Abstract:Observations of active galactic nuclei and microquasars by ASCA, RXTE, Chandra and XMM–Newton indicate the existence of wide X‐ray emission lines of heavy ionized elements in their spectra. The emission can arise in the inner parts of accretion discs where the effects of general relativity must be counted; moreover, such effects can dominate. We describe a procedure to estimate an upper limit of the magnetic fields in the regions where X‐ray photons are emitted. We simulate typical profiles of the iron Kα line… Show more
“…Even if we consider a supermassive black hole in the center of the quasar M SMBH = 10 9 M , then its Schwarzschild radius is r g = 3× 10 14 cm and assuming that the emission region for the X-ray radiation is located near the black hole r emission < 100 r g = 3 × † Simulations of X-ray line profiles are presented in a number of papers, see, for example, Zakharov & Repin (2002a,b,c,d, 2003a, 2003c) and references therein, in particular Zakharov et al (2003) showed that an information about magnetic filed may be extracted from X-ray line shape analysis; Zakharov & Repin (2003b) discussed signatures of X-ray line shapes for highly inclined accretion disks, Zakharov et al (2004a) calculated shapes of spectral lines for non-flat accretion flows. 10 16 cm, we obtain that r emission < R EC , therefore the point size source approximation can be adopted for the X-ray emitting region.…”
Section: Cosmological Distribution Of Microlensesmentioning
Abstract. We consider a contribution of microlensing to the X-ray variability of high-redshifted QSOs. Cosmologically distributed gravitational microlenses could be localized in galaxies (or even in bulge or halo of gravitational macrolenses) or could be distributed in a uniform way. We have analyzed both cases of such distributions. We found that the optical depth for gravitational microlensing caused by cosmologically distributed deflectors could be significant and could reach 10 −2 − 0.1 at z ∼ 2. This means that cosmologically distributed deflectors may contribute significantlly to the X-ray variability of high-redshifted QSOs (z > 2). Considering that the upper limit of the optical depth (τ ∼ 0.1) corresponds to the case where dark matter forms cosmologically distributed deflectors, observations of the X-ray variations of unlensed QSOs can be used for the estimation of the dark matter fraction of microlenses.
“…Even if we consider a supermassive black hole in the center of the quasar M SMBH = 10 9 M , then its Schwarzschild radius is r g = 3× 10 14 cm and assuming that the emission region for the X-ray radiation is located near the black hole r emission < 100 r g = 3 × † Simulations of X-ray line profiles are presented in a number of papers, see, for example, Zakharov & Repin (2002a,b,c,d, 2003a, 2003c) and references therein, in particular Zakharov et al (2003) showed that an information about magnetic filed may be extracted from X-ray line shape analysis; Zakharov & Repin (2003b) discussed signatures of X-ray line shapes for highly inclined accretion disks, Zakharov et al (2004a) calculated shapes of spectral lines for non-flat accretion flows. 10 16 cm, we obtain that r emission < R EC , therefore the point size source approximation can be adopted for the X-ray emitting region.…”
Section: Cosmological Distribution Of Microlensesmentioning
Abstract. We consider a contribution of microlensing to the X-ray variability of high-redshifted QSOs. Cosmologically distributed gravitational microlenses could be localized in galaxies (or even in bulge or halo of gravitational macrolenses) or could be distributed in a uniform way. We have analyzed both cases of such distributions. We found that the optical depth for gravitational microlensing caused by cosmologically distributed deflectors could be significant and could reach 10 −2 − 0.1 at z ∼ 2. This means that cosmologically distributed deflectors may contribute significantlly to the X-ray variability of high-redshifted QSOs (z > 2). Considering that the upper limit of the optical depth (τ ∼ 0.1) corresponds to the case where dark matter forms cosmologically distributed deflectors, observations of the X-ray variations of unlensed QSOs can be used for the estimation of the dark matter fraction of microlenses.
“…A detailed discussion of the magnetic field influence on spectral line shapes for flat accretion flows was given by [54] (see also paper [80]) and for non-flat accretion flows by [79]. A possibility to observe mirages (shadows) around black holes using space based interferometers (like Radioastron space radio telescope) was discussed in paper [81].…”
Section: Discussionmentioning
confidence: 99%
“…We used an approach discussed in detail in papers [38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54]. The approach was used in particular to simulate spectral line shapes.…”
Section: Methodsmentioning
confidence: 99%
“…The approach was used in particular to simulate spectral line shapes. For example, Zakharov et al [54] used this approach to simulate the influence of a magnetic field on spectral line profiles. This approach is based on results of a qualitative analysis (which was done by for different types of geodesics near a Kerr black hole [55,56]).…”
Abstract. Recent X-ray observations of microquasars and Seyfert galaxies reveal broad emission lines in their spectra, which can arise in the innermost parts of accretion disks. Simulations indicate that at low inclination angle the line is measured by a distant observer as characteristic two-peak profile. However, at high inclination angles (> 85 0 ) two additional peaks arise. This phenomenon was discovered by using the Schwarzschild black hole metric to analyze such effect. They assumed that the effect is applicable to a Kerr metric far beyond the range of parameters that they exploited. We check and confirm their hypothesis about such a structure of the spectral line shape for the Kerr metric case. We use no astrophysical assumptions about the physical structure of the emission region except the assumption that the region should be narrow enough. Positions and heights of these extra peaks drastically depend on both the radial coordinate of the emitting region (annuli) and the inclination angle. It was found that these extra peaks arise due to gravitational lens effect in the strong gravitational field, namely they are formed by photons with some number of revolutions around black hole. This conclusion is based only on relativistic calculations without any assumption about physical parameters of the accretion disc like X-ray surface emissivity etc. We discuss how analysis of the iron spectral line shapes could give an information about an upper limit of magnetic field near black hole horizon.
“…In fact, several observations show that there are various scenarios where the magnetic fields and general relativity can not be neglected . One of them is the presence of strong magnetic fields in active galactic nuclei [6,7,8,9]. These nuclei are known to produce more radiation than the rest of the entire galaxy and directly affect its structure and evolution.…”
An analytical solution of Einstein-Maxwell equations with a static fluid as a source is presented. The spacetime is represented by the axially symmetric Weyl metric and the energy-momentum tensor describes a coupling of a fluid with an electromagnetic field. When appropriate limits are performed we recover the well-known solutions of Gutsunaev-Manko and Schwarzschild. Also, using Eckart's thermodynamics, we calculated the temperature, the mechanical pressure, the charge density and the energy density of the system. The analysis of thermodynamic quantities suggests that the solution can be used to represent a magnetized compact stellar object surrounded by a charged fluid.
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