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Transient NS X-ray binaries with Simbol-X Sergio Campana Osservatorio astronomico di Brera [email protected] t Bologna, May 2007

T ransient NS X -ray binaries with S imbol- X

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T ransient NS X -ray binaries with S imbol- X. Sergio Campana Osservatorio astronomico di Brera [email protected]. Bologna, May 2007. Outline. A brief history: what we discovered and what we know now, focusing of hard X-ray emission The future: Simbol-X. - PowerPoint PPT Presentation

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Page 1: T ransient  NS X -ray binaries                   with  S imbol- X

Transient NS X-ray binaries with

Simbol-X

Sergio Campana Osservatorio astronomico

di [email protected]

.itBologna, May 2007

Page 2: T ransient  NS X -ray binaries                   with  S imbol- X

Outline

RXTE/ASM light curve

A brief history: what we discovered and what we know now, focusing of hard X-ray emission

The future: Simbol-X

Page 3: T ransient  NS X -ray binaries                   with  S imbol- X

X-ray binaries: variable

Page 4: T ransient  NS X -ray binaries                   with  S imbol- X

State transitions: SIGMA

Barret & Vedrenne 1994

Limiting luminosity for all LMXRBs (NS+BH) at 4x1036 erg/s

Maccarone 2003

Page 5: T ransient  NS X -ray binaries                   with  S imbol- X

Campana et al. 1998

Hard tails: INTEGRAL

Tarana et al. 2007

4U 1820-30

Paizis et al. 2006

Page 6: T ransient  NS X -ray binaries                   with  S imbol- X

BH XRB

NS XRB

Homan et al. 2007

State transitions: jets

Belloni 2007

Page 7: T ransient  NS X -ray binaries                   with  S imbol- X

Campana et al. 1998 Di Salvo et al. 2000

Farinelli et al. 2007

Occasional detection of very hard tails (BMC)

GX 17+2

Very hard tails: PDS/XTE

Page 8: T ransient  NS X -ray binaries                   with  S imbol- X

From outburst to quiescence

FAST !

e-folding time changing from ~20 d to ~1 d at transition

BeppoSAX data

Campana et al. 1998

Page 9: T ransient  NS X -ray binaries                   with  S imbol- X

NS transients in quiescence

Canonical spectrum: Soft component (NS atmosphere, kT~0.1-0.3 keV; ≥50% of the flux)

Hard component (Power law, photon index ~1-2; ≤50% of the flux)

ExN

(E)

ExN

(E)

Lx=1032-1033 erg/s

Page 10: T ransient  NS X -ray binaries                   with  S imbol- X

NS transients in quiescence: variability

Campana et al. 2003 Rutledge et al. 2001Campana &Stella 2004

Aql X-1

Page 11: T ransient  NS X -ray binaries                   with  S imbol- X

Transient X-ray pulsars

Campana et al. 2007

Wijnands 2005

SAX J1808.4-3658

mcr

ab

Page 12: T ransient  NS X -ray binaries                   with  S imbol- X

SAX J1808.4-3658 in quiescence

NS atmosphere model can account less than 10% of

the total flux and it is not required by the fit

XMM-Newton data

Campana et al. 2002

Heinke et al. 2007

Page 13: T ransient  NS X -ray binaries                   with  S imbol- X

Simbol-X strenghts (for XRBs)

• Broad-band capabilities (0.5-80 keV)

• Large effective area at low and high energies

• Good timing capabilities

• Focusing instrument and thus low background

(e.g. wrt RXTE)

Page 14: T ransient  NS X -ray binaries                   with  S imbol- X

Simbol-X: atoll spectrum

kTC

100 ks

Fx=10-9 erg/s/cm2

Lx=4x1036 erg/s @ 5 kpc

Monitoring of parameters

variations: study the physics

Page 15: T ransient  NS X -ray binaries                   with  S imbol- X

Simbol-X: very hard tails

kTc=5 keV 40 ks

Tau=3

CONT: Fx=2x10-9 erg/s/cm2

TAIL: Fx=6x10-12 erg/s/cm2

Tail/Cont(0.5-20)= 0.1%

Page 16: T ransient  NS X -ray binaries                   with  S imbol- X

NS transient in quiescence

100 ks

Diagnostic of the

power law tail and of

its variability

Page 17: T ransient  NS X -ray binaries                   with  S imbol- X

SAX J1808.4-3658 in quiescence

100 ks

XMM

Page 18: T ransient  NS X -ray binaries                   with  S imbol- X

Summary

Different mechanisms for explaining the transition to and the quiescent emission of NS XRTs approach the problem from the point of view of physics

Simbol-X is the first observatory able to disclose the high energy part of the spectrum at very high S/N and for persistent and transient sources, making possible a thorough study of the emission mechanisms through monitoring the variability