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By
A. B. Garson III, Washington University in St. Louis and McDonnell Center for the Space Sciences,
H. Krawczynski, Washington University in St. Louis and McDonnell Center for the Space Sciences
EXIST (Energetic X-ray Imaging Survey Telescope) is a proposed spaceborne observatory that combines a wide-field-of-view X-ray telescope (5–600 keV) with a pointed optical/infrared telescope, and possibly with a soft-X-ray telescope contributed by Italian collaborators. The primary science drivers of EXIST are the study of the high-redshift Universe and the epoch of re-ionization through the detection and follow-up observations of high-redshift gamma-ray bursts (GRBs) at z ∼ 10, the study of supermassive black holes in galaxies (including heavily obscured and dormant black holes), and the study of stellar-mass and intermediatemass black hole populations in the Milky Way galaxy and in the Local Group. In this contribution, we discuss the polarimetric capabilities of the EXIST hard X-ray telescope. Based on a pointed five-day observation (or based on four-months all-sky survey observations), EXIST can detect the hard X-ray polarization of 100 mCrab sources for polarization degrees down to 6%. The wide field of view of EXIST will make it possible to measure the polarization of transient events like GRBs and flaring galactic and extragalactic sources. We discuss the scientific potential of the hard-X-ray polarimetric measurements. The EXIST observations would allow us to (i) obtain qualitatively new constraints on the locale of particle acceleration in the vicinity of compact objects, (ii) gain key insights into the structure of jets from GRBs and active galactic nuclei, (iii) test high-order QED predictions in the extreme magnetic fields of neutron stars, and (iv) search for quantum gravity signatures (the helicity-dependence of the speed of light) with unprecedented sensitivity.
from
Part II
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Polarized emission in X-ray sources
By
M. Dovčiak, Astronomical Institute, Prague,
V. Karas, Astronomical Institute, Prague,
R. Goosmann, Observatoire Astronomique de Strasbourg,
G. Matt, Dipartimento di Fisica, Università degli Studi “Roma Tre”,
F. Muleri, INAF/IASF–Roma
Multicolour black-body emission from the accretion disc around the black hole can be polarized on its way through the atmosphere above the accretion disc. We model this effect by assuming Kerr metric for the black hole, a standard thin disc for the accretion flow and Thomson scattering in the atmosphere. We compute the expected polarization degree and the angle as they can be measured for different inclinations of the observer, optical thickness of the atmosphere and different values of the black hole spin. All relativistic effects near a compact centre are taken into account. We also assess the perspectives for the next generation of X-ray polarimeters.
Introduction
We consider polarization originating from a Keplerian, geometrically thin and optically thick accretion disc near a black hole. At each radius the accretion disc emits black body radiation, the temperature of which is given by the Novikov-Thorne expression for the outer part of the standard disc. The thermal photons are scattered in the atmosphere of the disc and thus the observed radiation becomes polarized. We assume multiple Thomson scattering with different optical depths of the disc atmosphere. The effect of hardening of the energy of photons due to scattering is taken into account via the hardening factor that increases the effective temperature.
Once the photons leave the atmosphere the polarization vector can be rotated due to strong gravity of the black hole. The energy of photons is shifted by the gravitational and Doppler effects.
Pulsar wind nebulae (PWNe) were the first objects where non-thermal polarized synchrotron emission was detected. They are one of the best astrophysical labs available for the study of high-energy processes like particle acceleration, properties of relativistic outflows, and non-thermal emission. Their broad-band spectrum makes them a suitable target for many instruments, and to date they are the only objects for which there is clear and undisputed evidence for high-energy X-ray polarized emission. In recent years a canonical model has been established which has proved incredibly successful in explaining many of the observed features. All of this makes PWNe a prime candidate for any future X-ray polarimetry study. I will review here the current MHD model, what we know from polarization in the optical and radio band, and what we might learn from next-generation polarimetry.
Introduction
Pulsar wind nebulae (PWNe) are bubbles of relativistic particles and magnetic field created when the ultra-relativistic wind from a pulsar interacts with the ambient medium, either SNR or ISM. The prototype, and the best studied of this entire class of objects, is the Crab Nebula. The canonical model of PWNe was first presented by Rees & Gunn, developed by Kennel & Coroniti, and is based on a relativistic MHD description. The pulsar wind is confined inside the SNR, and slowed down to non-relativistic speeds in a strong termination shock (TS).
PolariS (Polarimetry Satellite) is a Japanese small-satellite mission dedicated to polarimetry of X-ray and γ-ray sources. We aim to perform wide-band X-ray (2–80 keV) polarimetry of sources brighter than 10 mCrab, employing three hard X-ray mirrors and two types of polarimeters. X-ray and γ-ray polarimetry of transient sources with wide-field polarimeters is the second purpose. Most of the components have their prototype used or planned to be used in balloon and other satellite missions. Conceptual design is in progress for target launch in the mid 2010s.
PolariS concept
PolariS (Polarimetry Satellite) is a Japanese small satellite mission dedicated for polarimetry of X-ray and γ-ray sources. Design of the PolariS is now being discussed by the PolariS working group, which consists of 34 members from 11 institutes mainly in Japan, though informal international collaboration is under way.
The main purpose of the PolariS mission is wide-band X-ray (2–80 keV) polarimetry of sources brighter than 10 mCrab. We expect X-ray polarimetry with small satellites to be realized within several years. When measuring X-ray polarization of various type of sources, we consider the energy dependence of the polarization (degree and direction) to be essential to study the geometry and emission mechanisms of different objects, as has been pointed out by theoretical calculation. Furthermore, the hard X-ray band above 10 keV is of particular importance, since the physics we are exploring with polarimetry is in most cases nonthermal.
Active galactic nuclei (AGN) are definitely not spherical objects, but rather have an axisymmetric morphology. This, together with the fact that the primary X-ray emission is due to Comptonization, and that there are several circumnuclear regions which may scatter the primary radiation, implies that most, if not all, of the X-ray spectral components observed in radio-quiet AGN should be significantly polarized. Moreover, the polarization properties of the radiation emitted very close to the black hole are modified by Special and General Relativity effects, which therefore can be probed with X-ray polarimetry.
Introduction
AGN have a complex morphology (see Figure 18.1). The nucleus, where a super-massive (106–109M⊙) black hole accretes matter from an accretion disc, is surrounded by optically and geometrically thick matter, possibly clumpy and probably in a toroidal (or at least axisymmetric) configuration. If the line of sight intercepts this ‘torus’, the nucleus is not visible and the source is classified as of type 2. For type 1 sources, instead, the line of sight does not intercept the ‘torus’, and the nucleus can be directly seen. Outside the ‘torus’, ionized matter, responsible for scattering and polarizing the nuclear radiation in type 2 sources is present. A jet is also present in ‘radio-loud’ sources, which are not discussed in this contribution, devoted to ‘radio-quiet’ AGN.
Programs of X-ray polarimetry in Italy arise from the convergence of a long experience of X-ray astronomy missions with an outstanding tradition in development of radiation detectors. The gas pixel detector in the focus of X-ray optics can perform angular-resolved polarimetry with a breakthrough improvement in sensitivity, even with a moderate collecting surface. POLARIX makes a large use of already existing items and, in particular, of the three telescopes from the JET-X program. It can extend the X-ray polarimetry from one positive detection only, to tens of sources, including a few brighter extragalactics: an ambitious pathfinder on a very limited budget. Phase A study of POLARIX, and of four other missions, was performed in 2008 and ASI should select two missions to fly. Another pathfinder is under study: two short telescopes, designed with modern tight packing techniques, mounted as piggy-back on the Chinese mission HXMT.
The national context
X-ray polarimetry has been a line of research at IASF for many years. A scattering polarimeter was proposed for the XMM mission, but was not selected. An IASF team joined the collaboration headed by R. Novick for the Stellar X-ray Polarimeter, aboard the Spectrum X-Gamma mission, contributing the detectors as the sensors for both scattering and diffraction stages. SXRP was completed but the whole mission was not. Considering the large area of the telescope, SXRP was close to the best achievable with conventional techniques.
Hard X-ray / soft gamma-ray polarimetric analysis can be performed efficiently by the study of Compton scattering anisotropy in a detector composed of fine pixels. But in the energy range above 100 keV where source fluxes are extremely weak and instrumental background very strong, such delicate measurement is actually very difficult to perform. The Laue lens is an emerging technology based on diffraction in crystals allowing the concentration of soft gamma-rays. This kind of optics can be applied to realize an efficient high-sensitivity and highangular-resolution telescope, though at the cost of a field of view reduced to a few arcmin. A 20-m focal-length telescope concept focusing in the 100–600 keV energy range is taken as example here to show that recent progresses in the domain of high-reflectivity crystals can lead to very appealing performance. The Laue lens being fully transparent to polarization, this kind of telescope would be well suited to perform polarimetric studies since the ideal focal plane is a stack of finely pixelated planar detectors – in order to reconstruct the point spread function – which is also ideal to perform Compton tracking of events.
Introduction
A Laue lens concentrates gamma-rays using Bragg diffraction in the volume of a large number of crystals arranged in concentric rings and accurately orientated in order to diffract radiation coming from infinity towards a common focal point (e.g.).
Neutron stars generate powerful winds of relativistic particles that form bright synchrotron nebulae around them. Polarimetry provides a unique insight into the geometry and magnetic configuration of the wind, but high-energy measurements have failed until recently. The INTEGRAL-IBIS telescope has been used in its Compton mode to search for linearly polarized emission for energies above 200 keV from the Crab nebula. The asymmetries in the instrument response are small and we obtain evidence for a strongly polarized signal at an angle parallel to the pulsar rotation axis. This result confirms the detection recently reported by, and extends the polarization measure for all the pulsar's phases. We also report the recent observation of a variable polarization signal from the long GRB 041219A. The achieved sensitivity opens a new window for polarimetric studies at energies above 200 keV.
Introduction
Gamma-ray polarimetry has been possible with Compton telescopes since the 1970s. Photons that are Compton scattered between two detectors follow an azimuthal distribution around the source direction that allows quantification of the degree and direction of linear polarization because the photon is preferentially scattered in a plane at right angles to its incident electric vector. It was unsuccessful until recently because of intrinsic asymmetries in the detector response and nonuniformities in the large background signals. They induce pseudo-polarimetric signals, even from an unpolarized source, that limit the sensitivity to any detection.
Polarization measurements of rotation-powered pulsars have been a very powerful diagnostic in the radio band and promise to be at least as useful a diagnostic in the X-ray band. Since the relativistic particles that radiate pulsar high-energy emission tightly beam the radiation along the pulsar magnetic field, phase-resolved polarimetry has the potential to map the emission patterns. Fermi observations of young pulsars at gamma-ray energies have disfavored polar-cap models where emission takes place near the neutron star surface, and strongly favor outer-magnetosphere models where emission takes place close to the light cylinder or beyond. Since the different outer-magnetosphere models predict similar gamma-ray light curves, it is difficult to discriminate between them at gamma-ray energies. But X-ray polarization has the potential to provide this discrimination, since the models predict distinct polarization signatures and optical detections will only be possible for a small number of pulsars.
Introduction
Rotating systems are particularly interesting to study with polarization because the rotation provides changing views of the emitting regions. Rotation-powered pulsars have the additional advantage that the emission is radiated by highly relativistic particles moving along magnetic field lines and therefore the emission angle measures the field direction to within an angle of 1/γ, where γ is the particle Lorentz factor. The magnetic field structure is also able to be derived independently, using either retarded-vacuum, force-free (e.g.) or pair-starved solutions.
from
Part II
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Polarized emission in X-ray sources
By
M. Weżgowiec, Obserwatorium Astronomiczne UJ,
M. Ehle, ESA, European Space Astronomy Centre,
M. Urbanik, Obserwatorium Astronomiczne UJ,
K.T. Chyży, Obserwatorium Astronomiczne UJ,
M. Soida, Obserwatorium Astronomiczne UJ,
R. Beck, Max-Planck-Institut für Radioastronomie,
B. Vollmer, CDS, Obs. Astronomique de Strasbourg
We present X-ray and radio polarimetric observations of selected Virgo Cluster spiral galaxies. The X-ray extended emission traces hot-gas filaments in galactic halos and is sensitive to the environmental effects exerted by interactions inside the cluster, like ram-pressure stripping. The radio polarization studies provide clues about alignment, distortion, compression and strength of detected magnetic fields. When used together, the two types of observations constitute an excellent tool for examining disturbances in galactic disks and halos caused by interactions of galaxies with the intracluster medium or between the galaxies themselves. The coming of age of X-ray polarimetry could provide us with unprecedented tools to explore further the evolution of galaxies in a cluster environment.
Introduction
There are a number of environmental effects in clusters of galaxies that modify spiral galaxies causing their HI deficiency, Hα spatial truncation and distortions, as well as strong dynamical and morphological evolution[1]. They influence also galactic magnetic fields, which can be stretched and compressed while the distribution of the ISM is being changed. The Virgo Cluster is the best system to study such processes due to its proximity and large spiral galaxy content. In this work we investigate galaxy–galaxy and galaxy–ICM interactions in the Virgo Cluster in the radio and in the soft X-ray bands. We make use of the VLA and Effelsberg 100-m radio telescope to obtain high sensitivity for the extended total power and polarized nonthermal radio emission.
The radiative transfer code STOKES was extended to allow for X-ray polarimetry modelling. The physical mechanisms of Compton scattering, photo-absorption, and the production of iron K lines were added and are illustrated by modelling the X-ray polarization spectrum of irradiated, cold matter disks. These models confirm that the orientation of the polarization position angle is related to the size of the disk. Although strongly diminishing the spectral flux, an obscuring torus around a small irradiated disk significantly increases the polarization at intermediate viewing angles. Our modelling shows that the polarization can be very sensitive to the radiative coupling between different reprocessing regions.
Introduction
Polarimetry and spectropolarimetry are an important extension of photometry and spectroscopy techniques. In addition to the spectral intensity, i.e. the first Stokes parameter, the linear polarization percentage, P, and position angle, ψ, can provide further information about the geometry and the dynamics of a given object. To decode this information, accurate modelling is necessary. For this purpose I started the development of the radiative transfer code STOKES that is based on the Monte-Carlo method and that computes the polarization spectrum due to multiple photon-matter interactions in geometrically complex environments. The code is publicly available on the web. New versions of STOKES will be subsequently provided for download after they have been carefully tested and documented. The code has recently been extended to include polarization effects that are relevant in the X-ray range.
The advent of a new generation of X-ray polarimeters based on the photoelectric effect poses the problem of their calibration. We devised and built a calibration facility aimed at the study of the performances of photoelectric X-ray polarimeters such as the Gas Pixel Detector (GPD). The calibration facility exploits the 45° Bragg diffraction from crystals of both X-ray lines characteristic of X-ray tubes and from continuum. A set of linear and rotary stages allows the GPD to be calibrated on its whole surface. We successfully tested the GPD filled with a mixture of He-DME 30-70 at one atmosphere. We measured the modulation factor at 2.69 keV and 4.51 keV. We also studied the homogeneity of the modulation factor, of the angular phase and of the position reconstruction capability on the surface of the GPD.
Introduction
Since early 2000 we have been developing true 2-D X-ray polarimeters based on the photoelectric effect. The Gas Pixel Detector (GPD), an evolution based on the use of an ASICCMOS readout chip, has been calibrated at energies greater then 5 keV with a Thomson based X-ray polarizer. However, the sensitivity of the GPD at the focus of conventional X-ray optics peaks below 5 keV. In this regime the photoelectric effect severely competes with Thomson scattering. For this reason we developed a facility aimed at the production of polarized X-rays in the few keV band.
We developed an instrument design capable of measuring linear X-ray polarization over a broad band using conventional spectroscopic optics. A set of multilayer-coated flats reflects the dispersed X-rays to the instrument detectors. The intensity variation with position angle is measured to determine three Stokes parameters: I, Q, and U – all as a function of energy. By laterally grading the multilayer optics and matching the dispersion of the gratings, one may take advantage of high multilayer reflectivities and achieve modulation factors >50% over the entire 0.2–0.8 keV band. This instrument could be used in a small orbiting mission or scaled up for the International X-ray Observatory. Laboratory work has begun that would demonstrate the capabilities of key components.
Introduction
The soft X-ray band (0.1–1.0 keV) should prove to be a fruitful region to explore for polarized emission. One concept, the Polarimeter for Low Energy X-ray Astrophysical Sources (PLEXAS), proposed the use of multilayer-coated mirrors tuned to 0.25 keV as Bragg reflectors. As in similar Bragg reflection systems, the PLEXAS design had a narrow bandpass, reducing its attractiveness for astrophysical observations because one expects polarization to be energy dependent, so a wide bandpass is desired.
Marshall described a method to overcome this limitation by using transmission gratings to disperse in the incoming X-rays. Following up on this approach, Marshall suggested an arrangement that can be used in missions ranging from a small explorer to the International X-ray Observatory (IXO).
By
P. V. Rishin, Raman Research Institute, Sadashivanagar, India,
B. Paul, Raman Research Institute, Sadashivanagar, India,
R. Duraichelvan, Roman Research Institute, Sadashivanagar, India,
J. Marykutty, School of Pure and Applied Physics, Mahatma Gandhi University, India,
D. Jincy, School of Pure and Applied Physics, Mahatma Gandhi University, India,
R. Cowsik, McDonnell Center for the Space Sciences, Department of Physics, Washington University, St. Louis
We describe the current status of the design and development of a Thomson X-ray polarimeter suitable for a small satellite mission. Currently we are considering two detector geometries, one using rectangular detectors placed on four sides of a scattering element and the other using a single cylindrical detector with the scattering element at the center. The rectangular detector configuration has been fabricated and tested. The cylindrical detector is currently under fabrication. In order to compensate any pointing offset of the satellite, a collimator with a flat-topped response has been developed that provides a constant effective area over an angular range. We have also developed a double crystal monochromator/polarizer for the purpose of test and calibration of the polarimeter. Preliminary test results from the developmental activities are presented here.
Introduction
A Thomsom X-ray polarimeter experiment has been proposed for a small satellite mission of the Indian Space Research Organization (ISRO). Currently, a laboratory model has been developed. This experiment will be suitable for X-ray polarization measurement of hard X-ray sources like accretion powered pulsars, black hole candidates in low-hard states etc. For about 50 brightest X-ray sources a minimum detectable polarization of 2–3% will be achieved with the final configuration.
Two configurations are considered based on the geometry of the detector element: (1) rectangular detectors and (2) cylindrical detectors. The X-ray polarization will be measured by spinning the platform around the viewing axis. In both the cases, energy range covered will be 5–30 keV.
There are two kinds of gamma-ray burst (GRB) afterglows. One is the fireball afterglow that is the radiation of the external shock(s) driven by the GRB remnant. The other is the emission from the late ejecta launched by the prolonged activity of the central engine, i.e. the central engine afterglow. The former seems to be only weakly polarized and thus is not suitable for the upcoming X-ray polarimetry. For the latter, the polarization property is less clear. Some central engine afterglows, such as energetic flares and the plateau followed by a sharp drop, might be highly polarized because the outflows powering these behaviors may be Poynting-flux dominated. Furthermore, the breakdown of the symmetry of the visible emitting region may be hiding in some X-ray data and will give rise to interesting polarization signatures. For example, in the high latitude emission model for the sharp X-ray decline strong polarization evolution is possible. An XRT-like detector but with polarization capability on board a Swift-like satellite would be suitable to detect these possible signals.
The central engine afterglow
In the context of the standard fireball model of GRBs, the prompt γ-rays and the afterglow emission are powered by internal shocks and external shocks, respectively (see for a review). Before 2004, most of the afterglow data were collected hours after the prompt γ-ray emission and were found to be consistent with the external forward shock model, though at times energy injection, a wind medium profile, or a structured/patchy jet were needed.
The degree and the temporal evolution of linear polarization in the prompt and afterglow emission of gamma-ray bursts is a very robust diagnostic of some key features of gamma-ray-burst jets and their micro and macro physics. In this contribution, I review the current status of the theory of polarized emission from GRB jets during the prompt, optical flash, and afterglow emission. I compare the theoretical predictions to the available observations and discuss the future prospects from both the theoretical and observational standpoints.
Introduction
Gamma-ray bursts (GRBs) are the brightest explosions in the present day Universe. Unfortunately, our understanding of their physics is still incomplete, probably due to the fact that they are short-lived, point-like sources.
Polarization is a formidable tool to improve our understanding of GRB jets: their geometry, magnetization, and radiation mechanism could in principle be pinned down with a comprehensive and time-resolved analysis of linear polarization. Observationally speaking, however, polarization is not easy to measure. So far, only the optical afterglow has robust polarization measurements but the diverse features and the sensitivity of the models to detail has made their interpretation, at best, controversial.
In this review, I describe the theory underlying the production of polarized radiation in GRBs in their three main phases. I will focus on X-ray polarization but the discussion will be general, since the frequency dependence of GRB polarization is very weak, especially at frequencies where Faraday rotation is not relevant.