the x ray imaging polarimeter explorer giorgio mat univ
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The X-ray Imaging Polarimeter Explorer Giorgio Mat Univ. Roma Tre, Italy on behalf of the XIPE Study Science Team www.isdc.unige.ch/xipe Why X-ray polarimetry? Introductjon Informatjon on celestjal (extra-solar) sources are mostly provided


  1. The X-ray Imaging Polarimeter Explorer Giorgio Mat Univ. Roma Tre, Italy on behalf of the XIPE Study Science Team www.isdc.unige.ch/xipe

  2. Why X-ray polarimetry? Introductjon Informatjon on celestjal (extra-solar) sources are mostly provided by electromagnetjc radiatjon. They can be obtained by studying the spatjal, spectral, tjming and polarizatjon propertjes of the observed radiatjon. In partjcular, the polarizatjon propertjes give us informatjon on geometry (in a broad sense: geometry of the emittjng mater but also of magnetjc and gravitatjonal fjelds, of space-tjme, etc.): the polarizatjon degree depends on the level and type of symmetry of the system, the polarizatjon angle indicates its orientatjon. Our knowledge of the emission from a celestjal source in a certain energy band is therefore incomplete without polarimetry. However, polarimetric informatjons of astrophysical sources are basically missing in the X-ray band !

  3. Why X-ray polarimetry? Introductjon Polarimetry has proved very important in radio, IR and optjcal bands (eg. jet emission in blazars, Unifjcatjon Model of AGN, ...). In X-rays, where non-thermal emission processes and aspherical geometries are likely to be more common than at lower energies, polarimetry is expected to be vital to fully understand emittjng sources. However, only one measurement (P=19% for the Crab Nebula, indicatjng synchrotron emission) has been obtained so far, together with a tjght upper limit to Sco X-1. These measurements have been obtained in the 70s, for the two brightest sources in the X-ray sky. The lack, for many decades, of signifjcant technical improvements implied that no polarimeters were put on board of X-ray satellites.

  4. Why X-ray polarimetry? Why XIPE? The situatjon has changed dramatjcally with the advent of polarimeters based on the photoelectric efgect. Such detectors, on the focal plane of a X-ray telescope, may provide astrophysically interestjng measurements for hundreds of sources (remember that polarimetry is a photon hungry technique...). The brightest specimens of all major classes of X-ray sources are now accessible! Time is ripe for a X-ray polarimetric mission ! Indeed, a X-ray polarimeter was part of the focal plane suite of detectors of XEUS/IXO, but it did not survive the severe descooping towards Athena. A X-ray polarimetric mission, GEMS, was approved by NASA as a SMEX but later cancelled for programmatjc reasons. And fjnally, XIPE has been selected for a phase A study in ESA M4 (together with Ariel, devoted to exoplanets, and Thor, a solar magnetosphere mission; fjnal down-selectjon in Spring 2017). XIPE will perform spectrally-, spatjally- and tjme-resolved polarimetry of hundreds of celestjal sources to provide a breakthrough in astrophysics and fundamental physics

  5. Why X-ray polarimetry? XIPE goals A large community involved (as for the proposal): Astrophysics Acceleratjon phenomena 17 countries Pulsar wind nebulae SNRs Jets 146 scientjsts Emission in strong magnetjc fjelds Magnetjc cataclysmic variables 68 instjtutes around the world Accretjng millisecond pulsars Accretjng X-ray pulsars Magnetars Scatering in aspherical situatjons X-ray binaries Radio-quiet AGN X-ray refmectjon nebulae Fundamental Physics Mater in Extreme Magnetjc Fields: QED efgects Mater in Extreme Gravitatjonal Fields: GR efgects Galactjc black hole system & AGNs Quantum Gravity Search for axion-like partjcles XIPE will observe almost all classes of X-ray sources

  6. XIPE scientjfjc goals Astrophysics: Acceleratjon: PWN - The Crab Pulsar Infrared (Keck) Optjcal (Palomar) X-rays (Chandra) Radio (VLA) ? P=19% integrated over the entjre nebula (Weisskopf et al. 1978) IR polarisatjon Optjcal polarisatjon X-ray polarisatjon Radio polarisatjon X-rays probe freshly accelerated electrons and their acceleratjon site.

  7. XIPE scientjfjc goals Astrophysics: Acceleratjon: PWN 20 ks with XIPE • The OSO-8 observatjon, integrated over the entjre nebula, measured a positjon angle that is tjlted with respect to the jets and torus axes. • What is the role of the magnetjc fjeld (turbulent or not?) in acceleratjng partjcles and forming structures? • XIPE imaging capabilitjes will allow us to measure the pulsar polarisatjon by separatjng it from the much brighter nebula emission. • Other PWN, up to 5 or 6, are accessible for larger exposure tjmes (e.g. Vela or the “Hand of God”).

  8. XIPE scientjfjc goals Astrophysics: Acceleratjon: SNR Map of the magnetjc fjeld Spectral imaging allows to separate the thermalised plasma from the regions where shocks accelerate partjcles. What is the orientatjon of the magnetjc fjeld? How ordered is it? The spectrum cannot tell… 4-6 keV image of Cas A blurred with the PSF of XIPE 2 Ms observatjon with XIPE

  9. XIPE scientjfjc goals Astrophysics: Acceleratjon: Unresolved Jets in Blazars Schematjc view of an AGN ➡ Blazars are those AGN which not only have a jet (like all radiogalaxies), but it is directed towards us. Due to a Special Relatjvity efgect (aberratjon), the jet emission dominates over other emission components

  10. XIPE scientjfjc goals Astrophysics: Acceleratjon: Unresolved Jets in Blazars Blazars are extreme accelerators in the Universe, but the emission mechanism is far Sync. Peak IC Peak from being understood. In inverse Compton dominated Blazars, a XIPE observatjon can determine the origin of the seed photons: • Synchrotron-Self Compton ( SSC ) ? The polarizatjon angle is the same as for the synchrotron peak. • External Compton ( EC ) ? The polarizatjon angle may be difgerent. The polarizatjon degree determines the electron temperature in the jet. XIPE XIPE XIPE XIPE XIPE band band band band band

  11. XIPE scientjfjc goals Astrophysics: Acceleratjon: Unresolved Jets in Blazars Blazars are extreme accelerators in the Universe, but the emission mechanism is far Sync. Peak Sync. Peak Sync. Peak Sync. Peak Sync. Peak Sync. Peak Sync. Peak Sync. Peak Sync. Peak IC Peak IC Peak IC Peak IC Peak IC Peak IC Peak IC Peak IC Peak IC Peak from being understood. In synchrotron-dominated X-ray Blazars, multj- λ polarimetry probes the structure of the magnetjc fjeld along the jet. Models predict a larger and more variable polarisatjon in X-rays than in the optjcal. Coordinated multj-wavelength campaigns are crucial for blazars. Such campaigns (including polarimetry) are routjnely organised and it will be XIPE XIPE XIPE XIPE XIPE easy for XIPE to join them. band band band band band

  12. XIPE scientjfjc goals Astrophysics: Acceleratjon: Resolved Jets in Radiogalaxies In nearby, non-blazar radiogalaxies, the jet may be resolved. XIPE can map the X-ray polarisatjon and thus the magnetjc fjeld of resolved X-ray emittjng jets. MDP for the jet of Centaurus A is 5% in 1 Ms in 5 regions. The extended (4’) radio jet in Cen A.

  13. XIPE scientjfjc goals Astrophysics: Strong Magnetjc Fields: Cataclysmic variables Accretjon in Magnetjc Cataclysmic Variables occurs in accretjon column. Main emission process is thermal bremsstrahlung, but scatuering may be relevant. Polarizatjon gives informatjons on the accretjon mode (Matu 2004; Matu 2004 McNamara et al, 2008)

  14. XIPE scientjfjc goals Astrophysics: Strong Magnetjc Fields: Accretjng Millisecond Pulsars Emission due to scatuering in hot spots ⇒ Phase-dependent linear polarizatjon Viironen & Poutanen 2004

  15. XIPE scientjfjc goals Astrophysics: Strong Magnetjc Fields: Accretjng X-ray Pulsars Opacity in highly magnetjzed plasma ⇒ k ⊥ ≠ k∥ Phase-dependent linear polarizatjon From the (phase-resolved) swing of the polarisatjon angle : Orientatjon of the rotatjon axis and inclinatjon of the magnetjc fjeld (required for many purposes, e.g. measure of mass/radius relatjon) Meszaros et al. 1988

  16. XIPE scientjfjc goals Astrophysics: Strong Magnetjc Fields: Accretjng X-ray Pulsars “Fan” vs. “Pencil” beam Meszaros et al. 1988

  17. XIPE scientjfjc goals Astrophysics: Scatering: Coronae in X-ray binaries & AGN The geometry of the hot corona, considered to be responsible for the (non-disc) X-ray emission in binaries and AGN, is largely unconstrained. The geometry is related to the corona origin: • Slab – high polarisatjon (up to more than 10%): disc instabilitjes? • Sphere – very low polarisatjon: aborted jet?

  18. XIPE scientjfjc goals Astrophysics: Scatering: Coronae in X-ray binaries & AGN The geometry of the hot corona, considered to be responsible for the (non-disc) X-ray emission in binaries and AGN, is largely unconstrained. SLAB The geometry is related to the corona origin: SPHERE • Slab – high polarisatjon (up to more than 10%): disc instabilitjes? • Sphere – very low polarisatjon: aborted jet? Marin & Tamborra 2014

  19. XIPE scientjfjc goals Astrophysics: Scatering: X-ray refmectjon nebulae in the GC Cold molecular clouds around Sgr A* (i.e. the supermassive black hole at the centre of our own Galaxy) show a neutral iron line and a Compton bump → Refmectjon from an external source!?! No bright enough sources are in the surroundings. Are they refmectjng X-rays from Sgr A*? so, was it one million tjmes brighter a few hundreds years ago? Polarimetry can tell!

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