Magnetars in the Fermi Era On behalf of the Fermi/GBM Magnetar Team C. Kouveliotou (PI, NASA/MSFC) E. Gogus, Y. Kaneko (Sabanci University, Turkey) E.

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Presentation transcript:

Magnetars in the Fermi Era On behalf of the Fermi/GBM Magnetar Team C. Kouveliotou (PI, NASA/MSFC) E. Gogus, Y. Kaneko (Sabanci University, Turkey) E. Ramirez-Ruiz (UCSC, USA) J. Granot (University of Hertfordshire, UK) P. Woods (Dynetics, USA) A. von Kienlin (MPE, Germany) A. van der Horst (NPP, USA) A. Watts, M. van der Klis, L. Kaper (U. of Amsterdam, The Netherlands) M. Finger (USRA, USA) C. Wilson-Hodge (NASA/MSFC, USA) V. Connaughton (UAHuntsville, USA) A. Pe’er (STScI, USA) J. McEnery, N. Gehrels (NASA/GSFC, USA) S. Wachter (Caltech/IPAC, USA) V. Kaspi (McGill University, Canada)

Magnetars are magnetically powered neutron stars ~16 are discovered to date – two in the last year ( ) – Only 2 extragalactic sources Discovered in X/  -rays; radio, optical and IR observations: Short, soft repeated bursts P = [2-11] s, P ~[ ]s/s τ spindown (P/2 P) = k yrs B~[1-10]x10 14 G (mean surface dipole field: 3.2x10 19 √PP ) Bright sources, L~10 33–36 erg/s, >> rotational E-loss No evidence for binarity so far (fallback disks?) SNe associations?...

Neutron star populations which may comprise Magnetars: Soft Gamma Repeaters (SGRs) Anomalous X-ray Pulsars (AXPs) Dim Isolated Neutron Stars (DINs) Compact Central X-ray Objects (CCOs)

MAGNETARS AGE: 0-10 s 0-10,000 years above 10,000 years AGE: 0-10 s 0-10 million years above 10 million yrs RADIO PULSARS Ordinary Star (8-20 M ʘ ) Neuborn Neutron star Kouveliotou, Duncan & Thompson, Scientific American

Gavriil et al 2008 PSR J1846−0258 / Kes 75 Magnetar-like X-ray bursts were detected from the young pulsar PSR J1846−0258. Rotation-powered PSR with an inferred surface dipolar magnetic field of 4.9×10 13 G, P s =0.3 s, Age ~ 900 yrs Bursts accompanied by a sudden flux increase (200L x ) and unprecedented change in timing behavior (spin up->spin down). Is there a continuum of magnetic activity that increases with inferred magnetic field strength?

PSR J1846−0258

: A good year for Magnetars! Swift Fermi RXTE IP N

SGR Swift triggered on 4 bursts on 22 August 2008 RXTE ToO program triggered ~4 hours after the first Swift trigger for 600 s P = 5.769s ± s was reported ~ 9 hours after the first Swift trigger! P = 1.5 x s/s and B = 3 x G CXO HRC location: RA = 05h 01m s DEC = +45d 16m 33.92s (0.1” error) IR Counterpart with UKIRT, K~18.6 (Tanvir & Varricatt 2008) GBM triggered on 26 events from the source – total of 56 events in ~ 3.5 days.

1 st Outburst of SGR in July 1993! CGRO/BATSE

1 st Outburst of SGR

Gaensler & Chatterjee 2008 SNR HB9/G (1.4 GHz) Angular separation from the SNR center ~80 arcmin => projected space velocity = 1700km/s (for a distance to the SNR of 1.5 kpc and an age of 8000 years; Leahy & Aschenbach, 1995 ) SGR

Rea et al XMM-Newton observations ~40 Swift observations 1 Suzaku observation 2 INTEGRAL observations XMM August 23 rd 2008 Flux decay with time: F(t)= x exp-(t/23.81) Pure exponential for the first 160 days

Persistent Emission: Rapid Spectral Variations 87 hours of bursting activity Source cools while bursting ? Gogus et al. 2010

P = /- 1.66x s P = x /- 2.51x s/s B field = 2.1x10 14 G. Rea et al P = (1) s P = 6.77(8) × 10 −12 s s −1 P= 1.9(4) × 10 −19 s s −2  decreasing spin-down Consistent with a post-glitch (not observed!) recovery time of ~1yr... Gogus et al 2010

Pulsed Emission: Pulsed Fraction Variations Gogus et al. 2010

SGR : Evolution of pulse profile with energy RXTE/PCA ~40 days average Swift/XRT Gogus et al 2010

Suzaku data for _136: Integrated spectrum best fit by 2 BB: kT1 = 3.3 keV, kT2 = 15.1 keV BURSTS Enoto et al. 2009

GBM data for _136 (common with Suzaku): Integrated spectrum can be fitted with two BB or one BB + PL kT 1 = 8 keV, kT 2 = 18 keV or kT = 11 keV,  = -2.4 Kouveliotou et al Watts et al. 2010

Three episodes detected with GBM: Oct. 2008, Jan. & Mar P = 2.069s P = x s/s and B = 2.2 x G Near IR detection, Ks = 18.5±0.3 GBM triggered on 131 events from the source; many more in the data SGR formerly known as AXP 1E formerly known as an ASCA CCO in G

SGR 1550–5418 Bursting Activity See posters by A. von Kienlin (P2 78) and A. van der Horst (P2 234)

Bursting Activity during 22 January 2009: ~450 bursts in 24 hours van der Horst et al. 2010

Magnetar twist and shake… Kaneko et al Talk by Ersin Gogus tomorrow

1E outbursts: Swift, XMM, CXO, INTEGRAL, Parkes, VLT-IR Oct 08  L ~ 50 ToO: Swift INTEGRAL Jan 09  L > 1000 ! ToO: Chandra XMM Parkes VLT-IR Swift Israel et al 2009 Mereghetti et al 2009

GBM Dead time and pulse pile-up effects in bright SGR bursts WARNING: Flat area is due to instrumental effects TTE light curves saturate at a total of detector count rate of 375 kHz K-edge corrections need fine tuning Pulse pile-up effects are currently being studied with simulations of burst spectra and intensities

~10 43 ergs few ergs Rise time of ~ 50ms testifies of a different mechanism with respect to GFs (ms rise time) Mereghetti et al. 2009

Cohen et al SGR bursts observed via VLF propagation disturbances! Provide a unique measure of the total ionizing fluence of X-rays above 0.05keV Fishman et al. 2010

The 27 August 1998 Giant Flare from SGR (Inan et al. 2009)

Tiengo et al An expanding light echo clearly detected in Swift XRT See also Poster by Vianello et al. P2 80)

SGR GBM triggered on 5 June 2009 – new source confirmed with IPN RXTE ToO program triggered ~ 4 days after the GBM triggers P = (1) sec ν ~ 2 x Hz/s at 3σ and B < G CXO location: RA = 04h 18m s, Dec = +57d 32' 22.91" No IR (Ks > 21.3, Wachter et al 2009) or optical (R > 24, Ratti, Steeghs & Jonker 2009) counterpart detected GBM triggered on 2 events from the source.

Woods et al 2010 Apparent Glitch  ν / ν = 2x10 -5 ν -dot > 3.8x Hz/s at 3 σ B~5 x G (Israel et al. 2009)

Absorbed blackbody: N H =(0.13±0.03)x10 22 cm -2, kT=0.88±0.01 keV Unabsorbed flux ( keV) = 1.1x ergs/cm 2 /s. Woods et al 2010 Swift/XRT Persistent source spectrum

Magnetar Candidates

SGR burst time history with Fermi/GBM SGR (7/131) SGR (26) SGR (2) (2)

Conclusions We need to understand: The differences – if any – between AXPs, SGRs and rotationally powered pulsars, in: persistent emission spectra glitching properties magnetic field strengths burst fluences and spectra The associations of magnetars with SNRs, and their environments and track possible proper motions, now with two best candidates The progenitor properties of magnetars, such as mass and cluster memberships Magnetar Key Project status; very ambitious: 7 papers in progress, more ideas welcome!

Abstracts due: December 1 st Information, abstract submission and registration:

Astrophysics of Neutron Stars 2010 ASTRONS – 6 August 2010 Çeşme – Izmir Fermi results are welcome! visit