Abstract

Abstract. Following the release of the version 4 Cloud-Aerosol Lidar with Orthogonal Polarization (CALIOP) data products from Cloud-Aerosol Lidar and Infrared Pathfinder Satellite Observations (CALIPSO) mission, a new version 4 (V4) of the CALIPSO Imaging Infrared Radiometer (IIR) Level 2 data products has been developed. The IIR Level 2 data products include cloud effective emissivities and cloud microphysical properties such as effective diameter (De) and water path estimates for ice and liquid clouds. This paper (Part II) shows retrievals over ocean and describes the improvements made with respect to version 3 (V3) as a result of the significant changes implemented in the V4 algorithms, which are presented in a companion paper (Part I). The analysis of the three-channel IIR observations (08.65, 10.6, and 12.05 µm) is informed by the scene classification provided in the V4 CALIOP 5 km cloud layer and aerosol layer products. Thanks to the reduction of inter-channel effective emissivity biases in semi-transparent (ST) clouds when the oceanic background radiance is derived from model computations, the number of unbiased emissivity retrievals is increased by a factor of 3 in V4. In V3, these biases caused inconsistencies between the effective diameters retrieved from the 12/10 (βeff12/10 = τa,12/τa,10) and 12/08 (βeff12/08 = τa,12/τa,08) pairs of channels at emissivities smaller than 0.5. In V4, microphysical retrievals in ST ice clouds are possible in more than 80 % of the pixels down to effective emissivities of 0.05 (or visible optical depth ∼0.1). For the month of January 2008, which was chosen to illustrate the results, median ice De and ice water path (IWP) are, respectively, 38 µm and 3 g m−2 in ST clouds, with random uncertainty estimates of 50 %. The relationship between the V4 IIR 12/10 and 12/08 microphysical indices is in better agreement with the “severely roughened single column” ice habit model than with the “severely roughened eight-element aggregate” model for 80 % of the pixels in the coldest clouds (<210 K) and 60 % in the warmest clouds (>230 K). Retrievals in opaque ice clouds are improved in V4, especially at night and for 12/10 pair of channels, due to corrections of the V3 radiative temperature estimates derived from CALIOP geometric altitudes. Median ice De and IWP are 58 µm and 97 g m−2 at night in opaque clouds, with again random uncertainty estimates of 50 %. Comparisons of ice retrievals with Moderate Resolution Imaging Spectroradiometer (MODIS)/Aqua in the tropics show a better agreement of IIR De with MODIS visible–3.7 µm than with MODIS visible–2.1 µm in the coldest ST clouds and the opposite for opaque clouds. In prevailingly supercooled liquid water clouds with centroid altitudes above 4 km, retrieved median De and liquid water path are 13 µm and 3.4 g m−2 in ST clouds, with estimated random uncertainties of 45 % and 35 %, respectively. In opaque liquid clouds, these values are 18 µm and 31 g m−2 at night, with estimated uncertainties of 50 %. IIR De in opaque liquid clouds is smaller than MODIS visible–2.1 µm and visible–3.7 µm by 8 and 3 µm, respectively.

Highlights

  • The Imaging Infrared Radiometer (IIR) is one of the three instruments on board the Cloud-Aerosol Lidar and Infrared Pathfinder Satellite Observations (CALIPSO) satellite which has been in quasi-continuous operation since mid-June 2006 (Winker et al, 2010)

  • The only difference between effective emissivity version 4 (V4) retrievals in liquid and ice clouds is that Tr is taken as the temperature at the Cloud-Aerosol Lidar with Orthogonal Polarization (CALIOP) centroid altitude (Tc) in the case of liquid water clouds, whereas this initial temperature estimate is further corrected in the case of ice clouds

  • This paper describes the impacts of the various changes implemented in the V4 IIR Level 2 algorithm on the effective emissivities and microphysical retrievals in ice clouds

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Summary

Introduction

The Imaging Infrared Radiometer (IIR) is one of the three instruments on board the Cloud-Aerosol Lidar and Infrared Pathfinder Satellite Observations (CALIPSO) satellite which has been in quasi-continuous operation since mid-June 2006 (Winker et al, 2010). Two main pieces of information are needed to retrieve these quantities: the cloud top-of-atmosphere (TOA) blackbody radiance, which requires a good estimate of the cloud radiative temperature, and the TOA background radiance that would be observed if no cloud were present. The former drives the accuracy at large emissivities and the latter the accuracy at small emissivities. In the IIR algorithm, the TOA background radiance is preferentially determined using observations in neighboring pixels in those cases when clear-sky conditions, as determined by CALIOP, can be found Otherwise, it is computed using the fastcalculation radiative transfer (FASRAD) model (Garnier et al, 2012; Dubuisson et al, 2005).

Cloudy scene selection
Retrievals in ice clouds
Effective emissivity
Inter-channel effective emissivity differences
Visible cloud optical depth
Microphysical indices and effective diameter retrievals
Fraction of samples in sensitivity range
Changes in effective diameters
V4 microphysical retrievals
Effective diameter and ice water path
Ice habit model selection
Retrievals using parameterizations from in situ formulation
Comparisons with MODIS
V4 retrievals in liquid water clouds
Effective diameter and liquid water path
Findings
Conclusions and perspectives
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