Satellite Sensors

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This pages links to the observation of the satellites of following dates,  
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The CREW evaluation activities concentrate on passive imager instruments onboard both polar and geostationary satellites (SEVIRI, AVHRR, and MODIS). Furthermore some participants also use polarized radiances of POLDER, the spectral information of MERES, and the multi angle observation of MISR. The active sensors CALIOP and CPR and the micro waver intrument AMSR-E are used as reference for the retrievals using passive sensors.
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that were optimal for the validation purposes:
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== Passive Imagers ==
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{| class="wikitable sortable"
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'''''SEVIRI''''' <br>
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[http://www.eumetsat.int/Home/Main/Satellites/MeteosatSecondGeneration/Instruments/index.htm?l=en SEVIRI] is a 50 cm-diameter aperture, line-by-line scanning radiometer, which provides image
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| 13  || June  || 2008  || 12:00-15:30
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| 17/18 ||  June  || 2008  || 22:15-01:45
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| 22  || June  || 2008  || 10:30-12:15
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| 03  || July  || 2008    || 10:00-12:00
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<td> * 13 June    2008 12:00-15:30  </td>
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* 17/18 June 2008 22:15-01:45
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* 22 June    2008 10:30-12:15
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* 03 July    2008 10:00-12:00
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The data sets are stored on the FTP site of ICARE and '''''is available only for CREW members''''', see [[Data_Access]].
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== MSG/SEVIRI ==
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SEVIRI is a 50 cm-diameter aperture, line-by-line scanning radiometer, which provides image
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data in four Visible and Near-InfraRed (VNIR) channels and eight InfraRed (IR) channels. A
data in four Visible and Near-InfraRed (VNIR) channels and eight InfraRed (IR) channels. A
key feature of this imaging instrument (Fig. 1) is its continuous imaging of the Earth in 12
key feature of this imaging instrument (Fig. 1) is its continuous imaging of the Earth in 12
spectral channels with a baseline repeat cycle of 15 min. The imaging sampling distance is
spectral channels with a baseline repeat cycle of 15 min. The imaging sampling distance is
3 km at the sub-satellite point for standard channels, and down to 1 km for the High
3 km at the sub-satellite point for standard channels, and down to 1 km for the High
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Resolution Visible (HRV) channel. (from [http://www.esa.int/esapub/bulletin/bullet111/chapter4_bul111.pdf www.esa.int])<br>
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Resolution Visible (HRV) channel.<br>
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<!--
Data access for the CREW periods here:
Data access for the CREW periods here:
[ftp://ftp.icare.univ-lille1.fr:/DATA/FS117/crew/observations/SEVIRI ./crew/observations/SEVIRI]
[ftp://ftp.icare.univ-lille1.fr:/DATA/FS117/crew/observations/SEVIRI ./crew/observations/SEVIRI]
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-->
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== MODIS ==
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'''''MODIS'''''<br>
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MODIS (Moderate-resolution Imaging Spectroradiometer) is a payload scientific instrument launched into Earth orbit by NASA in 1999 on board the Terra (EOS AM) Satellite, and in 2002 on board the Aqua (EOS PM) satellite. The instruments capture data in 36 spectral bands ranging in wavelength from 0.4 µm  to 14.4 µm and at varying spatial resolutions (2 bands at 250 m, 5 bands at 500 m and 29 bands at 1 km). Together the instruments image the entire Earth every 1 to 2 days. (from [http://en.wikipedia.org/wiki/MODIS Wikipedia])<br>Data access for the CREW periods here:
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[http://en.wikipedia.org/wiki/MODIS MODIS] (Moderate-resolution Imaging Spectroradiometer) is a payload scientific instrument launched into Earth orbit by NASA in 1999 on board the Terra (EOS AM) Satellite, and in 2002 on board the Aqua (EOS PM) satellite. The instruments capture data in 36 spectral bands ranging in wavelength from 0.4 µm  to 14.4 µm and at varying spatial resolutions (2 bands at 250 m, 5 bands at 500 m and 29 bands at 1 km). Together the instruments image the entire Earth every 1 to 2 days. <br>
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A description of the MODIS instrument and access to the dataset is given at the official [http://modis-atmos.gsfc.nasa.gov/ MODIS website].
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<!-- 
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Data access for the CREW periods here:
[ftp://ftp.icare.univ-lille1.fr:/DATA/FS117/crew/observations/MODIS ./crew/observations/MODIS]
[ftp://ftp.icare.univ-lille1.fr:/DATA/FS117/crew/observations/MODIS ./crew/observations/MODIS]
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-->
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== AVHRR ==
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'''''AVHRR'''''<br>
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AVHRR instruments measure the reflectance of the Earth in 5 relatively wide (by today's standards) spectral bands. The first two are centered around the red (0.6 micrometer, 0.5 THz) and near-infrared  (0.9 micrometer, 0.3 THz) regions, the third one is located around 3.5 micrometer, and the last two sample the thermal radiation emitted by the planet, around 11 and 12 micrometers, respectively. (from [http://en.wikipedia.org/wiki/Advanced_Very_High_Resolution_Radiometer Wikipedia]). <br>Data access for the CREW periods here:
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The [http://en.wikipedia.org/wiki/Advanced_Very_High_Resolution_Radiometer AVHRR] instrument (Advanced Very High Resolution Radiometer) measure the reflectance of the Earth in 5 relatively wide (by today's standards) spectral bands. The first two are centered around the red (0.6 micrometer, 0.5 THz) and near-infrared  (0.9 micrometer, 0.3 THz) regions, the third one is located around 3.5 micrometer, and the last two sample the thermal radiation emitted by the planet, around 11 and 12 micrometers, respectively.  
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<!--
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<br>Data access for the CREW periods here:  
[ftp://ftp.icare.univ-lille1.fr:/DATA/FS117/crew/observations/AVHRR ./crew/observations/AVHRR]
[ftp://ftp.icare.univ-lille1.fr:/DATA/FS117/crew/observations/AVHRR ./crew/observations/AVHRR]
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-->
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'''''POLDER'''''<br>
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[http://smsc.cnes.fr/POLDER/ POLDER] (POLarization and Directionality of the Earth's Reflectances) is a wide field of view imaging radiometer that has provided the first global, systematic measurements of ''spectral, directional and polarized'' characteristics of the solar radiation reflected by the Earth/atmosphere system. Its original observation capabilities have opened up new perspectives for discriminating the radiation scattered in the atmosphere from the radiation actually reflected by the surface.
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'''''MERIS'''''<br>
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[http://envisat.esa.int/instruments/meris/ MERIS] (The Medium Resolution Imaging Spectrometer Instrument) is a wide field-of-view pushbroom imaging spectrometer with a swath width of 1150km (field-of-view (FOV) = 68.5°) measuring the solar radiation reflected by the Earth in 15 spectral bands in the solar range from about 412.5nm to 900nm. All bands are programmable in width (variable between 1.25 and 30 nm) and position, but are fixed before launch in response to the recommendations of the Science Advisory Group (SAG) for the main period of the mission. The instrument scans the Earth's surface by the so called "push-broom" method. Linear CCD arrays provide spatial sampling in the across-track direction, while the satellite's motion provides scanning in the along-track direction. Each MERIS pixel has a field of view of 0.019°. Due to the wide instrument field of view (68.5°), spatial sampling varies in the across track direction, between 0.26 km at nadir and 0.39 km at swath extremities. Along-track sampling is close to 0.29 km.
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'''''MISR'''''<br>
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Viewing the sunlit Earth simultaneously at nine widely spaced angles, [http://www-misr.jpl.nasa.gov/ MISR] (Multi-angle Imaging SpectroRadiometer) provides ongoing global coverage with high spatial detail. In each of the nine MISR cameras, images will be obtained in four spectral bands, i.e. in four different colors, one each for blue, green, red, and near-infrared. The center wavelength of each of these bands is 446, 558, 672, and 867 nanometers respectively. Each MISR camera sees instantaneously a single row of pixels at right angles to the ground track. MISR collects data only on the daylit side of the Earth. During each orbit, MISR obtains a swath of imagery that is 360 km wide by about 20,000 km long. The intrinsic crosstrack dimensions of the MISR pixels was therefore chosen to be 275 meters at all off-nadir angles. The nadir camera makes use of the A camera design, resulting in a slightly higher crosstrack resolution of 250 meters, and this allows it to provide a slightly better ground locating reference that is passed on to the observations from the other cameras.
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== A-TRAIN reference instruments ==
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== CALIOP ==
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'''''CALIOP'''''<br>
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The Cloud-Aerosol LIdar with Orthogonal Polarization (CALIOP) is the primary instrument on the CALIPSO satellite, which was launched in 2005. CALIOP provides profiles of total backscatter at two wavelengths, from which aerosol and cloud profiles will be derived. The instrument also measures the linear depolarization of the backscattered return, allowing discrimination of cloud phase and the identification of the presence of non-spherical aerosols.<br>Data access for the CREW periods here:
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CALIOP (Cloud-Aerosol LIdar with Orthogonal Polarization) [Anderson, et al., 2005] is the primary instrument on the CALIPSO satellite. It is a dual wavelength polarized Lidar launched in April 2006 on board CALIPSO. Measurements are taken at two wavelengths, 532 nm and 1064 nm. Primary products are the profiles of total backscatter, as well as profiles of cloud and aerosol properties. The instrument also measures the linear depolarization of the backscattered return at 532 nm, allowing discrimination of cloud phase and the identification of the presence of non-spherical aerosols. Individual CALIOP beams have a width of about 70 meters on the Earth’s surface with a sampling distance of 333 m on the surface. Products are available at different resolutions with a footprint size of typically 1-5 km and a vertical resolution of 30-60 meters (nominal). Its high sensitivity and vertical resolution make CALIOP an excellent candidate system for the analysis of cloud top height as well as cloud phase (near top). Additionally, its high sensitivity to aerosols makes it a valuable tool to detect aerosol layers above clouds. As regards water clouds, CALIOP saturates fairly quickly near the cloud top and will not provide much information about the inner structure of the clouds. However, for optically less dense ice clouds, CALIOP provides information about ice also from deeper within the cloud [Chiriaco, et al., 2007].<br>
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[ftp://ftp.icare.univ-lille1.fr:/DATA/FS117/crew/observations/CALIOP ./crew/observations/CALIOP]
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CALIOP observation and retrieval products are available on the ICARE FTP site: [http://www.icare.univ-lille1.fr/archive/index.php?dir=CALIOP/ CALIOP].
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== CPR ==
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'''''CPR'''''<br>
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[ftp://ftp.icare.univ-lille1.fr:/DATA/FS117/crew/observations/CPR ./crew/observations/CPR]
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[http://cloudsat.atmos.colostate.edu/instrument CPR] (Cloud Profiling Radar) onboard of Cloudsat is a 94-GHz nadir-looking radar was lanched in April 2006. It measures the power backscattered by clouds, scene classifications, and cloud optical properties as a function of distance from the radar with a vertical resolution of 500 m, a cross-track resolution of 1.4 km, and an along-track resolution of 1.7 km.<br>
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Cloudsat CPR observation and retrieval products are available on the ICARE FTP site: [http://www.icare.univ-lille1.fr/archive/index.php?dir=CLOUDSAT/ CLOUDSAT].
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== AMSR ==
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'''''AMSR'''''<br>
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[ftp://ftp.icare.univ-lille1.fr:/DATA/FS117/crew/observations/AMSR ./crew/observations/AMSR]
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[http://aqua.nasa.gov/about/instrument_amsr.php AMSR-E] (Advanced Microwave Scanning Radiometer for EOS) is a twelve-channel, six-frequency, total power passive-microwave radiometer system. It measures brightness temperatures at 6.925, 10.65, 18.7, 23.8, 36.5, and 89.0 GHz. Vertically and horizontally polarized measurements are taken at all channels. The Earth-emitted microwave radiation is collected by an offset parabolic reflector 1.6 meters in diameter that scans across the Earth along an imaginary conical surface, maintaining a constant Earth incidence angle of 55° and providing a swath width array of six feedhorns which then carry the radiation to radiometers for measurement. Calibration is accomplished with observations of cosmic background radiation and an on-board warm target. Spatial resolution of the individual measurements varies from 5.4 km at 89.0 GHz to 56 km at 6.9 GHz.<br>
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Brightness temperatures of AMSR are available of the ICARE FTP site: [http://www.icare.univ-lille1.fr/archive/index.php?dir=AMSR_E/ AMSR_E].
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== Syntetic ==
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== Synthetic datasets ==
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Simulated satellites scenes can be used to validate retrieval algorithms with a 'know truth'.<br>
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Instead of using real observations, it is possible to simulate the observations with a radiative transfer model.
 +
The advantage of these simulated satellites scenes is, that the state of the atmosphere and the clouds is known.
 +
In this way the results of the retrieval can be diretly compared to the 'known' atmospheric state.
 +
The disadvantage is, that assumptions and uncertainties may occur in the forward simulation,
 +
including the horizontal homogeneity, vertical structued clouds, three dimensional radiative transfer, and not perfectly known optical properties of the surface, gaseous absorption, and clouds.
 +
Noting deviations of the retrieval result and the 'known' atmospheric state, it is always nessesary to check weather the deviation is caused by an imprecise retrieval algorithm or an inaccuracy of the forward model.
 +
Using the same forward model and assumptions for the simulations of satellite observations and for training the retrieval algorithm may also lead to a situation, where inaccuracy of radiative transfer and retrieval cancel each other out.
 +
Nevertheless this approach is useful as plausibility check, to identify to rough assumptions in the retrieval algorithm, and to distinguish properties that may be retrieved and that are impossible to retrieve. Simulations may be performed with different radiative transfer models for different sensors. The most known radiative transfer models are [http://www.libradtran.org/ libRadtran], [http://6s.ltdri.org/ S6], and [http://research.metoffice.gov.uk/research/interproj/nwpsaf/rtm/ RTTOV] and [http://en.wikipedia.org/wiki/Atmospheric_radiative_transfer_codes more].
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<!--
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The CREW data set contains some forward simulations. These are look-up-tables used in retrieval algorithms or whole simulated satellite pictures including the three dimensional radiative transfer.
Data access for the CREW periods here:
Data access for the CREW periods here:
[ftp://ftp.icare.univ-lille1.fr:/DATA/FS117/crew/observations/SYNTHETIC ./crew/observations/SYNTHETIC]
[ftp://ftp.icare.univ-lille1.fr:/DATA/FS117/crew/observations/SYNTHETIC ./crew/observations/SYNTHETIC]
 +
-->

Latest revision as of 12:32, 20 August 2014

The CREW evaluation activities concentrate on passive imager instruments onboard both polar and geostationary satellites (SEVIRI, AVHRR, and MODIS). Furthermore some participants also use polarized radiances of POLDER, the spectral information of MERES, and the multi angle observation of MISR. The active sensors CALIOP and CPR and the micro waver intrument AMSR-E are used as reference for the retrievals using passive sensors.

Passive Imagers

SEVIRI
SEVIRI is a 50 cm-diameter aperture, line-by-line scanning radiometer, which provides image data in four Visible and Near-InfraRed (VNIR) channels and eight InfraRed (IR) channels. A key feature of this imaging instrument (Fig. 1) is its continuous imaging of the Earth in 12 spectral channels with a baseline repeat cycle of 15 min. The imaging sampling distance is 3 km at the sub-satellite point for standard channels, and down to 1 km for the High Resolution Visible (HRV) channel.

MODIS
MODIS (Moderate-resolution Imaging Spectroradiometer) is a payload scientific instrument launched into Earth orbit by NASA in 1999 on board the Terra (EOS AM) Satellite, and in 2002 on board the Aqua (EOS PM) satellite. The instruments capture data in 36 spectral bands ranging in wavelength from 0.4 µm to 14.4 µm and at varying spatial resolutions (2 bands at 250 m, 5 bands at 500 m and 29 bands at 1 km). Together the instruments image the entire Earth every 1 to 2 days.
A description of the MODIS instrument and access to the dataset is given at the official MODIS website.

AVHRR
The AVHRR instrument (Advanced Very High Resolution Radiometer) measure the reflectance of the Earth in 5 relatively wide (by today's standards) spectral bands. The first two are centered around the red (0.6 micrometer, 0.5 THz) and near-infrared (0.9 micrometer, 0.3 THz) regions, the third one is located around 3.5 micrometer, and the last two sample the thermal radiation emitted by the planet, around 11 and 12 micrometers, respectively.

POLDER
POLDER (POLarization and Directionality of the Earth's Reflectances) is a wide field of view imaging radiometer that has provided the first global, systematic measurements of spectral, directional and polarized characteristics of the solar radiation reflected by the Earth/atmosphere system. Its original observation capabilities have opened up new perspectives for discriminating the radiation scattered in the atmosphere from the radiation actually reflected by the surface.

MERIS
MERIS (The Medium Resolution Imaging Spectrometer Instrument) is a wide field-of-view pushbroom imaging spectrometer with a swath width of 1150km (field-of-view (FOV) = 68.5°) measuring the solar radiation reflected by the Earth in 15 spectral bands in the solar range from about 412.5nm to 900nm. All bands are programmable in width (variable between 1.25 and 30 nm) and position, but are fixed before launch in response to the recommendations of the Science Advisory Group (SAG) for the main period of the mission. The instrument scans the Earth's surface by the so called "push-broom" method. Linear CCD arrays provide spatial sampling in the across-track direction, while the satellite's motion provides scanning in the along-track direction. Each MERIS pixel has a field of view of 0.019°. Due to the wide instrument field of view (68.5°), spatial sampling varies in the across track direction, between 0.26 km at nadir and 0.39 km at swath extremities. Along-track sampling is close to 0.29 km.

MISR
Viewing the sunlit Earth simultaneously at nine widely spaced angles, MISR (Multi-angle Imaging SpectroRadiometer) provides ongoing global coverage with high spatial detail. In each of the nine MISR cameras, images will be obtained in four spectral bands, i.e. in four different colors, one each for blue, green, red, and near-infrared. The center wavelength of each of these bands is 446, 558, 672, and 867 nanometers respectively. Each MISR camera sees instantaneously a single row of pixels at right angles to the ground track. MISR collects data only on the daylit side of the Earth. During each orbit, MISR obtains a swath of imagery that is 360 km wide by about 20,000 km long. The intrinsic crosstrack dimensions of the MISR pixels was therefore chosen to be 275 meters at all off-nadir angles. The nadir camera makes use of the A camera design, resulting in a slightly higher crosstrack resolution of 250 meters, and this allows it to provide a slightly better ground locating reference that is passed on to the observations from the other cameras.

A-TRAIN reference instruments

CALIOP
CALIOP (Cloud-Aerosol LIdar with Orthogonal Polarization) [Anderson, et al., 2005] is the primary instrument on the CALIPSO satellite. It is a dual wavelength polarized Lidar launched in April 2006 on board CALIPSO. Measurements are taken at two wavelengths, 532 nm and 1064 nm. Primary products are the profiles of total backscatter, as well as profiles of cloud and aerosol properties. The instrument also measures the linear depolarization of the backscattered return at 532 nm, allowing discrimination of cloud phase and the identification of the presence of non-spherical aerosols. Individual CALIOP beams have a width of about 70 meters on the Earth’s surface with a sampling distance of 333 m on the surface. Products are available at different resolutions with a footprint size of typically 1-5 km and a vertical resolution of 30-60 meters (nominal). Its high sensitivity and vertical resolution make CALIOP an excellent candidate system for the analysis of cloud top height as well as cloud phase (near top). Additionally, its high sensitivity to aerosols makes it a valuable tool to detect aerosol layers above clouds. As regards water clouds, CALIOP saturates fairly quickly near the cloud top and will not provide much information about the inner structure of the clouds. However, for optically less dense ice clouds, CALIOP provides information about ice also from deeper within the cloud [Chiriaco, et al., 2007].
CALIOP observation and retrieval products are available on the ICARE FTP site: CALIOP.

CPR
CPR (Cloud Profiling Radar) onboard of Cloudsat is a 94-GHz nadir-looking radar was lanched in April 2006. It measures the power backscattered by clouds, scene classifications, and cloud optical properties as a function of distance from the radar with a vertical resolution of 500 m, a cross-track resolution of 1.4 km, and an along-track resolution of 1.7 km.
Cloudsat CPR observation and retrieval products are available on the ICARE FTP site: CLOUDSAT.

AMSR
AMSR-E (Advanced Microwave Scanning Radiometer for EOS) is a twelve-channel, six-frequency, total power passive-microwave radiometer system. It measures brightness temperatures at 6.925, 10.65, 18.7, 23.8, 36.5, and 89.0 GHz. Vertically and horizontally polarized measurements are taken at all channels. The Earth-emitted microwave radiation is collected by an offset parabolic reflector 1.6 meters in diameter that scans across the Earth along an imaginary conical surface, maintaining a constant Earth incidence angle of 55° and providing a swath width array of six feedhorns which then carry the radiation to radiometers for measurement. Calibration is accomplished with observations of cosmic background radiation and an on-board warm target. Spatial resolution of the individual measurements varies from 5.4 km at 89.0 GHz to 56 km at 6.9 GHz.
Brightness temperatures of AMSR are available of the ICARE FTP site: AMSR_E.

Synthetic datasets

Instead of using real observations, it is possible to simulate the observations with a radiative transfer model. The advantage of these simulated satellites scenes is, that the state of the atmosphere and the clouds is known. In this way the results of the retrieval can be diretly compared to the 'known' atmospheric state. The disadvantage is, that assumptions and uncertainties may occur in the forward simulation, including the horizontal homogeneity, vertical structued clouds, three dimensional radiative transfer, and not perfectly known optical properties of the surface, gaseous absorption, and clouds. Noting deviations of the retrieval result and the 'known' atmospheric state, it is always nessesary to check weather the deviation is caused by an imprecise retrieval algorithm or an inaccuracy of the forward model. Using the same forward model and assumptions for the simulations of satellite observations and for training the retrieval algorithm may also lead to a situation, where inaccuracy of radiative transfer and retrieval cancel each other out. Nevertheless this approach is useful as plausibility check, to identify to rough assumptions in the retrieval algorithm, and to distinguish properties that may be retrieved and that are impossible to retrieve. Simulations may be performed with different radiative transfer models for different sensors. The most known radiative transfer models are libRadtran, S6, and RTTOV and more.