black holes : observations lecture 1: introduction

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Black holes: observations Lecture 1: Introduction Sergei Popov (SAI MSU)

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Black holes : observations Lecture 1: Introduction. Sergei Popov ( SAI MSU ). Plan of the lectures. Introduction. Formation of stellar mass BHs. GRBs, SNae. 2. Isolated stellar mass BHs BHs in close binary systems. ULX. Binary population synthesis code. - PowerPoint PPT Presentation

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Page 1: Black holes :  observations Lecture  1:  Introduction

Black holes: observationsLecture 1: IntroductionSergei Popov

(SAI MSU)

Page 2: Black holes :  observations Lecture  1:  Introduction

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Plan of the lectures.

1. Introduction. Formation of stellar mass BHs. GRBs, SNae.2. Isolated stellar mass BHs3. BHs in close binary systems. ULX. Binary population synthesis code.4. Supermassive BHs. Mass measurements. Sgr A*.5. Mass growth of supermassive BHs. Hierarchical model.

BH coalescence. Gravitational waves. GW rocket.6. Jets from BHs. Tidal disruption.7. Horizon problem. Primordial BHs. Exotic alternatives.

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Main general surveys

• astro-ph/0610657 Neven Bilic BH phenomenology

• astro-ph/0604304 Thomas W. Baumgarte BHs: from speculations to observations • hep-ph/0511217 Scott A. Hughes Trust but verify: the case for astrophysical BHs

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BHs as astronomical sources

• Primordial BHs. Not discovered, yet. Only upper limits (mostly from gamma-ray observations). • Stellar mass BHs. There are more than twenty good candidates in close binary systems. Accretion, jets. Observed at all wavelenghts. Isolated stellar mass BHs are not discovered up to now. But there are interesting candidates among microlensing events. • Intermediate mass BHs. Their existence is uncertain, but there are good candidates among ULX. Observed in radio, x-rays, and optics.• Supermassive BHs. There are many (dozens) good candidates with mass estimates. In the center of our Galaxy with extremely high certainty there is supermassive BH. Accretion, jets, tidal discruptions of normal stars. Observed at all wavelenghts.

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The most certain BH – Sgr A*

(see the reference in gr-qc/0506078)

Stellar orbits from 1992 till 2007

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... and it becomes more and more certain

(see the reference in gr-qc/0506078)

Observations are going on.So, the number of stars with well measured orbits grows.

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Stellar mass BHs.The case of solar metallicity.

(Woosley et al. 2002)

BHs are formed by massive stars.The limiting mass separating BH and NS progenitors is not well known.In addition, there can be a range ofmasses above this limit in which, again,NSs are formed (also, there can bea range in which both types ofcompact objects form).

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Mass spectrum of compact objects

(Timmes et al. 1996, astro-ph/9510136)

Results of numerical models

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Mass spectrum of compact objects

(Timmes et al. 1996, astro-ph/9510136)

Comparison of a computer modelwith observations

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A NS from a massive progenitor

(astro-ph/0611589)

Anomalous X-ray pulsar in the cluster Westerlund1most probably has a very massive progenitor, >40 MO.

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Stellar mass BHs. The case of zero metallicity

(Woosley et al. 2002)

Pop III massive stars couldproduce very massive BHs whichbecame seeds for formationof supermassive BHs.

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BHs and NSs in close binary systemsStudying close binaries with compact objects we can obtain

mass estimates for progenitors of NSs and BHs (see, for example, Ergma, van den Heuvel 1998 A&A 331, L29).

An interesting result was obtained for the NS system GX 301-2. The progenitor mass was found to be equal to 50 solar masses or more.On the other hand, for many systems with BHs estimates of progenitor masses are lower: 20-50 solar masses.

Finally, for the BH system LMC X-3 the mass of the progenitor is estimated as >60 solar masses.

So, the situation is rather complicated.Most probably, in some range of masses, at least in binary systems,both variants are possible.

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Binary evolution

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“Scenario machine” calculations

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GRBs and BHs

According to the standard modern model of long GRBs, a BH is the main element of the “central engine”.

So, studying GRBs we can hope to get important informationabout the first moments of BH’s life.

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NS and BH coalescenceNumerical models show (astro-ph/0505007, 0505094) that such eventsdo not produce GRBs

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Prompt mergers of NSs with BHs

(astro-ph/0505094)

Coleman Miller in his recent paperdemonstrated that in NS-BH coalescence most probably there isno stable mass trasfer andan accretion disc is not formed.This means – no GRB!

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A signal from ergosphere

(arXiv: 0706.3191)

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Details on GRB light curves

(arXiv: 0706.3191)

Afterglow

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Supernovae and GRBs

(arXiv:0706.3047)

SN Ib/c are often observedin the radio band.

It was shown that just afraction of them can be relatedto GRBs or XRFs (about few %).

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SupernovaeThe neutrino signal during a (direct) BH formation must be significantly differentfrom the signal emitted during a NS formation.

(arXiv: 0706.3762)

Constant growth of neutrino energy and a sharp cut-off indicate a BH formation.

Different curves are plotted for different types of neutrino:electron – solid, electon anti-neutrino – dashed, mu and tau-neutrinos – dot dashed.

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BH signatures in SN light curves

Balberg, Shapiro astro-ph/0104215

(see also Zampieri et al., 1998, ApJ 505, 876)

For this plot no radiactive heatingis taken into account.