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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.
By
T. Michel, Ecap, University of Erlangen-Nürnberg,
J. Durst, Ecap, University of Erlangen-Nürnberg,
F. Bayer, Ecap, University of Erlangen-Nürnberg,
J. Jakubek, Ieap, Czech Technical University in Prague
We investigated the capability of the hybrid photon counting pixel detector Timepix to measure the degree of linear X-ray polarization between 27 and 84 keV. Due to its ability to measure energy deposition or the detection time in each pixel, both photoelectric effect and Compton scattering in the sensor can be exploited. The analyzing power exploiting photoelectric effect was found to be small compared to X-ray-sensitive CCDs due to the larger pixel pitch (55 μm) of the Timepix. We were able to measure a polarization asymmetry of (0.96±0.02)% between vertical and horizontal double-hit events in neighbouring pixels. The polarization asymmetry was measured with dependence on the energy deposition in the sensor. Asymmetries range between 0.2% at 29 keV and 3.4% at 78 keV. In order to exploit the polarization signature of Compton scattering in the sensor, the time-to-shutter mode of the Timepix was used. We measured a large modulation factor of about 68.1% in good agreement with simulations.
Introduction
It has already been demonstrated that X-ray-sensitive CCDs can be used to measure the degree of linear polarization of X-rays using the effect that photoelectrons are emitted with a nonisotropic angular distribution with respect to the orientation of the electric field vector of impinging photons. Up to the last year hybrid semiconductor pixel detectors like the Timepix-detector have never been used for X-ray polarimetry. The main reason for this is that the pixel pitch is large compared to CCDs which results in a much smaller analyzing power.
ASTRO-H is a next-generation JAXA X-ray satellite to be launched in 2014. The Soft Gamma-ray Detector (SGD) onboard ASTRO-H is a semi-conductor Compton camera with a narrow field-of-view (FOV) to achieve very low background. Although the SGD is primarily a spectrometer in the 40–600 keV energy band, it is also sensitive to polarization in the 50–200 keV energy band. This paper describes instrument design, expected performance, and experimental validation of polarimetric performance of the SGD.
Introduction
ASTRO-H, the new Japanese X-ray Astronomy Satellite following Suzaku, is a combination of
high energy-resolution soft X-ray spectroscopy (0.3–10 keV) provided by thin-foil X-ray optics (SXT, Soft X-ray Telescope) and a microcalorimeter array (SXS, Soft X-ray Spectrometer);
soft X-ray imaging spectroscopy (0.5–12 keV) provided by SXT and a CCD (SXI, Soft X-ray Imager);
hard X-ray imaging spectroscopy (3–80 keV) provided by multi-layer coating, focusing hard X-ray mirrors (HXT, Hard X-ray Telescope) and silicon (Si) and cadmium telluride (CdTe) cross-strip detectors (HXI, Hard X-ray Imager);
soft gamma-ray spectroscopy (40–600 keV) provided by semiconductor Compton camera with narrow FOV (SGD, Soft Gamma-ray Detector).
The SXT-SXS and SGD systems will be developed by an international collaboration led by Japanese and US institutions.
The SXS will use a 6×6 format microcalorimeter array. The energy resolution is expected to be better than 7 eV. The FOV and the effective area will be, respectively, about 3 arc minutes and about 210 cm2 combined with the ∼6 m focal-length SXT.