconsistent with observations

No, majority of GRBs have cooling frequency below the X-rays

  • supported by preliminary Evans results
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Conclusions

 Fermi acceleration can be ‘observed’ in GRBs, and parameters constrained via statistical methods  Allows for comparison with other sources, as well as theory/simulations  not consistent with a single, discrete value of p  consistent with Gaussian of p≈2.4, σ≈0.6*  94% of GRBs have cooling frequency below the X-rays

* Compared to Cosmic Rays (p≈2.5-2.7), X-ray binaries (p≈2.6, σ≈0.4), AGN (p~3)