The 3Pi Steradian Survey (as described in Chambers et al. 2016)

The Pan-STARRS telescope surveyed the sky in several different areas using various observing strategies.  The 3PI survey covers the 30,000 deg2 (3 steradians) of sky north of Declination -30º in 5 filters (grizy) with approximately 10 exposures per filter to a combined depth of approximately 21-23 mag.   Data were taken over the period  between 2009-06-02 and 2014-03-31. The Medium Deep Survey covers 10 fields, each about 7 deg2, with hundreds to thousands of exposures per filter to reach a combined depth of 24–26 mag. Other secondary surveys (M31 survey, ecliptic plane survey, celestial north pole) also were carried out.  The initial PS1 data release includes only the 3PI survey, but other data will be released as processing is completed.

The 3π survey pattern and scheduling followed two different strategies over the course of the  survey: the initial pattern layed out in the Design Reference Mission (DRM) Chambers & Denneau (2008) followed by the Modified Design Reference Mission (MDRM). We switched to MDRM on 2012-01-14. All exposures in the DRM were taken in pairs, with each exposure separated by a Transient Time Interval or TTI of 12 to 24 minutes, check for the purpose of detecting moving objects within the Solar System. These were referred to as “TTI pairs”.

The original plan was then to take 2 TTI pairs over an observing season with gri taken within the same lunation and separated by days to weeks. The z and y  were to be taken approximately 6 months apart to optimise stellar parallax and proper motion measurements (for low mass stars). Over 3.5 years this would give (allowing for weather interruptions) 12 exposures in each band or 60 in total over all 5 filters. In the MDRM, a series of 4 exposures, “quads”, all separated by approximately 15 minutes (therefore completed within about 1hr), were implemented for about half of the gri exposures with the express purpose of increasing the recovery of Near Earth Objects (NEOs). The relative exposure times in each were also chosen to make an asteroid of mean solar color  to have approximately the same signal-to-noise.

The exposure times for each individual exposure was as follows (e.g. a TTI pair in g is composed of 2 x 43 sec exposures, separated by 12 to 24 mins)

 

grizy
4340453030

There are typically a dozen pointings at each point of the sky in each filter over the course of the whole 3Pi survey.  The pointing centers are dithered to enable the construction of a seamless image that fills in regions of bad pixels in most parts of the sky.  The table below shows the mean number of pointings and its rms variation over the whole survey as a function of band.

grizy
9.6±3.011.8±3.817.4±6.911.2±3.011.7±3.2

Below is a histogram showing the coverage distributions per summary stack pixel (blue - g; green - r; red - i; black - z; purple - y)

 

PS1 has a floor to its image quality, arising from the wide field optics, so even the best images do not have a FWHM < 0.6".  The image quality also depends on the filter, with the reddest bands displaying the best. Figure 15 shows the cumulative distribution of the image quality as characterized by a FWHM for each filter for the PS1 Surveys.

 

FWHM cumulative probability distribution for all the observations in 3Pi survey  (from (Chambers et al, 2016)

 Cumulative probability distribution  for  the  sky  brightness  in  mag/arc2 for  all  the  observations  in  the  3pi  Survey. (from (Chambers et al, 2016)

 

The Table of 3Pi survey characteristics is taken from Chambers et al. 2016 and reproduced here for information. 

 

 

 

The 5σ point source depth is given in the table below for both the individual exposures and the stacked image sum.

Image Datag limitr limiti limitz limity limit
Single epoch22.222.021.520.819.8
Stacked sum23.423.222.722.021.1

Saturation occurs roughly at point source magnitudes of 14.5, 15, 15, 14, 13 for grizy respectively [Source: N. Metcalfe, priv. comm. - needs checking]

Medium Deep Survey

The 10 fields in the Medium Deep Survey are described below.  Each field was observed several times a night during the months of the year when it was observable.  In total there are hundreds to thousands of exposures in each of the 5 filters (grizy), enabling the construction of very deep stacked images. The depth of individual exposures is the same as for the 3PI survey in the table above; the depth of the stacked image sum is shown below. The MDS data will be released at  later date and more information will follow on these data. 

Observing Strategy

Observations of 3-5 MD filelds are taken each night and the lters are cycled through in the pattern:g and r in the same night (dark time), followed by i and z on the subsequent second and third night, respectively. Around full moon only y data are taken. An epoch consists of 8 dithered exposures of 8 times 113 seconds for g and r or 8 times 240 seconds for the other three (i,z, and y), giving nightly stacked images of 904 and 1920 seconds duration.

Field description

NameAlt NameRA (deg)Dec (deg)g limitr limiti limitz limity limitRA (J2000)Dec (J2000)Comment
PS1MD01XMM-LSS-DXS/VVDS-02h35.875-4.25025.925.826.025.624.302 23 30-04 15 00Multi-wavelength Survey Field
PS1MD02CDFS/GOODS/GEMS53.100-27.80025.625.425.825.324.103 32 24-27 48 00Multi-wavelength Survey Field
PS1MD03IFA/Lynx130.592+44.31725.825.826.025.624.308 42 22+44 19 00Radio Survey Field
PS1MD04COSMOS150.000+2.20025.825.725.825.424.010 00 00+02 12 00Multi-wavelength Survey Field
PS1MD05Lockman-DXS161.917+58.08325.825.725.925.423.910 47 40+58 05 00Multi-wavelength Survey Field
PS1MD06NGC 4258185.000+47.11725.825.625.925.323.912 20 00+47 07 00H20 Maser
PS1MD07DEEP2 Field 1/Extended Groth Strip213.704+53.08325.825.725.925.424.114 14 49+53 05 00Multi-wavelength Survey Field
PS1MD08ELAIS-N1-DXS242.787+54.95025.925.826.025.424.216 11 09+54 57 00Multi-wavelength Survey Field
PS1MD09SA22-DXS/VVDS-22h334.188+0.28326.025.926.125.624.122 16 45+00 17 00Multi-wavelength Survey Field
PS1MD10DEEP2-Field3352.312-0.43325.925.826.125.624.123 29 15-00 26 00Multi-wavelength Survey Field

The detection limits come from a 2015 January analysis by Nigel Metcalfe and will probably change in the final processing.  They are 5-sigma point source detection limits calculated from the databases by measuring (roughly) where psfflux_err/psfflux=0.2.

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