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Are there atoll/Z sources in HMXB
Are there atoll/Z sources in HMXB? A rapid aperiodic timing analysis of 4 accreting X-ray pulsars in outburst Pablo Reig IESL, Foundation for Research & Technology-HELLAS Astronomy Group, Physics Dept. University of Crete
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Be/X-ray binaries HMXB Accreting X-ray pulsars Mainly transients
Be + NS Accreting X-ray pulsars Mainly transients Two types of outbursts Type I: Lx < 1037 erg/s, (quasi)periodic Porb, short Type II: Lx ~ erg/s, unpredictable, long
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CD in LMXBs Atoll sources Z sources van der Klis (2006)
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CD in HMXBs two branches HC makes the difference horizontal at low Lx
diagonal at intermediate & high Lx HC makes the difference 4U , EXO & KS as flux increases SC decreases, HC increases V SC decreases, HC decreases
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Hardness-Intensity Diagrams
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PSD in LMXBs LLF Ll Lb' Lb'' Lb Lu Lb LLF Ll Lu
Atoll source Z source LLF Ll Lb' Lb'' Lb Lu van Straaten et al. (2002) Lb LLF Ll Lu Belloni et al. (2002) νmax =(ν02 + Δ2)1/ Δ=FWHM/2
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multi-Lorentzian profile
4 BLN (Lb, Ll, Lu, Lu’) & 2 PN ≈ QPO (LLF, Ls) νb < νLF < νl < νu νs ≈ νspin --> coupling periodic/aperiodic var.
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PSD in HMXBs Lb Ll LLF Ls
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PSD in HMXBs Lb Ll LLF Ls
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PSD in HMXBs Lb Ll Lu Lu'
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PSD in HMXBs Lb Ll Lu
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HMXB vs LMXB: similarities
two different types 4U , EXO , KS V (~ Z) spectral branches smooth motion without jumps horizontal branch low flux & high rms PSD: multi-Lorentzian broad (zero-centred L) noise for low and high frequencies peaked noise for intermediate frequencies
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HMXB vs LMXB: differences
different topology slower motion along the branches hr-days in LMXBs, days-weeks in HMXBs ~ one order of magnitude longer time scales mHz QPOs, ν ~ Hz typically Ls noise associated with the pulse noise no apparent correlation between spectral parameters (characteristic frequencies, rms) Mdot
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