Intercalibration of the GPM Microwave Radiometer Constellation

The Global Precipitation Measurement (GPM) mission is a constellation-based satellite mission designed to unify and advance precipitation measurements using both research and operational microwave sensors. This requires consistency in the input brightness temperatures (Tb), which is accomplished by...

Celý popis

Uložené v:
Podrobná bibliografia
Vydané v:Journal of atmospheric and oceanic technology Ročník 33; číslo 12; s. 2639 - 2654
Hlavní autori: Berg, Wesley, Bilanow, Stephen, Chen, Ruiyao, Datta, Saswati, Draper, David, Ebrahimi, Hamideh, Farrar, Spencer, Jones, W. Linwood, Kroodsma, Rachael, McKague, Darren, Payne, Vivienne, Wang, James, Wilheit, Thomas, Yang, John Xun
Médium: Journal Article
Jazyk:English
Vydavateľské údaje: Boston American Meteorological Society 01.12.2016
Predmet:
ISSN:0739-0572, 1520-0426
On-line prístup:Získať plný text
Tagy: Pridať tag
Žiadne tagy, Buďte prvý, kto otaguje tento záznam!
Popis
Shrnutí:The Global Precipitation Measurement (GPM) mission is a constellation-based satellite mission designed to unify and advance precipitation measurements using both research and operational microwave sensors. This requires consistency in the input brightness temperatures (Tb), which is accomplished by intercalibrating the constellation radiometers using the GPM Microwave Imager (GMI) as the calibration reference. The first step in intercalibrating the sensors involves prescreening the sensor Tb to identify and correct for calibration biases across the scan or along the orbit path. Next, multiple techniques developed by teams within the GPM Intersatellite Calibration Working Group (XCAL) are used to adjust the calibrations of the constellation radiometers to be consistent with GMI. Comparing results from multiple approaches helps identify flaws or limitations of a given technique, increase confidence in the results, and provide a measure of the residual uncertainty. The original calibration differences relative to GMI are generally within 2–3 K for channels below 92 GHz, although AMSR2 exhibits larger differences that vary with scene temperature. SSMIS calibration differences also vary with scene temperature but to a lesser degree. For SSMIS channels above 150 GHz, the differences are generally within ~2 K with the exception of SSMIS on board DMSP F19 , which ranges from 7 to 11 K colder than GMI depending on frequency. The calibrations of the cross-track radiometers agree very well with GMI with values mostly within 0.5 K for the Sondeur Atmosphérique du Profil d’Humidité Intertropicale par Radiométrie (SAPHIR) and the Microwave Humidity Sounder (MHS) sensors, and within 1 K for the Advanced Technology Microwave Sounder (ATMS).
Bibliografia:ObjectType-Article-1
SourceType-Scholarly Journals-1
ObjectType-Feature-2
content type line 14
ISSN:0739-0572
1520-0426
DOI:10.1175/JTECH-D-16-0100.1