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Spotting the life of stars

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on behalf of the Pi of the Sky collaboration 'Pi of the Sky' goal is ... Photometric data flown home every~ 3 months. An astronomical pipeline ... – PowerPoint PPT presentation

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Title: Spotting the life of stars


1
Spotting the life of starsPi of the Sky Project
  • Katarzyna Kwiecinska
  • UKSW-SNS
  • on behalf of the Pi of the Sky collaboration

2
Pi of the Sky goal is
  • to investigate objects of the variability
    timescale from seconds to years. Especially
  • to look for optical counterparts of GRB
    afterglows
  • GRB are short (0.01-100s) impulses
  • They are emitted by extragalactic sources
  • They can originate from supernovae explosions
    (collapse to a black hole), neutron stars
    collisions, etc
  • Nowadays satellites record 2-3 GRB per month and
    send alerts via GRB Coordinate Network

3
Pi of the Sky
  • Taking so many exposures we can observe many
    other astronomical phenomena like
  • Variable stars
  • Meteors, etc.

4
Pi of the Sky apparatus
5
Data flow
6
Data flow
  • 2 cams x 3000 exposures x 8 MB50 GB/night
  • First and Second Level Triggers implemented
  • 20 000 stars per image (30 000 on co added
    images)
  • 120 000 000 photometric measurements/night
  • Raw data accessible for 5 days
  • After reduction 2 GB/night
  • Photometric data flown home every 3 months

7
An astronomical pipeline
  • Obtaining a light curve of a star requires
    several steps of analysis on each frame.

8
Reduction. Its goal is to reduce an apparatus
effects. In general it consists of two steps
  • A dark frame subtraction. It allows to reduce
    effect of a dark current accumulating in CCD
    pixels. The dark frame is obtained by exposing a
    chip with a closed shutter.
  • A flat-field frame division. It permits to
    correct a lens optics. In general the flat-field
    frame is obtained by exposing the chip to a
    source of homogeneous light for example by
    taking sky pictures at dusk. Unfortunately, it is
    not a good method for large FOV because of a
    brightness gradient. So our flat-field is
    obtained from a median of frames taken at the
    same night with a fixed mount.

9
Photometry
  • It creates a list of stars occurring on the
    frame at coordinates (x,y) and calculates their
    instrumental brightness. The instrumental
    brightness is simply a sum of pixel values in a
    certain pre-defined neighborhood of a star,
    called aperture, minus the background level.

10
Astrometry
  • It compares the list of stars in instrumental
    coordinates (x,y) witha star catalogue and finds
    transformations of instrumental coordinates into
    the physical coordinates on the sky. Then it
    calculates the celestial coordinates of each
    star on the frame.

11
Cataloguing
  • It calibrates the instrumental brightness by
    comparing results for certain number of reference
    stars, and determines the physical brightness, or
    magnitudo, of each star on the frame.

12
Visualization - Data Base
13
Sigma vs. magnitudo
14
Effective FOV
15
Effective FOV
  • ?

16
Effective FOV
  • 33 x 33 CCD
  • 29 x 29 taking into account the mount drift
    and the mask
  • 28 x 28 if we want to compare two nights

17
Light curves
18
Conclusions
  1. Because of the mount drift and the shift between
    succeeding nights, effective FOV is about 5 deg
    smaller from each side of a frame.
  2. Imperfect cataloguing procedure makes that mean
    magnitudo depends significantly on time. It is of
    importance especially when we talk about
    long-period stars.
  3. If we want to distinguish a physical variability
    from the imperfect cataloguing effect, it is
    necessary to make the photometry much more
    stable.

19
  • The end.
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