Basic Principles of X-ray Source Detection - PowerPoint PPT Presentation

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Basic Principles of X-ray Source Detection

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Comparison to X-ray images. Why so few X-rays? What can we do about it? ... normal image, these would completely swamp the sources, but in X-ray astronomy ... – PowerPoint PPT presentation

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Title: Basic Principles of X-ray Source Detection


1
Basic Principles of X-ray Source
Detection Or Who Stole All Our Photons?.....
2
  • Overview
  • Optical sources
  • Comparison to X-ray images
  • Why so few X-rays?
  • What can we do about it?
  • The theory of low count levels
  • Application to X-ray sources
  • Calculating flux and luminosity.

3
Optical Sources
4
X-ray Images
5
Why so few X-rays? - Mirrors PSF
  • Mirrors
  • Made from Zerodur
  • Coated with Iridium
  • 100 reflectivity at 0.1keV
  • 10 reflectivity at 10keV
  • 10m focal length
  • Optical/UV filters remove 20 of low energy
    X-rays.
  • PSF
  • Angular resolution of 0.5 on axis
  • PSF increases rapidly off axis
  • Also a function of energy

6
Why so few X-rays? - Background
99.7 of detections are or could be background
that is of a non cosmic origin.
  • Distant Sources
  • Solar wind 11 year cycle
  • Solar flares short time scale
  • Radiation belt
  • (Cosmic rays)
  • Types of Particle
  • Mostly protons magnets deflect those with
    lowest momentum
  • Heavy ions
  • Neutrons
  • Gamma rays
  • X-rays
  • Local Sources
  • Flaring pixels
  • Detector radiation gold, aluminium, silicon
  • Trailing (only for bright sources)

In a normal image, these would completely swamp
the sources, but in X-ray astronomy we have one
major advantage
7
Why so few X-rays? CCDs
Position - x, y - obvious
Can obtain x, y, E, t and grade
  • Energy
  • 1 electron per 3.7eV
  • Typically 1000 electrons
  • Read noise 2 electrons
  • E/ E 50
  • Energy is summed over the surrounding pixels
    which share the signal.
  • Time of arrival
  • Low count rate
  • 3.2 sec frame time
  • 0.04 sec readout time
  • Fine for most sources (no pileup unless very
    bright)
  • Removes flickering pixels
  • Grade
  • Triggering one pixel will effect those around it
    in a way that depends on the type of particle and
    its incident angle.
  • Therefore looking at the 3x3 region around a peak
    can distinguish between true X-rays and
    background events.

8
Why so few X-rays? Grades and Filters
The 3x3 region around a peak can predict the
cause of the event. If all pixels with a value
above a given threshold are included, the
resulting shape determines the grade. Rejecting
certain grades greatly increases the signal to
noise ratio.
Rejected grades gt Accepted grades gt
  • Probable background events are removed by
    filtering for grade.
  • Events received during times of particularly high
    background are removed.
  • Events with Elt0.5keV or Egt8keV are removed.

9
Source Detection
  • Detect using Wavelets
  • Apertures and annulus defined by wavelet
  • Calculate counts and background
  • Find errors

10
Calculating Flux and Luminosity
  • Select all significant sources
  • Find source counts and error
  • Assume a source spectrum
  • Convert counts to ergs using assumed spectrum
  • Create Exposure Map allowing for Quantum
    Efficiency and source spectrum
  • Convert ergs to ergs/cm2/sec using exposure map
  • Convert to luminosity using distance (requires
    optical astronomers!)
  • Finished!
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