Observational appearance of strong gravity in X-rays
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1 Observational appearance of strong gravity in X-rays
2 Compact object Companion star (5000 K)
3
4 Schwarzschild radius Schwarzschild metric R s 2GM Schwarzschild radius (= 2.95 km for 1М ) c 2
5 Accretion Black holes can be seen via their influence on nearby objects Accretion gradual motion of matter towards gravitating object Where the matter comes from? interstellar from companion star Mass accretion rate and the luminosity
6 Accretion luminosity 1 GMcM 2R c 2 2 L ~ ~ Mc Mc R c R s 2GM Rs - Schwarzschildradius(= 3 km for 1M 2 c 2R Rs c 1 - accretionefficiency sun ) M ~ 10 L x ~ Msun/yr erg/s ~ 0.1, R c ~ 5R s (~ 15km for 1M sun )
7 Why X-rays? R ~ 5 R S = 4 R L x ~ T 2 4 s ~ 15 - emitting area S T ~ (Stefan - Boltzman law) M M M M Sun Sun 1/2 km K ~ 1-2 M M Sun 1/2 kev ~ 1 2 kev for NS ~ kev for BH
8 Black body emission Rayleigh-Jeans law
9 Stefan-Boltzman law
10 Black body normalization => size of the emitter
11 Scheme of BH with accreton disk
12 Non rotating BH Rotating BH Inner disk radius -> BH parameters
13 Radius of innermost stable orbit around rotating BH
14
15 ~kt ~Rin Inner disk radius?
16 Problem 1: Brightness distribution The simplest case T~ R -3/4
17 RJ law The simplest case
18 Shakura, Sunyaev 1973
19 Norman, Krolik, Schnittman et al.
20 Disk surface brightness in simulations Beckwith et al. 2008
21 Problem 2: Disk atmosphere (opacity and Comptonization)
22
23 Opacity dependence on energy/wavelength
24 Comptonization Одно рассеяние: ~ E e m e c 2 ~ 4kT e m e c 2 если гладкий спектр / 1 Степенной закон между ~kt seed and ~3kT e Тепловой завал e ~ + 4kT e m e c 2 h m e c 2
25 Suleimanov et al. In order to have the outgoing flux one need to have gradient of energy density, gradient of temperature Atmosphere
26 Suleimanov et al. Spectral kt c ~1.7kT distortion
27 Lum-Tdisk dependence and color correction Davis et al. 2006
28 Problem 3 (small) Light bending
29 Black hole parameters from properties of fluorescent emission lines?
30 Reflection from rapidly rotating accretion disk
31 Relativistic line in AGN MCG ? ASCA (1995) Tanaka et al. 1995
32 MCG XMM (2002)
33 Interpretation problem: line of sight absorption?
34 Problems 4. Characteristics of instruments
35 Energy response of instruments X-rays are measured in counts(c) at energy channels (h) h- energy channel (from pulse height ) M model of true emission of the source A(E) effective area of the instrument as a function of energy R(E,h) redistribution matrix of photons into channels
36 Finite energy resolution
37 Even worse in early experiments:
38 Processes in detectors
39 Counts Photopeak Ka photons Compton effect
40 Non-diagonal elements redistribution matrix of Si CCD
41 1995 Proportional Counters response 1979 Limited by electron counts Escape peaks
42 CCD camera SIS/ASCA ( )
43 CHANDRA/ACIS-I (1999- )
44 Effective area of instruments
45 Calibration issues Schellenberger et al XMM-CHANDRA cross-calibration
46 XMM-CHANDRA-SUZAKU cross-calibration with blazar Ishida et al. 2011
47 XMM-CHANDRA-SUZAKU-SWIFT-RXTE-INTEGRAL cross-calibration with supernova remnant Tsujimoto et al. 2010
48 Ice absorption on SSS detector of EINSTEIN
49 Accuracy of effective areas of detectors CHANDRA ACIS-S Effective area Drops at energies below 2 kev due to CCD surface contamination
50
51
52 Spatial distribution of abs.contamination (SUZAKU)
53 CHANDRA/ACIS
54 Charge transfer inefficiency
55 Catechism of X-ray astronomer 1. Before making strong claims one should pay attention to calibration issues!
56 E E Problem pile-up dt(pile-up) 2E 2 photons with some energies might look as one photon with larger energy
57
58 Or might even be rejected after post processing due to energy higher than high threshold
59 Even in gas counters pile up effect is present PCA spectrometer (dt~10-5 sec) For CCD dt~0.1-1 sec!
60 Pile-up problems of XMM
61 MOS PN comparison EPIC-PN CCD camera less affected by pile up
62 Fluorescent lines in emission of NS binaries Ng et al. 2011
63 With wrong Cackett et al. correction With correction Dias-Trigo et al.
64 Example of file with events
65 EXAMPLE of real event file of X-ray detector
66 Next step- microcalorimeter Astro-H(Japan) 2015?
67
68
69 Maximum likelihood
70
71
72
73
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