[an error occurred while processing this directive] IPHAS: Imaging Data [an error occurred while processing this directive]

Accessing IGAPS images

This server provides access to the entire collection of pipeline-reduced images that have been obtained as part of the IPHAS and UVEX surveys of the northern Galactic Plane. The data set consists of 527 760 CCD frames obtained between 2003 and 2018. The g, r, i and Hα frames that have undergone uniform calibration as part of the construction of the IGAPS point source catalogue number 349 175. The volume occupied by the compressed images is 3.0 TB. This page also provides the associated metadata and documents the use of the images.

Note that the raw telescope data and the calibration frames are not available here, they may be found in the Isaac Newton Group Archive instead. The raw and processed data are also available through the CASU dqc interface.

Use the form below to retrieve a list of IPHAS CCD frames at a given position.

Search by coordinates
Search by object name

Direct access

CCD frames may also be downloaded directly from our server. Each frame is uniquely identified by the combination of its run number, which identifies the exposure, and the CCD number, which identifies the detector within the INT/WFC camera used by the survey (i.e. CCD number 1, 2, 3 or 4). The run and CCD numbers for a desired position or epoch may be found in the metadata table provided below. They may also be found in the "detectionID" columns of the source catalogue, which are in the form "#RUN-#CCD-#SOURCE".

When the numbers of a desired frame are known, the URL of the image is composed as follows:

http://www.igapsimages.org/data/images/r{first 3 digits of #RUN}/r{#RUN}-{#CCD}.fits.fz

For example, the image for a source with rDetectionID equal to "570144-1-5487", i.e. detected in run 570144 by CCD 1, is located at:

http://www.igapsimages.org/data/images/r570/r570144-1.fits.fz

Note that the images are compressed using the Rice algorithm. Although this compression scheme is supported by professional software such as DS9 and Aladin, it is not supported by every FITS viewer yet. If you struggle to open an image, try to decompress it using funpack first.

Note: this data set includes all the images obtained during our observing runs, including those that were affected by poor conditions (e.g. clouds, bad seeing, electronic noise). You should verify the quality of the images using the metadata provided below. We recommend that, as far as possible, you avoid images for which the qcgrade equals "D".

A table detailing the run numbers, ccd numbers, sky coordinates, observing dates, conditions and quality information is available for download in FITS format:

Columns

The columns in the metadata table are as follows:

Column Unit Description
run Number of the exposure, corresponding to the run number found in the observing logs of the Isaac Newton Telescope (INT).
ccd Number of the CCD of the INT Wide Field Camera (1, 2, 3, or 4).
url URL of the FITS file containing the image, e.g. "http://www.igapsimages.org/data/images/r534/r534002-2.fits.fz".
ra degrees Right Ascension (J2000) in the centre of the frame, i.e. at pixel position (x,y)=(1024,2048).
dec degrees Declination (J2000) in the centre of the frame, i.e. at pixel position (x,y)=(1024,2048).
band Waveband of the filter used. One of "r", "i", or "halpha".
utstart Universal Time (UTC) at the start of the exposure, given as a ISO 8601 timestamp (e.g. "2003-08-08T22:07:10.4").
fieldid Internal IGAPS identifier for the observation composed of the field number and the observing month, e.g. "0001o_aug2003".
2020 Boolean column to indicate if the image was used in the construction of the IGAPS catalogue (Monguio et al 2020).
calibrated Boolean column, true if the exposure passed all the quality control criteria and was selected for inclusion in the IGAPS Catalogue Release. When this column is set to false, it is likely that the frame suffers from severe quality problems (e.g. clouds).
qcgrade IGAPS quality score. One of "A++", "A+", "A", "B", "C" or "D". D-graded data is generally unsuited for quantitative scientific use due to e.g. clouds or electronic noise in the image.
qcproblems Brief description of the issues encountered during quality control.
exptime seconds Exposure time adopted.
seeing arcsec Average Full Width at Half Maximum (FWHM) of point sources in the CCD frame.
ellipticity Average ellipticity of point sources in the CCD frame, defined as e = (1 - b/a) with b the semi-minor and a the semi-major axis.
skylevel counts/pixel Median sky brightness. An automatic 2D background-following algorithm is used to track and "remove" slowly varying background features such as image gradients etc.
skynoise counts/pixel Pixel noise at sky level, estimated using a robust MAD estimator for noise scaled to equivalent Gaussian rms value, ie. = MAD x 1.48, after removing large scale sky background variations. MAD = Median of the Absolute Deviations about the median.
airmass The airmass (sec z) of the observation.
moon_phase The phase of the moon expressed as a fraction, with 1.0 as full moon and 0.0 as new moon.
moon_separation degrees The angle between the moon and telescope pointing.
moon_altitude degrees The height of the moon above the horizon at time of image acquisition, expressed as an angle. A negative value indicates the moon was below the horizon.
depth mag 5-sigma limiting magnitude in the Vega system.
photzp mag Photometric zeropoint, computed such that it absorbs the required corrections for atmospheric extinction, gain variations, exposure time, and the IGAPS re-calibration shift (included only if the frame was part of the IGAPS release). See section on flux calibration below.
stdps mag. Only given for 2020 calibrated g,r,i data. This magnitude is the standard deviation around the photometric offset measured between the pipeline-calibrated IGAPS point source data for the CCD and the equivalent data from PanSTARRS. Where (in a very small number of cases) this is given as 9999.0, it could not be determined because of e.g. a very bright star flooding the CCD.
confmap Filename of the confidence map, relative to their location on the IPHAS server: http://www.igapsimages.org/data/images/confmaps
ra_min degrees Right Ascension (J2000) in the western-most corner of the CCD frame.
ra_max degrees Right Ascension (J2000) in the eastern-most corner of the CCD frame.
dec_min degrees Declination (J2000) in the southern-most corner of the CCD frame.
dec_max degrees Declination (J2000) in the northern-most corner of the CCD frame.

Quality grades

The metadata table explained above provides essential quality information such as the seeing, ellipticity, skylevel, and skynoise. The quality of each image is summarised in the qcgrade column, which classifies images as "A", "B", "C", or "D":

  • "A"-graded images were found to meet all our quality criteria;
  • "B"- and "C"-graded images do not meet the criteria in a strict sense, but may nevertheless be adequate for a range of scientific applications. For example, this category includes images that were obtained under sub-standard seeing (2 to 2.5 arcsec), but are fine otherwise.
  • "D"-graded images were not used in building the catalogue due to significant quality concerns.

Although the use of D-graded images is generally discouraged, we note that the quality grades were assigned on a field-by-field basis. That is, each trio of exposures of a field were given a single quality grade based on their combined properties. Hence, the D-graded category does contain some single-band exposures which are perfectly fine, but were graded poorly because of a problem in a different filter.

Some fields in the survey footprint were observed more than once to improve data quality. The best-available data for each field are flagged by the calibrated column, which marks the exposures that were used to compile the point-source catalogue. These are also the only exposures for which the photometric zeropoints are calibrated in a global sense to an accuracy of 0.03 mag (see Monguio et al 2020).

Header keywords

Useful keywords in the image headers include:
Keyword Description
RUN Unique exposure number. Corresponds to the run number found in the observing logs of the Isaac Newton Telescope.
DATE‑OBS Start time of the exposure in UTC, given in the ISO 8601 format "YYYY-MM-DDTHH:MM:SS".
EXPTIME Exposure time in seconds. This may deviate slightly from the value found in the raw data, because the INT/WFC is known to occasionally record incorrect exposure times in the headers. This has been corrected, as best we can, in the images hosted on the IGAPS website.
PHOTZP Photometric zeropoint, computed such that it absorbs the required corrections for atmospheric extinction, gain variations, exposure time, and the IGAPS re-calibration shift (if computed). Hence, the number counts stored in the images can be converted straight into Vega-based magnitudes using: mag(Vega) = -2.5*log(pixel value) + PHOTZP.
FLUXCAL Certifies the validity of PHOTZP. If set to 'ABSOLUTE' it means that the image has been globally re-calibrated to an accuracy of 0.03 mag (rms). If set to 'UNCALIBRATED' it indicates that the image has only been calibrated using the nightly average zeropoint obtained by observing standard stars, which may or may not be accurate depending on the zeropoint stability during the night. We recommend against using PHOTZP in the latter case.
MAGZPT Original nightly zeropoint for default extinction measured at unit airmass. Obtained by taking the average zeropoint of all standard star fields observed within the same night. Unlike PHOTZP, this value does NOT include the required corrections for atmospheric extinction at the altitude of the observed pointing, gain variations, the exposure time or for the global re-calibration. We do not recommend its use.

A typical header looks as follows:

XTENSION= 'BINTABLE'           / binary table extension
BITPIX  =                    8 / 8-bit bytes
NAXIS   =                    2 / 2-dimensional binary table
NAXIS1  =                    8 / width of table in bytes
NAXIS2  =                 4096 / number of rows in table
PCOUNT  =              5621622 / size of special data area
GCOUNT  =                    1 / one data group (required keyword)
TFIELDS =                    1 / number of fields in each row
TTYPE1  = 'COMPRESSED_DATA'    / label for field   1
TFORM1  = '1PB(1477)'          / data format of field: variable length array
EXTNAME = 'COMPRESSED_IMAGE'   / name of this binary table extension
ZIMAGE  =                    T / extension contains compressed image
ZBITPIX =                   16 / data type of original image
ZNAXIS  =                    2 / dimension of original image
ZNAXIS1 =                 2048 / length of original image axis
RUN     =               484995 / Run number
OBSERVAT= 'LAPALMA '           / Name of observatory (IRAF style)
OBJECT  = 'intphas_3260 i'     / Title of observation
LATITUDE=            28.761939 / Telescope latitude  (degrees), +28:45:43.0
LONGITUD=           -17.877587 / Telescope longitude (degrees), -17:52:39.3
HEIGHT  =                 2348 / [m] Height above sea level.
SLATEL  = 'LPO2.5  '           / Telescope name known to SLALIB
TELESCOP= 'INT     '           / 2.5m Isaac Newton Telescope
MJD-OBS =        53709.1836527 / Modified Julian Date at start of observation
JD      =      2453709.6836527 / Julian Date at start of observation
PLATESCA=             6.856013 / [d/m] Platescale ( 24.68arcsec/mm)
TELFOCUS=             0.043653 / Telescope focus (metres)
AIRMASS =             1.119865 / Effective mean airmass
TEMPTUBE=             7.793302 / Truss Temperature (degrees Celsius)
INSTRUME= 'WFC     '           / INT wide-field camera is in use.
WFFPOS  =                    4 / Position-number of deployed filter
WFFBAND = 'i       '           / Waveband of filter
WFFID   = '215     '           / Unique identifier of filter
SECPPIX =                0.333 / Arcseconds per pixel
DETECTOR= 'WFC     '           / Formal name of camera
CCDSPEED= 'FAST    '           / Readout speed
CCDXBIN =                    1 / Binning factor in x axis
CCDYBIN =                    1 / Binning factor in y axis
CCDSUM  = '1 1     '           / Binning factors (IRAF style)
CCDTEMP =              154.957 / [K] Cryostat temperature
NWINDOWS=                    0 / Number of readout windows
DATE-OBS= '2005-12-05T04:24:30.1' / Start time of the exposure [UTC]
ZNAXIS2 =                 4096 / length of original image axis
ZTILE1  =                 2048 / size of tiles to be compressed
ZTILE2  =                    1 / size of tiles to be compressed
ZCMPTYPE= 'RICE_1  '           / compression algorithm
ZNAME1  = 'BLOCKSIZE'          / compression block size
ZVAL1   =                   32 / pixels per block
BZERO   =       32768.00000000 / Pixel-data have 32K offset.
BSCALE  =           1.00000000 / Pixel-data are not scaled.
INHERIT =                    T / Extension inherits primary HDU.
EXTVER  =                    4 / Extension version number
IMAGEID =                    4 / Image identification
DASCHAN =                    4 / Number of readout channel
WINNO   =                    0 / Number of readout window
CHIPNAME= 'A5382-1-7         ' / Name of detector chip.
CCDNAME = 'A5382-1-7         ' / Name of detector chip.
CCDCHIP = 'A5382-1-7         ' / Name of detector chip.
CCDTYPE = 'EEV42-80          ' / Type of detector chip.
CCDXPIXE=           0.00001350 / [m] Size of pixels in x.
CCDYPIXE=           0.00001350 / [m] Size of pixels in y.
AMPNAME = 'LH                ' / Name of output amplifier.
GAIN    =           2.90000000 / Nominal Photo-electrons per ADU.
READNOIS=           5.80000000 / Nominal Readout noise in electrons.
SATURATE=              56008.0 / Highest value that is unsaturated
MAXBIAS =       65535.00000000 / Maximum expected bias level
BIASSEC = '[11:53,3:4098]'     / Bias pixels.
TRIMSEC = '[54:2101,3:4098]'   / Illuminated pixels.
RTDATSEC= '[-52:2101,1:4200]               ' / Location in d-space for RTD.
HISTORY
HISTORY Updated 2020-03-05
HISTORY ------------------
HISTORY This frame contains pipeline-reduced IGAPS data that was originally
HISTORY processed by the Cambridge Astronomical Survey Unit (CASU), but the
HISTORY headers have been updated following Monguio et al. in 2020
HISTORY to add a re-calibrated zeropoint and to tweak the WCS keywords.
HISTORY
RADESYS = 'ICRS    '           / WCS calibrated against Gaia-DR2
EQUINOX =               2000.0
CTYPE1  = 'RA---ZPN'           / Algorithm type for axis 1
CTYPE2  = 'DEC--ZPN'           / Algorithm type for axis 2
CRUNIT1 = 'deg     '           / Unit of right ascension coordinates
CRUNIT2 = 'deg     '           / Unit of declination coordinates
PV2_1   =                  1.0 / Coefficient for r term
PV2_2   =                  0.0 / Coefficient for r**2 term
PV2_3   =           212.409021 / Coefficient for r**3 term
PV2_5   =                  0.0 / Coefficient for r**5 term
CRVAL1  =             93.72109 / [deg] Right ascension at the reference pixel
CRVAL2  =           21.1490626 / [deg] Declination at the reference pixel
CRPIX1  =           1801.30718 / [pixel] Reference pixel along axis 1
CRPIX2  =           2967.45576 / [pixel] Reference pixel along axis 2
CD1_1   =          -1.2741E-06 / Transformation matrix element
CD1_2   =           -9.244E-05 / Transformation matrix element
CD2_1   =          -9.2439E-05 / Transformation matrix element
CD2_2   =           1.2691E-06 / Transformation matrix element
STDCRMS =   0.0305099337399365 / Astrometric fit error (arcsec)
HISTORY  trimmed to range     :     54  2101     3  4098
HISTORY  linearity LUT applied: /home/mike/pipeline/nonlincoeffs/int_non
HISTORY  bias-corrected with  : bias.fit
HISTORY  flatfielded with     : i_flat.fit
HISTORY  gain-corrected by    :      1.145
DEFRING0= 'Defringe image i_fringe_aug2003.fits scale =    0.0111'
MOONDIST=    152.1999969482422 / Distance to the moon in degrees
MOONALT =   -85.69999694824219 / Altitude of the moon above the horizon
MOONPHAS=    16.29999923706055 / Phase of the moon
SKYLEVEL=                57.02 / Sky level
SKYNOISE=    5.610000133514404 / Sky noise
PERCORR =                   0. / Sky calibration correction (mags)
MAGZPT  =                23.77 / Uncorrected nightly ZP (per second)
MAGZRR  =                 0.05 / Photometric ZP error (mags)
EXTINCT =                 0.09 / Extinction coefficient (mags)
PHOTZP  =              26.3149 / mag(Vega) = -2.5*log(pixel value) + PHOTZP
PHOTZPER=                 0.03 / Default 1-sigma PHOTZP uncertainty in IGAPS
PHOTSYS = 'Vega    '           / Photometric system
FLUXCAL = 'ABSOLUTE'           / Certifies the validity of PHOTZP
SEEING  =             0.897102 / Average FWHM (arcsec)
ELLIPTIC=    0.153999999165535 / Average ellipticity
EXPTIME =                 10.0 / [sec] Exposure time adopted
CONFMAP = 'iphas_dec2005/i_conf.fit'
CHECKSUM= '43Af416e41Ae415e'   / HDU checksum updated 2020-03-05T12:21:38
DATASUM = '908599464'          / data unit checksum updated 2020-03-05T12:21:38
COMMENT ------------------
COMMENT  _____  _____          _____   _____
COMMENT |_   _|/ ____|   /\   |  __ \ / ____|
COMMENT   | | | | ___   /  \  | |__) | (___
COMMENT   | | | ||__ | / /\ \ |  ___/ \___ \
COMMENT  _| |_| |__| |/ ____ \| |     ____) |
COMMENT |_____|\_____|_/    \_\_|    |_____/
COMMENT
COMMENT Data origin
COMMENT -----------
COMMENT This image is part of the INT Galactic Plane Survey
COMMENT (IGAPS).
COMMENT
COMMENT Photometric calibration info
COMMENT ----------------------------
COMMENT The pixel values (number counts) in this image can be converted into
COMMENT Vega-based magnitudes using the PHOTZP keyword as follows:
COMMENT
COMMENT     mag(Vega) = -2.5*log10(pixel value) + PHOTZP.
COMMENT
COMMENT The PHOTZP value has been computed such that it absorbs the required
COMMENT factors for atmospheric extinction, gain variations, exposure time,
COMMENT and the re-calibration shift.
COMMENT As these images still include moonlight and other sources of
COMMENT non-astronomical background, they can only support flux measurements
COMMENT that include a suitably-chosen local background subtraction.
COMMENT
COMMENT Uncompressing the images
COMMENT ------------------------
COMMENT These data are compressed using Rice lossless compression algorithm.
COMMENT This is a standard compression algorithm. Details can be found here:
COMMENT http://heasarc.gsfc.nasa.gov/fitsio/fpack/
COMMENT Compressed images can be opened using ds9.
COMMENT
COMMENT Acknowledgement instructions
COMMENT ----------------------------
COMMENT If you use these data, please cite Monguio et al. (2020) and
COMMENT Greimel et al. (2020).
END

Flux calibration

Each image contains a photometric zeropoint in the FITS header (keyword PHOTZP) which allows the pixel values to be converted into Vega-based magnitudes as follows:

mag(Vega) = -2.5*log10(pixel value) + PHOTZP

The PHOTZP value has been computed such that it absorbs the required corrections for atmospheric extinction, gain variations, exposure time, and the DR2 re-calibration shift (if available).

Note: only the images specifically identified as calibrated have photometric zeropoints that are globally calibrated to a precision of 0.03 mag (rms).

To estimate absolute narrow-band Hα fluxes from the image data, we note that the integrated in-band energy flux for Vega in the WFC narrow-band Hα filter is 1.51 x 10−7 erg cm−2 s−1 at the top of the Earth’s atmosphere, which is the flux obtained by folding the CALSPEC SED with the filter transmission curve only (the correction for atmosphere and detector quantum efficiency, otherwise scales down the narrow-band flux by 0.707). We note that the Hα magnitude for Vega is now set to a value of 0.045 (see table 2 in Monguio et al 2020), implying that the in-band flux corresponding to zero magnitude is:

F(Hα=zero) = 1.57 x 10−7 erg cm−2 s−1
Note: as these images still include moonlight and other sources of non-astronomical background, they can only support flux measurements that include a suitably-chosen local background subtraction.

Astrometry

An astrometric solution for the IGAPS images has been determined by comparing the positions of our stars in all bands against those found in the DR2 release of the Gaia mission. This is a change from IPHAS DR2 where the astrometry was referred to the Two-Micron All Sky Survey (2MASS). All positions are specified in the International Celestial Reference System (ICRS). The Root Mean Square (RMS) residual of our astrometric fit against Gaia DR2 is in most cases appreciably better than 0.1 arcsec (see header keyword STDCRMS).

The astrometric solution is recorded in the FITS headers by means of a series of World Coordinate System (WCS) keywords. IGAPS uses the Zenithal PolyNomial (ZPN) projection, which is required to model the radial distortions in the focal plane (see Calabretta & Greisen, 2002).

An example WCS extracted from an IGAPS image (same as above) is given below. Note that each image contains its own solution. For more detail, see section 4 in Monguio et al (2020).

HISTORY This frame contains pipeline-reduced IGAPS data that was originally
HISTORY processed by the Cambridge Astronomical Survey Unit (CASU), but the
HISTORY headers have been updated following Monguio et al. in 2020
HISTORY to add a re-calibrated zeropoint and to tweak the WCS keywords.
HISTORY
RADESYS = 'ICRS    '           / WCS calibrated against Gaia-DR2
EQUINOX =               2000.0
CTYPE1  = 'RA---ZPN'           / Algorithm type for axis 1
CTYPE2  = 'DEC--ZPN'           / Algorithm type for axis 2
CRUNIT1 = 'deg     '           / Unit of right ascension coordinates
CRUNIT2 = 'deg     '           / Unit of declination coordinates
PV2_1   =                  1.0 / Coefficient for r term
PV2_2   =                  0.0 / Coefficient for r**2 term
PV2_3   =           212.409021 / Coefficient for r**3 term
PV2_5   =                  0.0 / Coefficient for r**5 term
CRVAL1  =             93.72109 / [deg] Right ascension at the reference pixel
CRVAL2  =           21.1490626 / [deg] Declination at the reference pixel
CRPIX1  =           1801.30718 / [pixel] Reference pixel along axis 1
CRPIX2  =           2967.45576 / [pixel] Reference pixel along axis 2
CD1_1   =          -1.2741E-06 / Transformation matrix element
CD1_2   =           -9.244E-05 / Transformation matrix element
CD2_1   =          -9.2439E-05 / Transformation matrix element
CD2_2   =           1.2691E-06 / Transformation matrix element
STDCRMS =   0.0305099337399365 / Astrometric fit error (arcsec)
Note: users of the images should be aware that the astrometry achieved for the URGO band is coarser, with residuals relative to Gaia DR2 (median in CCD4: 79 mas) counterparts almost twice those seen in the longer wavelength bands. Differences in its optical properties, as a liquid Cu2SO4 filter, also lead to higher-order (non-zero PV2_5) distortion within the camera footprint.
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