Authors:
Dr. David Patrick Donovan | Royal Netherlands Meteorological Institute (KNMI) | Netherlands
Dr. Gerd-Jan van Zadelhoff | Royal Netherlands Meteorological Institute (KNMI) | Netherlands
Dr. Ping Wand | Royal Netherlands Meteorological Institute (KNMI)
The Earth Clouds Aerosol and Radiation Explorer (EarthCARE) mission is an ESA/JAXA multi-instrument mission to launch in 2023. The mission consists of a cloud-profiling radar (CPR), a cloud/aerosol lidar (ATLID), a cloud/aerosol imager (MSI), and a three-view broadband radiometer (BBR) covering both LW and SW bands. The mission will deliver a unique and powerful suite of cloud, aerosol and radiation products.
The EarthCARE lidar is called ATLID (ATmospheric Lidar) and is a high-spectral resolution lidar (HSRL). Like ALADIN (the HSRL lidar carried aboard Aeolus) ATLID operates at 355nm . However, ATLID is optimized for cloud and aerosol sensing, while ALADIN's main focus is on the retrieval of winds. Accordingly, ATLID will measure with a much higher resolution compared with ALADIN and possesses a depolarization channel (unlike ALADIN).
ATLID uses a Fabry-Perot etalon based design to distinguished the thermally broadened return from atmospheric molecules from the spectraly narrower return from clouds and aerosols. This allows for the determination of both the extinction profile as well as the extinction-to-backscatter ratio (also known as the lidar-ratio or S). This is in contrast to elastic backscatter lidars (e.g. CALIPSO) which must specify the S in order to derive the extinction profile. In principle, rather simple direct methods for retrieving extinction and S profiles using HSRL attenuated backscatters exist, however, they require high signal-to-noise ratios. In general, the low SNR of space-based lidars compared to their terrestrial counterparts, leads to the need for extensive horizontal smoothing windows.
Averaging intervals on the order of 100km are often defensible for aerosol fields, but certainly not for cloud observations. For clouds, intervals on the order of a very few kilometers or even finer are necessary. Therefore, it is necessary to separate the "strong" (e.g. cloud) and "weak"(e.g. aerosol) regions at high resolution before smoothing the attenuated backscatter returns. In the ATLID processing chain, this is largely accomplished by using the output of the Featuremask processor (A-FM) which uses adaptive thresholds and ideas drawn from image-processing to provide a high-resolution target mask.
After the cloud-screened signals are averaged, then direct techniques for retrieving the extinction and lidar-ratio profiles at low horizontal resolution are employed. To retrieve the cloud properties, a second pass employing a forward-modelling optimal estimation approach (using the low-resolution results as priors) is applied at high horizontal resolution. The processor that accomplishes this is called the ATLID profile processor (A-PRO). In addition to the retrieval of the optical properties, targets are also classified (e.g. water, ice, aerosol(type)) using e.g. extinction, temperature, lidar-ratio and linear-depolarization ratio) by the ATLID target classification procedure (A-TC) which is embedded within the A-PRO processor.
A-FM and A-PRO have been extensively tested using detailed simulated L1 data derived from the application of advanced lidar radiative transfer models and instrument simulators to high-resolution atmospheric model data. Adaptations of A-FM and A-PRO, called AEL-FM and AEL-PRO respectively, have also been created and successfully applied to ALADIN observations. In this presentation, A-FM and A-PRO will be briefly introduced, new developments highlighted, and various illustrative examples drawn from the set of simulated tests scenes presented and discussed. Additionally, example AEL-FM and AEL-PRO results will be presented.