Nanda Rea. XMM-Newton reveals magnetars magnetospheric densities. University of Amsterdam Astronomical Institute Anton Pannekoek NWO Veni Fellow

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Transcription:

XMM-Newton reveals magnetars magnetospheric densities Nanda Rea University of Amsterdam Astronomical Institute Anton Pannekoek NWO Veni Fellow In collaboration with : Silvia Zane Roberto Turolla Maxim Lyutikov Diego Gotz Luciano Nobili

Introduction: Magnetars bright X-ray pulsars Lx ~ 10 33-10 36 erg/s rotating with periods of 2-12s large period derivatives glitches bursts on many timescales (ms to 100s) transient outbursts radio pulsars only during outbursts (review: Woods & Thompson 2006, Cambridge Press; Mereghetti 2008, A&AR)

Introduction: Magnetars Hard X-rays soft X-rays Gamma-rays IR and optical Radio

Introduction: Magnetars RXS J1708-4009 XTE 1810-197 (Rea et al. 2005, MNRAS; Gotthelf et al. 2004, ApJ)

Main point: closed field lines in NS magnetospheres are not dead. Populated by hot, highly over-dense plasma, n >> ngj (e.g. Thompson, Lyutikov & Kulkarni 2002; Liutykov & Gavriil 2006) Twisted magnetospheres are filled with plasma which may modify radiation properties. # " RCS ~ R & L % (" T ~ 10 5 " T $ ' at 1 kev with " B R L ~ 8R NS NS $ # r e B crit 1/ 3 % " 1keV ' $ & # h( B % ' & 1/ 3

ω 0 =ω B n + ω 0 n- Δr ~r β T /3 <<r How does a warm plasma in the magnetosphere modify the emergent spectra?

3 free parameters, same as for the empirical blackbody+powerlaw model: Flux same statistical significance Optical depth $ e dz. " RCS = # RCS n (1-10) 0.1 - Energy (kev) - 10 Electron thermal velocity " T (0.1-0.5) Surface Temperature (kev) kt (0.1-1.3) Flux 1 - Energy (kev) - 10 Rea, Zane, Turolla, Lyutikov & Gotz 2008, ApJ submitted, arxiv:0802.192v2

The Magnetar Sample Hosts P (s) B (10 14 G) kt(kev) / Γ L (10 33 erg/s) (0.2-10keV) comments 4U 0142+61 8.7 1.3 0.46 / 3.4 72 hard X RXS J1708-4009 11 4.7 0.44 / 2.4 80-190 hard X 1E 1841-045 Kes 73 11.8 7.1 0.44 / 2.0 110 hard X 1E 2259+586 CTB 109 7.0 0.6 0.41 / 3.8 17-159 ~ transient/hard X CXO J0100-72 in SMC 8.0 3.9 0.38 / 2.0 200 1E 1048-5937 6.4 3.9 0.63 / 2.9 5.3-250 ~ transient 1E 1547-5408 2.0 2.2 0.52 / 2.9 2.6-170 transient/radio XTE 1810-197 5.5 2.9 0.67 / 3.7 5-260 transient/radio CXO 1647-4552 in Wes1 10.6 1.5 0.68/2.0 1-130 transient AX J1845-0258 G29.6+0.1 7.0 - / 4.6 5-120 transient SGR 1900+14 OB 5.2 5.7 0.43 / 2.0 200-350 GF/hardX SGR 1806-20 OB 7.5 7.8 0.6 / 1.4 320-540 GF/hardX/outburst SGR 0526-66 in LMC 8.0 7.4 0.53 / 3.1 260 GF/? SGR 1627-41 G337.0-0.1? 6.4? - / 2.9 4-100 outburst

AXPs with hard X-ray emission 4U 0142+61 4U 0142+61 Flux BB+PL+PL 1 - Energy (kev) - 200 RXS J1708-4009 RXS J1708-4009 RCS+PL BB+PL+PL RCS+PL 1E 1841-045 1E 1841-045 BB+PL RCS+PL Rea, Zane, Turolla, Lyutikov & Gotz 2008, ApJ submitted, arxiv:0802.192v2

Transient AXPs 1E 1048-5937 CXO 1647-4552 BB+PL Flux RCS BB+PL RCS 1 - Energy (kev) - 10 1E 1547-5408 XTE 1810-197 BB+PL BB+PL RCS RCS Rea, Zane, Turolla, Lyutikov & Gotz 2008, ApJ submitted, arxiv:0802.192v2

SGRs with hard X-ray emission SGR 1900+14 SGR 1806-20 Flux SGR 1900+14 BB+PL 1 - Energy (kev) - 200 BB+PL SGR 1806-20 Flux RCS+PL RCS+PL 1 - Energy (kev) - 10 Rea, Zane, Turolla, Lyutikov & Gotz 2008, ApJ submitted, arxiv:0802.192v2

kt (kev) L 1-10keV (10 34 erg/s) Rea, Zane, Turolla, Lyutikov & Gotz 2008, ApJ submitted, arxiv:0802.192v2

τ res L 1-10keV (10 34 erg/s) Magnetospheric e- density of n~1.5x10 13 cm -3 = 10 3 n GJ Rea, Zane, Turolla, Lyutikov & Gotz 2008, ApJ submitted, arxiv:0802.192v2

3D Monte Carlo RCS: applications (preliminary) 1E 1547-5408 RCS 3D kt ~ 0.2-0.6 kev β bulk ~ 0.2-0.4 Δφ ~ 1-1.8 1E 1048-5937 Magnetospheric e- density consistent with the simplified 1D model, hence being ~ 10 3 n GJ 1E 1841-045 RCS 3D RCS 3D +PL (Nobili, Turolla & Zane 2008, MNRAS; Rea et al. 2008, in prep; Albano et al. 2008, in prep)

Conclusions done We built an analytical model to threat resonant cyclotron scattering Implementing it in XSPEC for real data fitting Resonant cyclotron scattering reproduces all magnetar spectra This model has a clear physical motivation, unlike BB+PL models We could derive for the first time the magnetospheric density of magnetars Much larger than for normal pulsars, as indeed predicted by the theory Absorption values now matches what has been derived from single edge fitting The BB+PL model overestimates the N H http://heasarc.gsfc.nasa.gov/docs/xanadu/xspec/models/rcs.html in progress More advanced 3D Monte-Carlo models for magnetar magnetospheres Full 3-D magnetosphere (Fernandez & Thompson 2007; Nobili, Turolla & Zane 2008) Application to the data (Rea et al. in prep; Albano et al. in prep)