Download presentation
Presentation is loading. Please wait.
Published byHannah Hart Modified over 6 years ago
1
Recent Suzaku Results on Strongly Magnetized Neutron Stars
Kazuo Makishima (University of Tokyo and RIKEN) T. Enoto, T. Mihara, M. Nakajima, K. Nakazawa, & Y. Terada 2008/5/29 X-ray Universe 2008
2
1. Strongly Magnetized NSs
Measurements of surface m.f. using electron cyclotron resonances; Ea = 11.6 (B/1012G) keV Measured m.f. strengths clustered in (1~5)x1012 G (Makishima + 99). “Field decay” hypothesis unlikely. Resonance photosphere height depends on Lx (Nakajima Poster D.7). 2 4 6 8 10 Resonance Energy (keV) Number 100 20 5 50 Log B (Gauss) 12 13 BeppoSAX Ginga RXTE Suzaku ASCA Is m.f. due to nuclear ferromagnetism (Makishima + 99)? Magnetars really have G? Any objects in between ordinary pulsars and magnetars? Origin of the resonance width? 2008/5/29 X-ray Universe 2008
3
2. Suzaku Observations [Accreting Binary Pulsars]
A Terada+ ApJL (2006); Naik+ ApJ (2008) Her X Enoto+ PASJ (2008); Terada+ AdSpRes (2007) 4U GRO J (TOO) [Rotation-Powered Pulsars] The Crab pulsar PSR Terada+ PASJ (2008) [Magnetars] 4U Enoto+. in prep. 1E Morii+ AIPC (2008) AXP CXOU J (TOO) Naik+ PASJ (2008) SGR (TOO) SGR (TOO; burst+persistent) Esposito+ A&A (2008) PSR 1509 On-Off, 45 ks HXD-PIN HXD-GSO 2008/5/29 X-ray Universe 2008
4
3. Crab Ratios Continuum and absorption couple strongly.
0.05 0.02 0.01 .002 42 keV 2005 36 keV HXD-GSO 2006 0.1 .01 Lx=4x1035 erg/s A (Suzku,Terada+06) HXD-PIN Her X-1 on-off (Suzaku, Enoto + 08) Lx=3x1037 erg/s 23 keV 1 .1 .01 Energy (keV) Continuum and absorption couple strongly. Using regions near Ea1/2 and >3Ea1, define the continuum as f(E)=AEα exp(-E/Ecut) X (RXTE ; Nakjima + 08) Lx=3x1038 erg/s 2008/5/29 X-ray Universe 2008
5
4. Extraction of Absorption Profiles
Assuming spectrum = f(E)xexp[-S(E)], exp[-S] is plotted logarithmically. The vertical scale thus becomes -S itself. The energy axis is normalized to Ea1, and ordinatge is adjusted by ~20% The three objects exhibt very similar profiles. A Her X-1 On-Off X0331 RXTE 1 0.5 0.2 0.1 pivot 2008/5/29 X-ray Universe 2008
6
5. Joint Fitting of the 3 Pulsars
F(E)=(aE-α+bEβ) exp(-E/Ecut) exp{-S1(E/Ea1)-S2(E/Ea2)} ・“NPEX” continuum : independent among the three. ・S1: Lorentzian xE2, common to the three as a function of E/Ea. ・S2 : likewise, but X0331 is allowed to have separate Ea2 and W2. Count Spectra X0331 (PCA) X0331 (HEXTE) Deconvolved νFν keV Her X-1 A0535 (PIN) A0535 (GSO) χ2/ν=1.08 D1=1.61 ± 0.06 W1/Ea1=0.36 ±0.02 D2=1.51 ± 0.13 keV 2008/5/29 X-ray Universe 2008
7
6. Implications The 3 objects are in common physical conditions, despite the luminosity differences by ~3 orders of magnitude. cf. Not claiming that this applies to all accreting pulsars. The NPEX continuum is justified; the1st and 2nd resonances heavily affect the continuum even in between Ea1 and Ea2. Gaussian absorption cross section gives significantly worse joint fits than the Lorentzian x E2 cross section (Enoto et al. 2008); chi^2= vs for the same d.o.f=287. The resonance width may not be explained by the thermal Doppler effects. Unexpectedly short lifetimes of the excited Landau levels (Enoto et al. 2008)? 2008/5/29 X-ray Universe 2008
8
7. AXP 4U (Enoto et al.) Observed with Suaku on 2007 Aug. 13 for 93 ksec. Soft pulsations are stable. Hard pulses vary on ~30 ks. Very hard component with Gamma~1. Improves INTEGRAL results (Kuiper+06). GSO XIS PIN P= sec 1st 30 ks 2nd 30 ks 3rd 30 ks 0.06 0.04 0.02 e+e- creation --> rush onto mag.poles --> non-thermal Bremss --> Compton back scatt. (Kotoku+07 PASJ) A BGD-subtracted keV folded pulse profile 2008/5/29 X-ray Universe 2008
9
8. Summary Spectra of accreting X-ray pulsars are strongly affected by electron cyclotron resonances, but the effects may be rather common among different objects. The continuum must be carefully determined using wide-band data. The spectrum of an AXP, 4U is clearly distinct from those of any accreting/rotating X-ray pulsars. A ultra-strong MF provides the most likely explanation. Existence of intermediate objects between magnetars and normal strong-field NSs is open (cf. Dr. Haberl’s talk). Further Suzaku observations are of great value. 2008/5/29 X-ray Universe 2008
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.