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Untitled - Laboratoire d'Astrophysique de l'Observatoire de Grenoble

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states, combining a still powerful jet and a luminous accretion disk. In these states, disk photons can be scattered<br />

up to very high energy by non thermal particles from the jet, which would produce enough gamma-ray photons<br />

to trigger pair production. Detailed quantitative calculations are un<strong>de</strong>r work.<br />

In another work, with the PhD stu<strong>de</strong>nt Cl?ment Cabanac, we are studying the time behavior of X-ray<br />

binaries observed with the hard X and γ-rays satellite INTEGRAL. We are currently <strong>de</strong>veloping numerical<br />

tools to extract the time information from the raw data, especially the presence of quasi-periodic oscillations<br />

(QPO) that have been commonly <strong>de</strong>tected by the RXTE satellite. The origin of these QPO is still disputed<br />

and an important question is their energy spectrum. We are <strong>de</strong>veloping in parallel a theoretical mo<strong>de</strong>l for these<br />

QPO based on an instability at the transition region between the SAD and the JED.<br />

15.6 Relativistic Plasmas and Cosmic Rays<br />

The non-thermal radiation from Black Hole environments is emitted by a relativistic plasma generated in the<br />

jets. Therefore high energy radiation (including TeV gamma rays, cosmic rays and possible neutrinos) is an<br />

important consequence of accretion-ejection flows around Black Holes. These relativistic plasmas are generated<br />

by specific dissipation mechanisms occurring at relativistic shocks and magnetic reconnections that require some<br />

theoretical <strong>de</strong>velopments. Moreover the dynamics of these accretion-ejection flows cannot be fully mastered<br />

without a significant un<strong>de</strong>rstanding of these microphysics processes. Some progress have been recently done in<br />

our team on these topics which are at the forefront of the physics of the so-called ”Astroparticle Science”.<br />

15.6.1 Relativistic plasmas<br />

Relativistic aspect of the accretion-ejection phenomenon.<br />

The issue of the formation of relativistic jets involves three important intricate problems, namely, the crossing<br />

of critical surfaces, collimation and conversion of the Poynting flux into matter-energy flux. These problems<br />

have been addressed in a synthesis that will appear in a collective book organized by R. Blandford and M.<br />

Lyutikov (Pelletier 2005).<br />

A major problem of the physics of accretion disks is the excitation of a turbulence state able to efficiently<br />

transfer the angular momentum of matter in or<strong>de</strong>r that it progressively falls on the central Black Hole. In the<br />

nineties, a successful solution has been proposed with the so-called ”Magneto-Rotational Instability”. We have<br />

exten<strong>de</strong>d the analysis of the instability to the case of a Kerr Black Hole and found an expected intensification<br />

and a wi<strong>de</strong>r window of the instability, that makes it compatible with the intense magnetic field required for<br />

launching jets, <strong>de</strong>spite the stabilizing ten<strong>de</strong>ncy of its tension effect. The analysis has been presented in the<br />

same chapter as before and will be <strong>de</strong>veloped in a forthcoming paper.<br />

Magnetic reconnection in relativistic regime.<br />

Nowadays the process of ”magnetic reconnection” is invoked in or<strong>de</strong>r to convert Poynting flux into matter<br />

energy flux and radiation in ultra-relativistic flows. Only very fast reconnection processes can be relevant in this<br />

context. Now standard reconnection processes based on the generalization of the Sweet-Parker scheme are too<br />

slow. New investigations in Tokamaks and space plasma physics revealed a new mechanism that turns out to be<br />

in<strong>de</strong>pen<strong>de</strong>nt on dissipation and fast. We are extending this approach to relativistic plasmas. A fair <strong>de</strong>scription<br />

of the phenomenon can be obtained in the frame of an appropriate modification of relativistic MHD for both<br />

baryon loa<strong>de</strong>d plasmas and e + − e − -plasmas. This has been presented in a first publication (Pelletier 2005) and<br />

a paper on relativistic reconnection is to be submitted (Pelletier & Longaretti 2005).<br />

15.6.2 Cosmic Rays<br />

Transport of Cosmic Rays in chaotic magnetic fields.<br />

The properties of the transport of Cosmic Rays in weak turbulence theory are known since the seventies.<br />

154

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