Project Supported by
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NSF, National Science Foundation
KICP, Kavli Institute for Cosmological Physics
USAP, United States Antarctic Program
Raytheon Polar Support Corporation
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Related Websites
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CBI, Cosmic Background Imager
DASI, Degree Angular Scale Interferometer
WMAP, Wilkinson Microwave Anisotropy Probe
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| Overview |
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This page provides data products associated with the point-source catalog from 2530 square degrees of SPT data described in Everett et al. (2020). Linked below are the full three-band source catalog (down to a significance threshold of 4.5 sigma), the differential number counts in each band---total and divided into synchrotron- and dust-dominated counts---and the cumulative number counts in each band.
If you have any questions regarding this data set or its use please contact Wendy Everett (wendeline.everett_at_colorado.edu).
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| Catalog |
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The full 4.5-sigma source catalog at 95, 150, and 220 GHz from Everett et al. (2020) is here .
Column descriptions from Everett et al. 2020:
- Source ID: the IAU designation for the SPT-detected source.
- RA: right ascension (J2000) in degrees.
- DEC: declination (J2000) in degrees.
- S/N (95 GHz): detection significance (signal-to-noise ratio) in the 95 GHz band.
- Sraw (95 GHz): raw flux (uncorrected for flux boosting) in the 95 GHz band.
- Sbest (95 GHz): median value of de-boosted flux at 95 GHz.
- dSup (95 GHz): upper error bar (1-sigma normal equivalent) of de-boosted flux at 95 GHz.
- dSdown (95 GHz): lower error bar (1-sigma normal equivalent) of de-boosted flux at 95 GHz.
- S/N (150 GHz): detection significance (signal-to-noise ratio) in the 150 GHz band.
- Sraw (150 GHz): raw flux (uncorrected for flux boosting) in the 150 GHz band.
- Sbest (150 GHz): median value of de-boosted flux at 150 GHz.
- dSup (150 GHz): upper error bar (1-sigma normal equivalent) of de-boosted flux at 150 GHz.
- dSdown (150 GHz): lower error bar (1-sigma normal equivalent) of de-boosted flux at 150 GHz.
- S/N (220 GHz): detection significance (signal-to-noise ratio) in the 150 GHz band.
- Sraw (220 GHz): raw flux (uncorrected for flux boosting) in the 220 GHz band.
- Sbest (220 GHz): median value of de-boosted flux at 220 GHz.
- dSup (220 GHz): upper error bar (1-sigma normal equivalent) of de-boosted flux at 220 GHz.
- dSdown (220 GHz): lower error bar (1-sigma normal equivalent) of de-boosted flux at 220 GHz.
- alpha95-150raw: estimate (from the raw flux in each band) of the 95 GHz-150 GHz spectral index alpha
- alpha95-150best: median value of spectral index.
- d_alpha95-150up: upper error bar (1-sigma normal equivalent) of spectral index.
- d_alpha95-150down: lower error bar (1-sigma normal equivalent) of spectral index.
- alpha150-220raw: estimate (from the raw flux in each band) of the 150 GHz-220 GHz spectral index alpha
- alpha150-220best: median value of spectral index.
- d_alpha150-220up: upper error bar (1-sigma normal equivalent) of spectral index.
- d_alpha150-220down: lower error bar (1-sigma normal equivalent) of spectral index.
- P(alpha > 1.51): fraction of the spectral index posterior probability distribution above the threshold value of 1.51. A higher value of P means the source is more likely to be dust-dominated.
- Type: source classification ((sync)hrotron- or (dust)-dominated).
- External counterparts: (1): SUMSS, (2): IRAS, (3): AT20G, (4): WISE, (5): PMN, (6): AKARI/FIS, (7): AKARI/IRC, (8): RASS
- Extended flag: flag for extended sources.
- Redshift: cross-matched redshift from NED, if available.
- Cut selection: (1): Ext cut, (2): z cut, (3): SMG list, (4): stars
If you have any questions regarding this data set or its use please contact Wendy Everett (wendeline.everett_at_colorado.edu).
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| Differential Source Counts at 95 GHz |
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The differential number counts as a function of 95 GHz flux from Everett et al. (2020) are here .
Columns in the file are:
- Flux range [low]: Low end of flux bin in which counts were estimated. In units of Jy.
- Flux range [high]: High end of flux bin in which counts were estimated. In units of Jy.
- dN/dS total no cuts, central: Central value of differential counts (in units of number per square degree per Jy) for all sources detected at 95 GHz.
- dN/dS total no cuts, lower error bar: 1-sigma lower error bar for differential counts (in units of number per square degree per Jy) for all sources detected at 95 GHz.
- dN/dS total no cuts, upper error bar: 1-sigma upper error bar for differential counts (in units of number per square degree per Jy) for all sources detected at 95 GHz.
- dN/dS synchrotron z cut, central: Same as [3] for synchrotron-dominated sources detected at 95 GHz.
- dN/dS synchrotron z cut, lower error bar: Same as [4] for synchrotron-dominated sources detected at 95 GHz.
- dN/dS synchrotron z cut, upper error bar: Same as [5] for synchrotron-dominated sources detected at 95 GHz.
- dN/dS dust z cut, central: Same as [3] for dust-dominated sources detected at 95 GHz.
- dN/dS dust z cut, lower error bar: Same as [4] for dust-dominated sources detected at 95 GHz.
- dN/dS dust z cut, upper error bar: Same as [5] for dust-dominated sources detected at 95 GHz.
- Completeness: Average value of completeness across the flux range given by [1] and [2].
If you have any questions regarding this data set or its use please contact Wendy Everett (wendeline.everett_at_colorado.edu).
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| Differential Source Counts at 150 GHz |
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The differential number counts as a function of 150 GHz flux from Everett et al. (2020) are here .
Columns in the file are:
- Flux range [low]: Low end of flux bin in which counts were estimated. In units of Jy.
- Flux range [high]: High end of flux bin in which counts were estimated. In units of Jy.
- dN/dS total no cuts, central: Central value of differential counts (in units of number per square degree per Jy) for all sources detected at 150 GHz.
- dN/dS total no cuts, lower error bar: 1-sigma lower error bar for differential counts (in units of number per square degree per Jy) for all sources detected at 150 GHz.
- dN/dS total no cuts, upper error bar: 1-sigma upper error bar for differential counts (in units of number per square degree per Jy) for all sources detected at 150 GHz.
- dN/dS synchrotron z cut, central: Same as [3] for synchrotron-dominated sources detected at 150 GHz.
- dN/dS synchrotron z cut, lower error bar: Same as [4] for synchrotron-dominated sources detected at 150 GHz.
- dN/dS synchrotron z cut, upper error bar: Same as [5] for synchrotron-dominated sources detected at 150 GHz.
- dN/dS dust z cut, central: Same as [3] for dust-dominated sources detected at 150 GHz.
- dN/dS dust z cut, lower error bar: Same as [4] for dust-dominated sources detected at 150 GHz.
- dN/dS dust z cut, upper error bar: Same as [5] for dust-dominated sources detected at 150 GHz.
- dN/dS SMG, central: Same as [3] for SMG list sources detected at 150 GHz.
- dN/dS SMG, lower error bar: Same as [4] for SMG list sources detected at 150 GHz.
- dN/dS SMG, upper error bar: Same as [5] for SMG list sources detected at 150 GHz.
- Completeness: Average value of completeness across the flux range given by [1] and [2].
If you have any questions regarding this data set or its use please contact Wendy Everett (wendeline.everett_at_colorado.edu).
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| Differential Source Counts at 220 GHz |
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The differential number counts as a function of 220 GHz flux from Everett et al. (2020) are here .
Columns in the file are:
- Flux range [low]: Low end of flux bin in which counts were estimated. In units of Jy.
- Flux range [high]: High end of flux bin in which counts were estimated. In units of Jy.
- dN/dS total no cuts, central: Central value of differential counts (in units of number per square degree per Jy) for all sources detected at 220 GHz.
- dN/dS total no cuts, lower error bar: 1-sigma lower error bar for differential counts (in units of number per square degree per Jy) for all sources detected at 220 GHz.
- dN/dS total no cuts, upper error bar: 1-sigma upper error bar for differential counts (in units of number per square degree per Jy) for all sources detected at 220 GHz.
- dN/dS synchrotron z cut, central: Same as [3] for synchrotron-dominated sources detected at 220 GHz.
- dN/dS synchrotron z cut, lower error bar: Same as [4] for synchrotron-dominated sources detected at 220 GHz.
- dN/dS synchrotron z cut, upper error bar: Same as [5] for synchrotron-dominated sources detected at 220 GHz.
- dN/dS dust z cut, central: Same as [3] for dust-dominated sources detected at 220 GHz.
- dN/dS dust z cut, lower error bar: Same as [4] for dust-dominated sources detected at 220 GHz.
- dN/dS dust z cut, upper error bar: Same as [5] for dust-dominated sources detected at 220 GHz.
- dN/dS SMG, central: Same as [3] for SMG list sources detected at 220 GHz.
- dN/dS SMG, lower error bar: Same as [4] for SMG list sources detected at 220 GHz.
- dN/dS SMG, upper error bar: Same as [5] for SMG list sources detected at 220 GHz.
- Completeness: Average value of completeness across the flux range given by [1] and [2].
If you have any questions regarding this data set or its use please contact Wendy Everett (wendeline.everett_at_colorado.edu).
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| Cumulative Source Counts at 95 GHz |
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The cumulative number counts as a function of 95 GHz flux from Everett et al. (2020) are here .
Columns in the file are:
- Flux range [low]: Low end of flux bin in which counts were estimated. In units of Jy.
- Flux range [high]: High end of flux bin in which counts were estimated. In units of Jy.
- N(>S) total no cuts, central: Central value of cumulative counts (in units of number per square degree) for all sources detected at 95 GHz.
- N(>S) total no cuts, lower error bar: 1-sigma lower error bar for cumulative counts (in units of number per square degree) for all sources detected at 95 GHz.
- N(>S) total no cuts, upper error bar: 1-sigma upper error bar for cumulative counts (in units of number per square degree) for all sources detected at 95 GHz.
- N(>S) synchrotron z cut, central: Same as [3] for synchrotron-dominated sources detected at 95 GHz.
- N(>S) synchrotron z cut, lower error bar: Same as [4] for synchrotron-dominated sources detected at 95 GHz.
- N(>S) synchrotron z cut, upper error bar: Same as [5] for synchrotron-dominated sources detected at 95 GHz.
- N(>S) dust z cut, central: Same as [3] for dust-dominated sources detected at 95 GHz.
- N(>S) dust z cut, lower error bar: Same as [4] for dust-dominated sources detected at 95 GHz.
- N(>S) dust z cut, upper error bar: Same as [5] for dust-dominated sources detected at 95 GHz.
If you have any questions regarding this data set or its use please contact Wendy Everett (wendeline.everett_at_colorado.edu).
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| Cumulative Source Counts at 150 GHz |
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The cumulative number counts as a function of 150 GHz flux from Everett et al. (2020) are here .
Columns in the file are:
- Flux range [low]: Low end of flux bin in which counts were estimated. In units of Jy.
- Flux range [high]: High end of flux bin in which counts were estimated. In units of Jy.
- N(>S) total no cuts, central: Central value of cumulative counts (in units of number per square degree) for all sources detected at 150 GHz.
- N(>S) total no cuts, lower error bar: 1-sigma lower error bar for cumulative counts (in units of number per square degree) for all sources detected at 150 GHz.
- N(>S) total no cuts, upper error bar: 1-sigma upper error bar for cumulative counts (in units of number per square degree) for all sources detected at 150 GHz.
- N(>S) synchrotron z cut, central: Same as [3] for synchrotron-dominated sources detected at 150 GHz.
- N(>S) synchrotron z cut, lower error bar: Same as [4] for synchrotron-dominated sources detected at 150 GHz.
- N(>S) synchrotron z cut, upper error bar: Same as [5] for synchrotron-dominated sources detected at 150 GHz.
- N(>S) dust z cut, central: Same as [3] for dust-dominated sources detected at 150 GHz.
- N(>S) dust z cut, lower error bar: Same as [4] for dust-dominated sources detected at 150 GHz.
- N(>S) dust z cut, upper error bar: Same as [5] for dust-dominated sources detected at 150 GHz.
- N(>S) SMG, central: Same as [3] for SMG list sources detected at 150 GHz.
- N(>S) SMG, lower error bar: Same as [4] for SMG list sources detected at 150 GHz., excluding IRAS-FSC counterparts.
If you have any questions regarding this data set or its use please contact Wendy Everett (wendeline.everett_at_colorado.edu).
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| Cumulative Source Counts at 220 GHz |
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The cumulative number counts as a function of 220 GHz flux from Everett et al. (2020) are here .
Columns in the file are:
- Flux range [low]: Low end of flux bin in which counts were estimated. In units of Jy.
- Flux range [high]: High end of flux bin in which counts were estimated. In units of Jy.
- N(>S) total no cuts, central: Central value of cumulative counts (in units of number per square degree) for all sources detected at 220 GHz.
- N(>S) total no cuts, lower error bar: 1-sigma lower error bar for cumulative counts (in units of number per square degree) for all sources detected at 220 GHz.
- N(>S) total no cuts, upper error bar: 1-sigma upper error bar for cumulative counts (in units of number per square degree) for all sources detected at 220 GHz.
- N(>S) synchrotron z cut, central: Same as [3] for synchrotron-dominated sources detected at 220 GHz.
- N(>S) synchrotron z cut, lower error bar: Same as [4] for synchrotron-dominated sources detected at 220 GHz.
- N(>S) synchrotron z cut, upper error bar: Same as [5] for synchrotron-dominated sources detected at 220 GHz.
- N(>S) dust z cut, central: Same as [3] for dust-dominated sources detected at 220 GHz.
- N(>S) dust z cut, lower error bar: Same as [4] for dust-dominated sources detected at 220 GHz.
- N(>S) dust z cut, upper error bar: Same as [5] for dust-dominated sources detected at 220 GHz.
- N(>S) SMG, central: Same as [3] for SMG list sources detected at 220 GHz.
- N(>S) SMG, lower error bar: Same as [4] for SMG list sources detected at 220 GHz.
- N(>S) SMG, upper error bar: Same as [5] for SMG list sources detected at 220 GHz.
If you have any questions regarding this data set or its use please contact Wendy Everett (wendeline.everett_at_colorado.edu).
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| Covariance matrices for number counts |
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Following are covariance matrices for the synchrotron-dominated number counts from Everett et al. (2020) at 95 GHz , 150 GHz , and 220 GHz .
Following are covariance matrices for the SMG number counts from Everett et al. (2020) at 150 GHz , and 220 GHz .
The matrix elements in the files above are in units of Jy^(-2) and correspond to the flux bins with well-defined number counts (in the number counts above).
If you have any questions regarding this data set or its use please contact Wendy Everett (wendeline.everett_at_colorado.edu).
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| Point-source-filtered, CLEAN'ed maps and associated products |
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The point-source-filtered, CLEAN'ed (to 4.5 sigma) maps from Everett et al. (2020) are linked below.
There is one map per band (90, 150, 220 GHz) and per field in the SPT-SZ 2500-square-degree survey.
These per-field maps are in the Lambert azimuthal equal-area (ZEA) projection with 0.25-arcmin pixels.
They are stored in the primary array of a FITS file, with a header that includes world coordinate system
(WCS) information. Also linked below is one file per band in the full-sky Healpix pixelization with
nside=8192, in Galactic coordinates. The data in these files has been reprojected from the individual-field
maps. To save disk space, all files have been gzipped.
The signal from all sources detected at 4.5 sigma or greater in these maps
(including negative "sources" such as SZ decrements from clusters---although note that these
detections are not included in the source catalog linked here, for information on detected clusters
see the SPT-SZ 2500d cluster catalog papers
Bleem et al. 2015 and
Bocquet et al. 2019)
has been removed using
the CLEAN algorithm. These maps are intended to be used in conjunction with the 4.5-sigma
detected source catalog, linked above. To determine the flux density at a given sky location, first check
if a source at that location is included in the catalog; if not, the best-fit source flux density
at that location can be read off the CLEAN'ed maps.
These maps are not meant to have aperture photometry performed on them, as they are high-passed
strongly (particularly in the scan direction), and the total flux density within an aperture will tend to
zero as the aperture size is increased. The typical profile of a point source in the map (the "dirty
beam") in each band is stored in the "kernel" fits files linked below. The orientation of the
(anisotropic) profile varies across the field; the profile provided is for the center of the map.
The horizontal filtering wing follows lines of constant declination in the map, except in the
ra21hdec-50 field, where the true profile is roughly 1/3 times this profile plus 2/3 times this
profile 90 degrees rotated (with the filtering wing following lines of constant R.A.).
Files provided are (all gzipped fits files):
Full-sky Healpix nside=8192 CLEAN'ed map at 90 GHz: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_8192_90GHz.fits.gz .
Full-sky Healpix nside=8192 CLEAN'ed map at 150 GHz: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_8192_150GHz.fits.gz .
Full-sky Healpix nside=8192 CLEAN'ed map at 220 GHz: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_8192_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra0h50dec-50: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra0h50dec-50_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra0h50dec-50: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra0h50dec-50_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra0h50dec-50: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra0h50dec-50_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra1hdec-42.5: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra1hdec-42.5_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra1hdec-42.5: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra1hdec-42.5_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra1hdec-42.5: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra1hdec-42.5_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra1hdec-60: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra1hdec-60_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra1hdec-60: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra1hdec-60_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra1hdec-60: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra1hdec-60_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra21hdec-42.5: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra21hdec-42.5_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra21hdec-42.5: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra21hdec-42.5_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra21hdec-42.5: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra21hdec-42.5_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra21hdec-50: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra21hdec-50_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra21hdec-50: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra21hdec-50_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra21hdec-50: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra21hdec-50_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra21hdec-60: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra21hdec-60_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra21hdec-60: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra21hdec-60_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra21hdec-60: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra21hdec-60_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra22h30dec-55: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra22h30dec-55_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra22h30dec-55: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra22h30dec-55_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra22h30dec-55: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra22h30dec-55_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra23h30dec-55: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra23h30dec-55_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra23h30dec-55: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra23h30dec-55_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra23h30dec-55: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra23h30dec-55_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra23hdec-45: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra23hdec-45_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra23hdec-45: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra23hdec-45_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra23hdec-45: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra23hdec-45_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra23hdec-62.5: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra23hdec-62.5_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra23hdec-62.5: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra23hdec-62.5_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra23hdec-62.5: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra23hdec-62.5_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra2h30dec-50: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra2h30dec-50_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra2h30dec-50: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra2h30dec-50_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra2h30dec-50: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra2h30dec-50_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra3h30dec-42.5: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra3h30dec-42.5_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra3h30dec-42.5: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra3h30dec-42.5_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra3h30dec-42.5: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra3h30dec-42.5_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra3h30dec-60: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra3h30dec-60_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra3h30dec-60: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra3h30dec-60_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra3h30dec-60: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra3h30dec-60_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra4h10dec-50: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra4h10dec-50_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra4h10dec-50: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra4h10dec-50_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra4h10dec-50: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra4h10dec-50_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra5h30dec-45: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra5h30dec-45_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra5h30dec-45: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra5h30dec-45_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra5h30dec-45: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra5h30dec-45_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra5h30dec-55: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra5h30dec-55_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra5h30dec-55: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra5h30dec-55_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra5h30dec-55: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra5h30dec-55_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra6h30dec-45: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra6h30dec-45_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra6h30dec-45: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra6h30dec-45_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra6h30dec-45: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra6h30dec-45_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra6h30dec-55: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra6h30dec-55_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra6h30dec-55: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra6h30dec-55_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra6h30dec-55: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra6h30dec-55_220GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 90 GHz for field ra6hdec-62.5: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra6hdec-62.5_90GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 150 GHz for field ra6hdec-62.5: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra6hdec-62.5_150GHz.fits.gz .
Single-field ZEA 0.25-arcmin CLEAN'ed map at 220 GHz for field ra6hdec-62.5: spt_E20_map_mjy_ptsrc_filtered_clean4p5sig_ra6hdec-62.5_220GHz.fits.gz .
Beam and filter kernel (typical point-source profile or "dirty beam" for 90 GHz: spt_E20_beam_and_filter_kernel_90GHz.fits.gz .
Beam and filter kernel (typical point-source profile or "dirty beam" for 150 GHz: spt_E20_beam_and_filter_kernel_150GHz.fits.gz .
Beam and filter kernel (typical point-source profile or "dirty beam" for 220 GHz: spt_E20_beam_and_filter_kernel_220GHz.fits.gz .
If you have any questions regarding this data set or its use please contact Wendy Everett (wendeline.everett_at_colorado.edu).
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