Contributors: W. Preimesberger (tuwien), W. Dorigo (tuwien), A. Dostalova (EODC), T. Frederikse (vandersat/planet labs), J. Lems (tuwien) and R. Kidd (EODC)
Issued by: EODC/Alena Dostalova
Date: 13/05/2025
Ref: C3S2_313c_EODC_WP1-DDP-SSM-v1_202506_ATBD; C3S2_313c_EODC_WP1-DDP-RZSM-v1_202506_ATBD; C3S2_313c_EODC_WP1-DDP-FT-v1_202506_ATBD
Official reference number service contract: 2024/C3S2_313c_EODC/SC1
History of modifications
List of datasets covered by this document
Acronyms
General definitions
Active (soil moisture) retrieval: the process of modelling soil moisture from radar (scatterometer and synthetic aperture radar) measurements. The measurand of active microwave remote sensing systems is called “backscatter”.
Backscatter is the measurand of “active” microwave remote sensing systems (radar). As the energy pulses emitted by the radar hit the surface, a scattering effect occurs and part of the energy is reflected back. The received energy is called “backscatter”, with rough surfaces producing stronger signals than smooth surfaces. It comprises reflections from the soil surface layer (“surface scatter”), vegetation (“volume scatter”) and interactions of the two. Under very dry soil conditions, structural features in deeper soil layers can act as volume scatterers (“subsurface scattering”).
Bias : “Bias is defined as an estimate of the systematic measurement error” GCOS-200 (WMO, 2016)
Brightness Temperature is the measurand of “passive“ microwave remote sensing system (radiometers). Brightness temperature (in degree Kelvin) is a function of kinetic temperature and emissivity. Wet soils have a higher emissivity than dry soils and therefore a higher brightness temperature. Passive soil moisture retrieval uses this difference between kinetic temperature and brightness temperature, to model the amount of water available in the soil of the observed area, while taking into account factors such as the water held by vegetation. "Upwelling" brightness temperature refers to the fraction that is emitted towards the satellite, while "downwelling" referes to the fraction that is emitted towards the Earth's surface.
Emissivity is a measure of how effectively an object radiates thermal energy compared to a black body. In the context of passive microwave remote sensing, it represents the ratio of the microwave radiation emitted by the surface (soil or vegetation) to the radiation emitted by a black body at the same physical temperatur. Emissivity is primarily a function of the dielectric properties of a media, which - in the context of soil moisture retrieval - is strongly influenced by the water content of the ground and vegetation in a scene observed by the satellite.
Freeze/Thaw refers to the state of soil moisture during a year. Water in the upper soil layer transitions within the soil between its liquid and solid (ice) states due to changes in temperature. When soil temperatures drop below freezing, liquid soil water turns into ice, altering the soil's dielectric properties, which is a key factor in microwave remote sensing of soil conditions. Conversely, as temperatures rise above freezing, the ice in the soil melts, reintroducing liquid water and activating various ecological and hydrological processes. The freeze/thaw cycle significantly influences energy, water, and mass exchanges between the land surface and the atmosphere, affecting surface runoff, plant growth, soil respiration, and other crucial environmental factors. In remote sensing, detecting these freeze/thaw states is important for accurately estimating soil moisture and understanding surface conditions. Frozen soil can be detected using changes in brightness temperature and backscatter observed by microwave sensors
Level 2 pre-processed (L2P): this is a designation of satellite data processing level. “Level 2” means geophysical variables derived from Level 1 source data on the same grid (typically the satellite swath projection). “Pre-processed” means ancillary data and metadata added following GHRSST Data Specification.
Level 3 /uncollated/collated/super-collated (L3U/L3C/L3S): this is a designation of satellite data processing level. “Level 3” indicates that the satellite data is a geophysical quantity (retrieval) that has been averaged where data are available to a regular grid in time and space. “Uncollated” means L2 data granules have been remapped to a regular latitude/longitude grid without combining observations from multiple source files. L3U files will typically be “sparse” corresponding to a single satellite orbit. “Collated” means observations from multiple images/orbits from a single instrument combined into a space-time grid. A typical L3C file may contain all the observations from a single instrument in a 24-hour period. “Super-collated” indicates that (for those periods where more than one satellite data stream delivering the geophysical quantity has been available) the data from more than one satellite have been gridded together into a single grid-cell estimate, where relevant.
Passive (soil moisture) retrieval: the process of modelling soil moisture from radiometer measurements. The measurand of passive microwave remote sensing is called “brightness temperature”. The retrieval model in the context of Copernicus Climate Change Service (C3S) soil moisture is generally the Land Parameter Retrieval Model.
Polarisation: The polarization of microwaves refers to the orientation of the electric field vector of the transmitted beam with respect to the horizontal direction. the beam is said to be "V" polarized when the electric field vector oscillates along a direction perpendicular to the horizontal direction and "H" polarized when the electric field vector oscillates along a direction parallel to the horizontal direction.
Radiometer: Spaceborne radiometers are satellite-carried sensors that measure energy in the microwave domain emitted by the Earth. The amount of radiation emitted by an object in the microwave domain (~1-20 GHz). The observed quantity is called “brightness temperature” and depends on kinetic temperature of an object and its emissivity. Due to the high emissivity of water compared to dry matter, radiometer measurements of Earth’s surface contain information in the water content in the observed area.
Root Zone Soil Moisture: Water content in the 0–1 m soil layer where most plant roots extract water, expressed as volumetric soil moisture (m³m-³).
Scatterometer: Spaceborne scatterometers are satellite-carried sensors that use microwave radars to measure the reflection or scattering effect produced by scanning a large area on the surface of the Earth. The initially submitted pulses of energy are reflected by the Earth’s surface depending on its geometrical and geophysical properties in the target area. The received energy is called “backscatter”. Soil moisture retrieval relies on the fact that wet soils have a higher reflectivity (and therefore backscatter) than dry soils due to the high dielectric constant of liquid water compared to dry matter.
Surface Soil Moisture: The water content in the surface layer. There is no common definition of the surface layer, but it is generally assumed to range between 0.02-0.05 m. It is given in volumetric soil moisture (m³m-³) or percentage of saturation (%).
Transmissivity is a measure of how much an object allows microwave radiation to pass through it. In the context of soil moisture retrieval, it represents the fraction of radiation emanating from the soil that is not absorbed or scattered (and therefore masked) by the vegetation layer as it travels upwards to the sensor. Transmissivity varies across frequency bands, which show a different level of attenuation by vegetation: Longer wavelengths, like L-band (around 1.4 GHz), generally have a greater penetration depth through vegetation compared to shorter wavelengths (e.g., X-band).
Uncertainty: “Satellite soil moisture retrievals […] usually contain considerable systematic errors which, especially for model calibration and refinement, provide better insight when estimated separate from random errors. Therefore, we use the term bias to refer to systematic errors only and the term uncertainty to refer to random errors only, specifically to their standard deviation (or variance)” (Gruber et al., 2020).
Executive summary
This document is the Algorithm Theoretical Basis Document (ATBD) for products Copernicus Climate Change Service (C3S) Satellite Surface Soil Moisture (SSM), Freeze/Thaw (F/T) and Root Zone Soil Moisture (RZSM), version v202505, produced by TU Wien, EODC, and Planet Labs from a large set of active and passive microwave remote sensing instruments. It describes the physical and mathematical basis of algorithms and systems used to generate the ACTIVE SSM, PASSIVE SSM, COMBINED SSM, F/T and RZSM products, including the scientific justification for the algorithms (i.e. underlying physics) selected to derive the product, an outline of the approach implemented (inc. data dependencies; use and source of auxiliary data; all aspects of data processing and quality control; calibration and bias adjustment; filtering, interpolation, transformation, etc.), as well as a description of the error propagation and identification of major sources of uncertainty, and a listing of the assumptions and limitations of the algorithm. It contains sufficient detail to be able to serve as a reference document for implementing the production systems, including the choice of the Fundamental Data Record used as baseline reference for L3/L4 products, and ensure full traceability to the source.
The C3S Soil Moisture production system (C3S SM) is based on the algorithms initially developed within European Space Agency’s (ESA) Climate Change Initiative (CCI) Soil Moisture Project (Dorigo et al., 2024) and has been updated and re-engineered to enable the provision of soil moisture retrievals on a near-real-time basis. In this context “near real time” refers to the provision of soil moisture information with a minimum delay of 10 days and a maximum of 23 days after sensing.
This document relates to the C3S Soil Moisture production system used to generate product versions v202505 and is based on the algorithm developed for ESA CCI SM v09.
Chapter 1 provides an overview of the satellite instruments that are used for the production of the soil moisture data, which is a combination of both passive and active microwave sensors dating back to the year 1978. Chapter 2 presents an overview of all the auxiliary data that is used during the generation and evaluation of the soil moisture record respectively. Chapter 3 gives an in-depth description of the algorithm used to retrieve surface soil moisture from passive microwave observations (Section 3.1) and points to relevant resources regarding active microwave retrievals from external operational sources (Section 3.2). It also describes the merging strategy applied in C3S surface soil moisture, i.e. how the retrievals from different satellite sensors are combined into a consistent merged surface soil moisture database (Section 3.3). Freeze/thaw and root zone soil moisture retrieval algorithms are described in Sections 3.4 and 3.5, respectively. Finally, chapter 4 briefly describes the output fields of the final soil moisture products.
Instruments
The soil moisture (SM) Climate Data Record (CDR) / Interim Climate Data Record (ICDR) comprise of the following products:
- The surface soil moisture (SSM) products are termed "ACTIVE" (based on the merged scatterometer soil moisture products), "PASSIVE" (based on the merged radiometer soil moisture products) and "COMBINED" (using both input sensor types).
- The freeze/thaw (F/T) and,
- Root zone soil moisture (RZSM) products apply the same input data as the COMBINED SSM product.
SSM and RZSM products are provided at three different temporal sampling frequencies (daily, dekadal and monthly) while F/T product is provided only at daily temporal sampling frequency. A schematic overview of the instruments used in the generation of the CDR/ICDR is provided in Figure 1, with information about the sensor characteristics being provided in Sections 1.1 and 1.2.
Figure 1: Temporal coverage of input products used to construct the CDR/ICDR: ACTIVE (blue), PASSIVE (red), COMBINED (red and blue) products.
Passive Microwave Systems
Satellite missions from different space agencies during the last 40+ years were equipped with microwave radiometers to measure electromagnetic radiation emitted by Earth at different frequencies in the microwave domain. A selection of frequency bands (L-, C-, X-, and Ku-band) allows the retrieval of soil moisture information from these measurements using the Land Parameter Retrieval Model (LPRM; described in more detail in Section 3.1). The model is applied to all hereafter listed passive sensors as part of the production of Copernicus Climate Change Service (C3S) SM products. An overview over the data providers, data properties, used sensors and their main characteristics are given in the following sections.
Nimbus-7 SMMR (NASA)
Originating System | Scanning Multichannel Microwave Radiometer on board Nimbus 7 |
|---|---|
Data class | Earth observation |
Sensor Type and key technical characteristics |
|
Data Availability and Coverage | October 1978 – August 1987, 180°W 90°S – 180°E 90°N
|
Source Data Name and Product Technical Specifications | SMMR Level 1b
|
Data Quantity | Total volume is ~90 GB |
Data Quality and Reliability | Instrument specification:
Validation reports
|
Ordering and delivery mechanism | Ordering via NSIDC Data Centre Delivery is possible via
|
Access conditions and pricing | Freely accessible |
Issues | In 1986 there is a high frequency of bad antenna counts, especially during and for some time after the Special Operations Period (April – October 1986). Interpolating radiometric samples within scans and between adjacent scans tends to smear the effect of these "bad" antenna counts, which are most noticeable in browse image maps of 6.6 GHz horizontal polarization data. |
DMSP-SSM/I (NESDIS NOAA)
Originating System | the Special Sensor Microwave Imager (SSM/I) of the Defense Meteorological Satellite Program (DMSP) |
|---|---|
Data class | Earth observation |
Sensor Type and key technical characteristics |
|
Data Availability and Coverage | F08 (Jun 87 – Aug 1991), F10 (Dec 1990 – Nov 1997), F11 (Nov 1991 – Dec 2000), F13 (Mar 1995 – Now), F14 (May 1997 – Aug 2008), F15 (Dec 1999, Now), 180°W 90°S – 180°E 90°N
|
Source Data Name and Product Technical Specifications | Version 6 20+ years SSMI brightness temperatures
|
Data Quantity | ~100 GB/year for each sensor (L1) |
Data Quality and Reliability | Instrument specification:
Validation reports
|
Ordering and delivery mechanism | Ordering via SSMI Data Centre [No longer available online] Delivery is possible via
|
Access conditions and pricing | Freely accessible |
Issues | The data used here is based on a series of different satellites. |
TRMM-TMI (NASA/JAXA)
Originating System | Tropical Rainfall Measurement Mission Microwave Imager (TRMM-TMI) |
|---|---|
Data class | Earth observation |
Sensor Type and key technical characteristics |
|
Data Availability and Coverage | November 1997 – April 2015, 180°W 38°S – 180°E 38°N
|
Source Data Name and Product Technical Specifications | Level 1 b calibrated brightness temperatures TRMM TMI
|
Data Quantity | 100 GB per year (L1) |
Data Quality and Reliability | Instrument specification:
Validation reports
|
Ordering and delivery mechanism | Ordering via NASA GES DISC Data Centre
|
Access conditions and pricing | Freely accessible |
Issues | The satellite observations slightly changed after a boost in August 2001 and there is a pre-boost dataset (before 7-8-2001) and a post boost dataset (after 24-8-2001). TRMM satellite orbit declining March/April 2015. |
AQUA-AMSR-E
Originating System | The Advanced Microwave Scanning Radiometer onboard the AQUA satellite |
|---|---|
Data class | Earth observation |
Sensor Type and key technical characteristics |
|
Data Availability and Coverage | June 2002 – October 2011, 180°W 89.24°S – 180°E 89.24°N
|
Source Data Name and Product Technical Specifications | AMSR-E/Aqua L2A Global Swath Spatially-Resampled Brightness Temperatures
|
Data Quantity | ~1 TB per year (L2A) |
Data Quality and Reliability | Instrument specification:
Validation reports
|
Ordering and delivery mechanism | Ordering via NASA GES DISC or NSIDC data center:
|
Access conditions and pricing | Freely accessible |
Issues | Versions older than V07 had significant geolocation problems (a few km off). |
Coriolis WindSat (Naval Research Laboratory)
Originating System | WindSat Radiometer onboard the Coriolis satellite |
|---|---|
Data class | Earth observation |
Sensor Type and key technical characteristics |
|
Data Availability and Coverage | January 2003 – present, 180°W 90°S – 180°E 90°N A summary of the data can be found on
|
Source Data Name and Product Technical Specifications | WindSat Brightness Temperatures Technical Specification
|
Data Quantity | ~75 GB per year (L1) |
Data Quality and Reliability | Instrument specification:
|
Ordering and delivery mechanism | Ordering via Naval Research laboratory Please contact windsat@nrl.navy.mil Delivery is possible via Hard disk |
Access conditions and pricing | Access to brightness temperature data is restricted by data provider and only possible upon request. |
Issues | Access to data from February 2003 to July 2012 was given but is not public. |
GCOM-W1 AMSR-2 (JAXA)
Originating System | The second Advanced Microwave Scanning Radiometer onboard the GCOM-W1 satellite |
|---|---|
Data class | Earth observation |
Sensor Type and key technical characteristics |
|
Data Availability and Coverage | Launch 2012 - Present, 180°W 89.24°S – 180°E 89.24°N |
Source Data Name and Product Technical Specifications | LPRM/AMSR2/GCOM-W1 L2 Surface Soil Moisture, Ancillary Params, and QC |
Data Quantity | ~500 GB per year (L1) |
Data Quality and Reliability | Instrument specification:
|
Ordering and delivery mechanism | Please see |
Access conditions and pricing | Freely accessible |
Issues | N/A |
SMOS (ESA)
Originating System | Soil Moisture and Ocean Salinity Mission |
|---|---|
Data class | Earth observation |
Sensor Type and key technical characteristics |
|
Data Availability and Coverage | November 2009 – Now, 180°W 90°S – 180°E 90°N |
Source Data Name and Product Technical Specifications | SMOS Level 3 brightness temperatures (MIR_CDF3TA & MIR_CDF3TD datasets for ascending and descending overpass)
|
Data Quantity | ~5 Tb per year (L1) |
Data Quality and Reliability | Instrument specification:
|
Ordering and delivery mechanism | Ordering via ESA at https://earth.esa.int/eogateway/missions/smos/data (URL link last accessed 25/03/2025)
|
Access conditions and pricing | Freely accessible |
Issues | Data is continuously reprocessed |
SMAP (NASA)
Originating System | Soil Moisture Active Passive Mission |
|---|---|
Data class | Earth observation |
Sensor Type and key technical characteristics |
|
Data Availability and Coverage | March 2015 – cont., N: 85.044, S: -85.044, E: 180, W: -180 |
Source Data Name and Product Technical Specifications | SMAP L3 Radiometer Global Daily 36 km EASE-Grid Soil Moisture (SPL3SMP, ascending and descending overpass) (O'Neill et al. (2020a))
|
Data Quantity | 10GB/year (Level 3, daily data) |
Data Quality and Reliability | Calibration and Validation for the L2/3_SM_P Version 7 and L2/3_SM_P_E Version 4 Data Products (O'Neill et al. (2020c)) |
Ordering and delivery mechanism | Download via NSIDC at https://nsidc.org/data/SPL3SMP (URL link last accessed 25/03/2025) |
Access conditions and pricing | Freely accessible |
Issues | Data is continuously reprocessed |
FengYun 3B/C/D (CMA/NSMC)
Originating System | FengYun 3 Series |
|---|---|
Data class | Earth observation |
Sensor Type and key technical characteristics | MWRI Micro-Wave Radiation Imager
Sun-synchronous orbit, Altitude: 836 km Design life 3 years with a goal of 4 years |
Data Availability and Coverage | FY3B: ECT 14:45 asc; available 2011-2021 (decommissioned) |
Source Data Name and Product Technical Specifications | FengYun-3 swath based brightness temperature data from Ka- and X-band |
Data Quantity | ~200 GB per year (L1) |
Data Quality and Reliability | The FengYun-3 Microwave Radiation Imager On-Orbit Verification (Yang et al., 2011) |
Ordering and delivery mechanism | Ordering through data portal (limited to 100 GB per day) |
Access conditions and pricing | Access is via registration and made available for use within the projects via the dragon 5 cooperation https://dragon5.esa.int/ (URL link last accessed 25/03/2025) |
Issues | Documentation is largely missing / not publicly accessible, no programmatic Near real time (NRT) data access possible at the moment, hence no inclusion in C3S SM ICDRs. |
GPM (NASA, JAXA)
Originating System | GPM Microwave Imager (GMI) onboard the GPM core observatory. Satellite Evolution of TMI on TRMM |
|---|---|
Data class | Earth observation |
Sensor Type and key technical characteristics | GPM Microwave Imager, Multi-purpose imager, with emphasis on precipitation
|
Data Availability and Coverage | GPM Core Observatory launched on February 27th, 2014, data is available from 2014-03-04 to presentNear-global coverage in 2 days; high latitudes (> 70°) not covered. |
Source Data Name and Product Technical Specifications | Raw data: GPM GMI XCAL Common Calibrated Brightness Temperatures L1BASE 1.5 hours 13 km V07 (GPM_BASEGPMGMI_XCAL)
|
Data Quantity | 165.0 MB per file (Brightness Temperature level)~2.5 GB / year (L3 LPRM derived soil moisture data) |
Data Quality and Reliability |
|
Ordering and delivery mechanism | Access through GES DISC portal (HTTP) at https://disc.gsfc.nasa.gov/ (URL link last accessed 25/03/2025) |
Access conditions and pricing | Freely accessible |
Issues | Data is continuously reprocessed |
Active Microwave Systems
Soil moisture retrieval from radar scatterometers was first done for European Space Agency's (ESA) European Remote Sensing Satellite (ERS) satellites (Wagner 1998; Wagner et al., 1999b). Since then, the Water Retrieval Package (WARP) was developed based on the TU Wien method to derive soil moisture from backscatter measurements of European Organisation for the Exploitation of Meteorological Satellites (EUMETSAT) Meteorological Operational Satellite (MetOp) Advanced Scatterometer (ASCAT) sensors (H SAF, 2018a, H SAF, 2018b), which is now distributed by H SAF1 as an operational product in near-real-time and used in the generation of C3S soil moisture. Soil moisture products from synthetic aperture radar (SAR) measurements (such as Sentinel-1) are gaining popularity due to their higher spatial resolution and therefore potential new applications. They are, however, not yet part of the C3S records.
ERS AMI (ESA)
Originating System | Active Microwave Instrument (AMI) Wind Scatterometer (WS) on-board ERS-1 and ERS-2 |
|---|---|
Data class | Earth Observation data |
Sensor Type and key technical characteristics |
|
Data Availability and Coverage | IFREMER |
Source Data Name and Product Technical Specifications | IFREMER
ESA Rolling Archive ERS.WSC.UWI (fast delivery product BUFR Format)
|
Data Quantity | ~32 GB |
Data Quality and Reliability | Instrument specification
|
Ordering and delivery mechanism | IFREMER
|
Access conditions and pricing | Freely accessible |
Issues | Due to the loss of gyroscopes onboard of ERS-2 in January 2001, data from 2001/01/17 to 2003/08/13 was initially lost but partly restored later on. |
ASCAT Metop-A (EUMETSAT)
Originating System | Advanced Scatterometer (ASCAT) onboard Metop-A |
|---|---|
Data class | Earth observation |
Sensor Type and key technical characteristics |
|
Data Availability and Coverage | 2007/01/01 – 2021/11/15., 180°W 90°S – 180°E 90°N
|
Source Data Name and Product Technical Specifications | ASCAT Soil Moisture at 12.5 km (EUMETSAT) H121 SSM CDR v8 12.5 km (H SAF) Technical Specification
|
Data Quantity | ~100 GB/year for L2 soil moisture 25 km resolution |
Data Quality and Reliability | Instrument specification
|
Ordering and delivery mechanism | Ordering via EUMETSAT Data Centre
|
Access conditions and pricing | EUMETSAT data policy |
Issues | ASCAT-A was decommissioned as of 15 November 2021 |
ASCAT Metop-B (EUMETSAT)
Originating System | Advanced Scatterometer (ASCAT) onboard Metop-B |
|---|---|
Data class | Earth observation |
Sensor Type and key technical characteristics |
|
Data Availability and Coverage | 2012/11/06 – cont., 180°W 90°S – 180°E 90°N |
Source Data Name and Product Technical Specifications | ASCAT Soil Moisture at 12.5 km (EUMETSAT) H121 SSM CDR v8 12.5 km (H SAF) ASCAT Soil Moisture at 12.5 km (EUMETSAT) H139 SSM CDR v8 EXT 12.5 km (H SAF) ASCAT Soil Moisture at 12.5 km (EUMETSAT) H29 SSM NRT 12.5 km V2 (H SAF) Technical Specification
|
Data Quantity | ~100 GB/year for L2 soil moisture 25 km resolution |
Data Quality and Reliability | Instrument specification
Validation reports
|
Ordering and delivery mechanism | Ordering via EUMETSAT Data Centre
|
Access conditions and pricing | EUMETSAT data policy |
Issues | Intercalibration between MetOp-B and MetOp-A NRT data is only available after June 2015 because of which MetOp-B can only be used after this date in C3S SM. A backward processing of MetOp-B may be performed once intercalibrated data become available from H-SAF/EUMETSAT. |
ASCAT Metop-C (EUMETSAT)
Originating System | Advanced Scatterometer (ASCAT) onboard Metop-C |
|---|---|
Data class | Earth Observations |
Sensor Type and key technical characteristics |
|
Data Availability and Coverage | 2018/11 – cont., 180°W 90°S – 180°E 90°N (global) |
Source Data Name and Product Technical Specifications | ASCAT Soil Moisture at 12.5 km (EUMETSAT) H121 SSM CDR v8 12.5 km (H SAF) ASCAT Soil Moisture at 12.5 km (EUMETSAT) H139 SSM CDR v8 EXT 12.5 km (H SAF) ASCAT Soil Moisture at 12.5 km (EUMETSAT) H29 SSM NRT 12.5 km V2 (H SAF) Technical Specification
Formats: Values in grid points of specified coordinates in the orbital projection (BUFR, EPS Native, NetCDF) |
Data Quantity | ~100 GB/year for L2 soil moisture 25 km resolution |
Data Quality and Reliability | Accuracy: threshold S/N 3 dB, target S/N 3 dB, optimal S/N 6 dB |
Ordering and delivery mechanism | Dissemination: FTP, EUMETCast (type NRT) |
Access conditions and pricing | EUMETSAT data policy |
Issues | N/A |
Input and auxiliary data
In the following an overview of the input and auxiliary data is provided. A division is made between data which is used as input for data production (Sections 2.1 and 2.2) and for validation activities (Section 2.3).
Advisory flags
The following section describes datasets that are used to generate the advisory flags provided as additional information to the soil moisture products. The advisory flags are not provided as part of the soil moisture datasets but only as datasets to support interpretation and analysis of the soil moisture products.
SSM/I-SSMIS EASE-Grid Daily Global Ice Concentration and Snow Extent
Originating System | Special Sensor Microwave Imager (SSM/I) and Special Sensor Microwave Imager/Sounder (SSMIS) |
|---|---|
Data class | Earth observation |
Sensor Type and key technical characteristics | The SSM/I is a seven-channel, four-frequency, orthogonally polarized, passive microwave radiometric system that measures atmospheric, ocean and terrain microwave brightness temperatures at 19.35, 22.2, 37.0, and 85.5 GHz. |
Data Availability and Coverage | 1995/05/04 – cont., 180°W 90°S – 180°E 90°N |
Source Data Name and Product Technical Specifications | SSM/I-SSMIS EASE-Grid Daily Global Ice Concentration and Snow Extent |
Data Quantity | ~800 MB/year |
Data Quality and Reliability | |
Ordering and delivery mechanism | Data are available via FTP over Internet |
Access conditions and pricing | Freely accessible |
Issues | N/A |
Global Lakes and Wetlands Database (GLWD)
Originating System | See Table 1 in Lehner and Döll (2004) |
|---|---|
Data class | GIS database |
Sensor Type and key technical characteristics | Organisation in three levels: |
Data Availability and Coverage | Global (except Antarctica) |
Source Data Name and Product Technical Specifications | GLWD https://www.worldwildlife.org/pages/global-lakes-and-wetlands-database (URL links last accessed 25/03/2025) |
Data Quantity | ~50 MB |
Data Quality and Reliability | More information is provided in Lehner, B. & Döll, P., 2004. |
Ordering and delivery mechanism | Download from FTP |
Access conditions and pricing | GLWD is available for non-commercial scientific, conservation, and educational purposes. |
Issues | N/A |
Global 30 Arc-Second Elevation (GTOPO30)
Originating System | GTOPO30 is based on data derived from 8 sources of elevation information, including vector and raster data sets |
|---|---|
Data class | GIS database |
Sensor Type and key technical characteristics | Digital Terrain Elevation Data (DTED) is a raster topographic data base with a horizontal grid spacing of 3-arc seconds (approximately 90 meters) produced by the National Imagery and Mapping Agency (NIMA) (formerly the Defense Mapping Agency). |
Data Availability and Coverage | Global |
Source Data Name and Product Technical Specifications | |
Data Quantity | ~3 GB |
Data Quality and Reliability | ±650 m (Vertical) |
Ordering and delivery mechanism | USGS Earth Explorer (https://earthexplorer.usgs.gov/, URL links last accessed 25/03/2025) Global 30 Arc-Second Elevation (GTOPO30) Digital Object Identifier (DOI) number: /10.5066/F7DF6PQS (URL links last accessed 25/03/2025) |
Access conditions and pricing | Free |
Issues | N/A |
Merging Framework
The following data sets are used for merging L3 satellite soil moisture products into the harmonised C3S soil moisture records.
Global Land Data Assimilation System (GLDAS) V2.0
GLDAS Noah is used in the Triple Collocation Analysis (TCA) step to estimate random uncertainties of the satellite products before merging. GLDAS Noah also acts as the scaling reference for the COMBINED soil moisture product and is used there to harmonize all sensor time series via Cumulative Distribution Function (CDF) matching.
Originating System | The forcing data set combines multiple data sets for the period of January 1, 1979 to present |
|---|---|
Data class | Water and energy budget components, forcing data |
Sensor Type and key technical characteristics | Spatial resolution: 0.25° |
Data Availability and Coverage | 1948 – 2000 for 0.25°x0.25° |
Source Data Name and Product Technical Specifications | Global Land Data Assimilation System: |
Data Quantity | 3-hourly data |
Data Quality and Reliability | Please see Rodell et al. (2004); "The Global Land Data Assimilation System". |
Ordering and delivery mechanism | Data are available via https://disc.gsfc.nasa.gov/datasets?keywords=GLDAS (URL links last accessed 25/03/2025) |
Access conditions and pricing | Freely accessible |
Issues | N/A |
Global Land Data Assimilation System (GLDAS) V2.1
GLDAS Noah is used in the TCA step to estimate random uncertainties of the satellite products before merging. GLDAS Noah also acts as the scaling reference for the COMBINED product and is used there to harmonize all sensor time series via CDF matching.
Originating System | The forcing data set combines multiple data sets for the period of January 1, 2000 to present. (see Rodell et al. (2004)), Beaudoing and Rodell (2016) and https://ldas.gsfc.nasa.gov/gldas/ for details, URL links last accessed 25/03/2025) |
|---|---|
Data class | Water and energy budget components, forcing data |
Sensor Type and key technical characteristics | Spatial resolution: 0.25° |
Data Availability and Coverage | 2000 – present for 0.25°x0.25° |
Source Data Name and Product Technical Specifications | Global Land Data Assimilation System: |
Data Quantity | 3-hourly data |
Data Quality and Reliability | Rodell et al. (2004). The Global Land Data Assimilation System. |
Ordering and delivery mechanism | Data are available via https://disc.gsfc.nasa.gov/datasets?keywords=GLDAS (URL links last accessed 25/03/2025) |
Access conditions and pricing | Freely available |
Issues | None identified |
ERA 5 / ERA5-Land
European Centre for Medium-Range Weather Forecasts (ECMWF) ReAnalysis 5 (ERA5) and ERA5-Land variables are used as part of the soil moisture retrieval process (surface temperature) and act as the reference for break correction (surface soil moisture) in the production of the COMBINED product.
Originating System | ERA5 is the fifth generation ECMWF reanalysis for the global climate and weather for the past 8 decades. Data is available from 1940 onwards. ERA5 replaces the ERA-Interim reanalysis. |
|---|---|
Data class | Gridded analyses, modelled data |
Sensor Type and key technical characteristics | 1-hourly surface parameters, describing weather as well as ocean-wave and land-surface conditions, upper-air parameters covering the troposphere and stratosphere, as well as vertical integrals of atmospheric fluxes, monthly averages for many of the parameters, and other derived fields. ERA5-Land has been produced by replaying the land component of the ECMWF ERA5 climate reanalysis. |
Data Availability and Coverage | 1950 – present., 180°W 90°S – 180°E 90°N |
Product Technical Specifications | ERA5: https://doi.org/10.24381/cds.adbb2d47 (URL links last accessed 25/03/2025) |
Data Quantity | Depends upon number of variables that are required from the dataset |
Data Quality and Reliability | See Hersbach et al. (2020) and Muñoz-Sabater et al. (2021) |
Ordering and delivery mechanism | ERA5 and ERA5-Land data can be downloaded from the Copernicus Climate Data Store (CDS). Available at https://cds.climate.copernicus.eu (URL links last accessed 25/03/2025) |
Access conditions and pricing | Free for research users, see: |
Issues | N/A |
Validation data
In situ data from the International Soil Moisture Network (ISMN)
ISMN in situ observations are the primary reference to assess the quality of the satellite based C3S soil moisture products.
Originating System | In situ soil moisture measurements provided mainly from universities and regional and national organizations. Depending on the sites, there are different original data sets generated in 1952 (oldest) or to present. |
|---|---|
Data class | Ground-based in situ measurements data |
Sensor Type | The sensor types most commonly used has changed over the time period of the ISMN:
|
Data Availability and Coverage | Some of the networks began their measurements in 1952, and nowadays there are around 20 networks proving data, five of which are now providing data in near real time. See Dorigo et al. (2011) |
Source Data Name and Product Technical Specifications | The source is open due to the networks data sets are provided from different countries worldwide operated by different universities and national and regional organizations. |
Data Quantity | The temporal resolution of the data sets is very diverse depending on the site: 20 min, 30 min, hourly, 6-hourly, 12-hourly, daily and weekly.
|
Data Quality and Reliability | Each site is responsible of the quality of its data. Nevertheless, after processing the original data a Quality Control is performed with a data flagging system. See Dorigo et al. (2011) and Dorigo et al. (2021) for more information. |
Ordering and | Via ISMN data viewer providing a compressed (.zip) file at https://ismn.earth (URL links last accessed 25/03/2025) |
Access conditions and pricing | Free with previous registration and for scientific use only. Neither onward distribution nor commercial use is permitted. |
Issues | Data Formats:
|
ERA5-Land
ERA5-Land (see Chapter 2.2.3) is the main globally available, gap-free reference source for evaluating C3S soil moisture products. While ERA5 is also used in the production of the data set (during break correction; Chapter 3.3.7), it was found that no features from ERA5 are introduced to the satellite data in that step. ERA5-Land is therefore considered to be independent and is therefore used as a reference for validation.
Algorithms
Surface Soil Moisture Retrieval from PASSIVE Microwave Sensors
This chapter is largely based upon Dorigo et al. (2024).
Principles of the Land Parameter Retrieval Model
Brightness temperatures can be derived from passive microwave sensors with different radiometric characteristics. The observed brightness temperatures are converted to soil moisture values with the Land Parameter Retrieval Model (LPRM; van der Schalie et al., 2017). This model is based on a microwave radiative transfer model that links soil moisture to the observed brightness temperatures. A unique aspect of LPRM is the simultaneous retrieval of vegetation optical depth (VOD) in combination with soil moisture and surface temperature.
A result of this physical parameterisation is that any differences in frequency and incidence angle that exist among different satellite platforms are accounted for within the framework of the radiative transfer model based on global constant parameters (de Jeu et al., 2014). This important aspect makes LPRM suitable for the development of a long-term consistent soil moisture products as in the ESA CCI Soil Moisture2 and C3S Soil Moisture (SM) products.
2 https://climate.esa.int/en/projects/soil-moisture/ (URL last accessed 25/03/2025)
The different processing steps of LPRM are described in detail in the next section, while Figure 2 presents a summary flowchart of the entire methodology with the most important parameters:
① Land surface temperature (soil and vegetation, TS, TV) is based on observed Ka-band brighness temperature (Tb), or, for the SMAP and SMOS satellites (which operate exclusively in L-band), reanalysis temperature fields.
② Atmospheric effects affecting the measured brighness temperature, i.e., upwelling, downwelling, and extraterrestrial brighness temperature (Tu, Td, Textra) as well as atmospheric opacity (Γa) are modelled based on surface temperature from ①, the satellite incidence angle (u), and atmospheric optical depth (τa).
③ Dielectric properties (dielectric constant) for a scene with the soil moisture content θ are modelled by a dielectric mixing model, which uses Porosity (P), Wilting Point (WP), Temperature (TS), and the observation frequency (F).
④ Reflectivity is modelled for a given incidence angle (u) using the dielectric properties from ③.
⑤ Surface roughness is modelled for different soil moisture conditions (θ), considering frequency-dependent soil roughness (h1) and vegetation roughness parameters (Av, Bv), as well as an initial estimate of vegetation density (τ̅v).
⑥ The surface emissivitiy requires the surface reflectivity from ③, as well as an estimate of the surface roughness from ④, and the polarization mixing factor (Q).
⑦ Vegetation effects on brightness temperature are estimated based on the difference between horizontally and vertically polarized microwave radiation (MPDI). MPDI, emissivity from ⑤, and the single scattering albedo (ω) are used to describe vegetation optical depth (τv) and vegetation transmissvity (Γv).
⑧ The radiative transfer model uses the components from ① to ⑦ to model the received brightness temperature as observed by the satellite. The model is fitted for different soil moisture scenarios, minimizing the difference between the modelled and observed brightness temperature. Upon convergence, the model is inverted to retrieve soil moisture
Figure 2: Flowchart of the main processes of the Land Parameter Retrieval Model (LPRM). Soil moisture is solved when the observed brightness temperature equals the modelled brightness temperature as derived by the radiative transfer.
Methodology
The thermal radiation in the microwave region is emitted by all natural surfaces and is a function of both the land surface and the atmosphere. According to LPRM the observed brightness temperature (Tb ) as measured by a space borne radiometer can be described as:
Where Γa and Γv are the atmosphere and vegetation transmissivity respectively, Tb_s is the surface brightness temperature, er is the rough surface emissivity, Tb_extra , the extra-terrestrial brightness temperature and the Tb_u and Tb_d are the upwelling and downwelling atmospheric brightness temperatures. The subscript p denotes either horizontal (H) or vertical (V) polarization. The vegetation/atmosphere transmissivity is further defined in terms of the optical depth, τ v/a , and satellite incidence angle, u, such that
The upwelling brightness temperature from the atmosphere is estimated as (Bevis et al. 1992):
Were Ta is the atmospheric temperature. In LPRM the downwelling Temperature (Td ) is assumed to be equal to the upwelling temperature (Tu ) and the extraterrestrial temperature is set to 2.7 K (Ulaby et al. 1982). The radiation from a land surface (Tb_s,p ) is described according to a simple radiative transfer (Mo et al. 1982):
Where Ts and Tv are the thermodynamic temperatures of the soil and the vegetation, ω is the single scattering albedo. LPRM uses the model of Wang and Choudhury (1981) to describe the rough surface emissivity as:
rs is the surface reflectivity and p1 and p2 are opposite polarization (horizontal (H) or vertical (V)). The surface reflectivity is calculated from the Fresnel equations:
Where rs,H is the horizontal polarized reflectivity, and rs,V is the vertical polarized reflectivity and ε the complex dielectric constant of the soil surface (ε = ε' + ε"i). The dielectric constant is an electrical property of matter and is a measure of the response of a medium to an applied electric field. The dielectric constant is a complex number, containing a real (ε ') and imaginary (ε ") part. The real part determines the propagation characteristics of the energy as it passes upward through the soil, while the imaginary part determines the energy losses (Schmugge et al. 1986). There is a large contrast in dielectric constant between water and dry soil, and several dielectric mixing models have been developed to describe the relationship between soil moisture and dielectric constant (Dobson et al. 1985; Mironov et al. 2004; Peplinski et al. 1995; Wang and Schmugge 1980). Owe and Van de Griend (1998) compared the Dobson and Wang and Schmugge model and they concluded that the Wang and Schmugge model had better agreement with the laboratory dielectric constant measurements. Consequently, LPRM uses the Wang and Schmugge model, which requires information on the soil porosity (P) and wilting point (WP), observation frequency (F), TS, and θ.
A special characteristic of LPRM is the internal analytical approach to solve for the vegetation optical depth, τv (Meesters et al. 2005). This unique feature reduces the required vegetation parameters to one, the single scattering albedo. LPRM makes use of the Microwave Polarization Difference Index (MPDI) to calculate τv. The MPDI is defined as:
When one assumes that τ and ω have minimal polarization dependency at satellite scales, then the vegetation optical depth can be described as:
Where
And
By using all these equations in combination with the dielectric mixing model, soil moisture could be solved in a forward model together with a parameterization of the following parameters: atmosphere, soil and vegetation temperature (Ta , Ts , Tc ), the optical depth of the atmosphere (τa ), the roughness parameters Q and h, soil wilting point (WP) and porosity (P), and the single scattering albedo (ω).
The temperatures were estimated using Ka-band (37 GHz) observations according to the method of Holmes et al. (2009).
For the day-time (ascending) observations the following equation is used:
and for the night-time (descending):
However, since the current L-band missions do not observe the Earth at the Ka-band frequency, they still require modelled TS from land surface models as an input. Van der Schalie et al. (2021) have developed a method to replace the land surface model with data from an inter-calibrated dataset (ICTB) based on six passive microwave sensors. However, this is not yet applied to L-band data used in C3S SM.
The soil P and WP were derived from the Food and Agriculture Organisation (FAO) soil texture map available from the Harmonised World Soil Database (FAO/IIASA/ISRIC/ISS-CAS/JRC, 2009), while all the other parameters were given a fixed value. Table 1 summarizes the values used for the different frequencies.
Table 1: Values of the different parameters used in LPRM for the different frequencies
Parameter | Frequency | |||
|---|---|---|---|---|
L-band (~1.4 GHz) | C-band (~6.9 GHz) | X-band (~10.8 GHz) | Ku-band (~19 GHz) | |
τa | 0 | 0.01 | 0.01 | 0.05 |
ω | 0.12 | 0.075 | 0.075 | 0.06 |
h1 (h for Ku-band) | 1.1 to 1.3 | 1.2 | 1.2 | 0.13 |
Q | 0 | 0.115 | 0.127 | 0.14 |
AV | 0.7 | 0.3 | 0.3 | n/a |
BV | 2 | 2 | 2 | n/a |
C-, X- and Ku-band Model Parametrization
Soil moisture retrieval using higher frequencies are known to have issues in the more extreme climates, e.g. tropical regions, deserts and boreal forests. A single global parameterization function is used for L-band but leads to questionable behavior for some of the higher frequencies. For example, unnaturally high/low soil moisture values over certain land cover classes or non-valid model retrievals. Starting from LPRMv7 onwards, a variable parameterization is used. This counts for two parameters, dT (a local bias correction of the land surface temperature) and ⍵ (the single scattering albedo).
Due to more dynamic VOD behavior as compared to L-band, the VOD based vegetation correction has too much impact on the soil moisture signal from C-, X- and Ku-band. Therefore, we have studied ways to remove this effect from LPRM for the higher frequencies. Together with the renewed parameterization, the roughness has now been simplified to the soil moisture (SM) and Porosity (P) dependent:
with h = 0 when SM > P.
Prior to the optimization of the parameters, the temperature relation with Ka-band has been revisited for use in LPRMv7. Local slope and intercept have been calculated between Ka-band and the average of the ERA5-Land land surface temperature (0 cm) and ERA5-Land layer 1 soil temperature (0-7cm), see Figure 3. This dataset is known to have a good quality and the expected seasonal behavior.
Figure 3: Scaling paramters for Ka-band brightness temperature against ERA5-Land temperature. Intercept of the regression from (a) descending and (b) ascending overpass data. Slope of the regression from (c) descending and (d) ascending overpass data.
On top of this new local temperature relation, the dT is used in the optimization to correct the effective temperature from the microwave emission, assuming that the seasonal dynamics are similar to that of ERA5-Land. During testing, a variable slope has also been considered, but this gave a negligible effect on the final results. The optimization process for both parameters (simultaneously) searches for the best correlation against SMAP L-band LPRM and limits the results to datasets that had at least 90% valid retrievals between 0.01 and 0.75 m3m-3. Resulting parameterization can be found in Figure 4, with an example of the final quality: the standard deviation and the 10/90 percentiles, in Figure 5.
Figure 4: The single scattering albedo (⍵) and local bias correction of the land surface temperature (dT), results from the optimization for C- (6.9 GHZ, top row), X- (10.7 GHZ, middle row) and Ku-band (18.7 GHZ, bottom row).
Figure 5: The 10/90 percentiles (P10/P90) and standard deviation (STDEV) of the LPRMv7 soil moisture retrievals from C- (6.9 GHZ, top row), X- (10.7 GHZ, middle row) and Ku-band (18.7 GHZ, bottom row). Note that Greenland is normally not run and therefore shows artefacts that are not in the final product.
Day-time Retrievals
Since the temperature distribution within the vegetation and soil is not in equilibrium during the 1:30 am observation period, and the situation varies throughout the seasons, a standard approach of optimizing LPRM left too many regions without a functional parameterization. Therefore, an alternative was found that corrects the day-time brightness temperatures to night-time values and is applied to all frequencies including Ka-band for the temperature retrieval. This was done using the following steps:
- Linearly interpolated dataset for day-time and night-time to allow sufficient overlap.
- Calculate the median ratio between day-time and night-time over a 3-week (±10 day) window. The median was chosen over the mean to reduce the impact of strong individual events between overpasses.
- Apply this ratio to correct the day-time data to night-time.
- Apply LPRM to the dataset using the exact same parameterization as for night-time retrievals.
The resulting skill of the day-time retrievals from AMSR2 using LPRMv7.0 can be seen in Figure 6. The day-time values are still reaching good (r > 0.6) correlations over much of the same regions where the night-time performs well against SMAP Level 4 SM. Because the theoretical issue of non-existing thermal equilibrium for midday observations remains present within the vegetation and soil surface, an increase in overall noise within the day-time datasets does lead to an average decrease in correlation, therefore, when available, the night-time retrievals still have a preference.
Figure 6: Visualized correlation of night-time (descending: Desc.) and day-time (ascending: Asc.) observations against SMAP Level 4 SM, for C- (6.9 GHZ, top row), X- (10.7 GHZ, middle row) and Ku-band (18.7 GHZ, bottom row) from AMSR2, using LPRMv7.0.
Barren grounds classification
Very dry conditions in deserts and other barren areas lead to subsurface scattering phenomena and complicate the process of defining a correct land surface temperature due to the increased sensing depth. To account for uncertainties in very dry soils, we detect barren soil conditions and flag them. A pixel is classified as barren following Eq. 16:
Barren grounds are flagged in a similar manner as the snow/frozen conditions described in chapter 3.4.1 (Van der Vliet et al., 2020). Figure 7 shows the fraction of observations flagged as barren for various months of the year. Deserted regions are clearly visible, as well as seasonal changes in barren soil conditions.
Figure 7: Fraction of the observations per pixel that have been flagged as barren soil for four different months. The fraction has been computed over all observations for each month over 2012-2024.
Known Limitations
The known limitations in deriving soil moisture from passive microwave observations are listed and described in detail in this section. These issues do not only apply to the current C3S CDR and ICDR soil moisture dataset releases but also to soil moisture retrieval from passive microwave observations in general.
Vegetation
Vegetation affects the microwave emission, and under a sufficiently dense canopy the emitted soil radiation will become completely masked by the overlying vegetation. The simultaneously derived vegetation optical depth can be used to detect areas with excessive vegetation, of which the boundary varies with observation frequency.
Figure 8 gives an example of the relationship between the analytical error estimate in soil moisture as described in the previous section and vegetation optical depth. This figure shows larger error values in the retrieved soil moisture product for higher frequencies at similar vegetation optical depth values. For example, for a specific agricultural crop (VOD=0.5), the error estimate for the soil moisture retrieval in the C-band is around 0.07 m3·m−3; in the X-band, this is around 0.11 m3·m−3, and in the Ku-band, this is around 0.16 m3·m−3. All relevant frequency bands show an increasing error with increasing vegetation optical depth. This is consistent with theoretical predictions, which indicate that, as the vegetation biomass increases, the observed soil emission decreases, and therefore, the soil moisture information contained in the microwave signal decreases (Owe et al., 2001).
In addition, retrievals from the higher frequency observations (i.e., X- and Ku-bands) show adverse influence by a much thinner vegetation cover. Soil Moisture retrievals with a soil moisture error estimate beyond 0.2 m3m-3 are considered to be unreliable and are masked out.
Figure 8: Error of soil moisture as related to the vegetation optical depth for 3 different frequency bands (from Parinussa et al., 2011).
For the L-band based retrievals from SMOS, the vegetation influence is less as compared to the C-, X- and Ku-band retrievals, which can be seen from the Rvalue and TCA results in Figure 9 (top). In Figure 9 (bottom), the SMOS LPRM and AMSR-E LPRM (based on C-band) are included and show more stable results over dense vegetation, i.e. Normalized Difference Vegetation Index (NDVI) values of over 0.45.
Figure 9: Triple collocation analysis (TCA: top) and R-value results (bottom) for several soil moisture datasets, including SMOS LPRM and AMSR-E LPRM, for changing vegetation density (NDVI). Based on Van der Schalie et al. (2018).
Water bodies
Water bodies within the satellite footprint can strongly affect the observed brightness temperature due to the high dielectric properties of water. Especially when the size of a water body changes over time, they can dominate the signal. LPRM uses a 5 % water body threshold based on MODIS observations and pixels with more than 5 % surface water are masked (Owe et al., 2008).
Rainfall
Rainstorms during the satellite overpass can strongly affect the brightness temperature observations, and therefore should be flagged in LPRM. Ongoing investigations are done to define a proper filtering mechanism derived from the passive microwave observations themselves. Currently, only strong events are removed due to its effect on the retrieved temperature from Ka-band, which then drops below 274.15K.
Radio Frequency interference
Natural emission in several low frequency bands is affected by artificial sources, so called Radio Frequency Interference (RFI). As a diagnostic for possible errors, an RFI index is calculated according to De Nijs et al. (2015). Most passive microwave sensors that are used for soil moisture retrieval observe in several frequencies. This allows LPRM to switch to higher frequencies in areas affected by RFI.
The new methodology that is now used for RFI detection uses the estimation of the standard error between two different frequencies. It uses both the correlation coefficient between two observations and the individual standard deviation to determine the standard error in Kelvin. A threshold value of 3 Kelvin is used to detect RFI. This method does not produce false positives in extreme environments and is more sensitive to weak RFI signals in relation to the traditional methods (e.g. Li et al., 2004).
As the currently integrated SMOS mission does not have multiple frequencies to apply this method, here we base the filtering on the RFI probability information that is supplied by in the SMOS Level 3 data. SMAP, by using different channels around 1.4GHz, already has an internal mitigation of RFI that removes almost all occurrence of RFI, therefore no extra filtering is needed for use with the C3S SM.
Updated temperature input from Ka-band observations
The land surface temperature plays a unique role in solving the radiative transfer model and therefore directly influences the quality of the soil moisture retrievals. The current linear regression to link Ka-band measurements to the effective soil temperature has been adjusted and optimized by Parinussa et al. (2016) for day-time observations (Figure 10). This is done using an optimisation procedure for soil moisture retrievals through a quasi-global precipitation-based verification technique, the so-called Rvalue metric. In this optimisation, different biases were locally applied to the existing linear regression and final results have been used to create an updated global linear regression. The focus of this study was to improve the skill to capture the temporal dynamics of the soil moisture. After the updated linear regression for the land surface temperature, the Rvalue increased on average with 16.5% and the triple collocation analysis showed an average reduction in Root Mean Square Error (RMSE) of 15.3%, showing an improved skill in day-time retrievals from LPRM.
Figure 10: (a) comparison of R-value with the old and new day-time land surface temperature binned over NDVI, (b) the difference in R-value compared to the old temperature parameterisation in [%].
This explorative work showed the high impact of temperature on the quality of the LPRM retrievals. Secondly, there are issues with (seasonal) bias in the effective temperature derived from Ka-band using a linear regression method, which are caused by the seasonal changes in soil moisture, vegetation cover and atmospheric composition. The day-time retrieval has been finally integrated with LPRM as of version 7.0, according to the methodology detailed in Section 3.1.4 .
In order to remove model dependency for the L-band soil moisture retrievals, we have collocated Ka-band observations from other satellites to SMAP and SMOS. This way, temperature input to the L-band missions is taken from actual satellite observations. This also allows to apply the new filtering methodology developed by Van der Vliet et al. (2020).
Surface Soil Moisture Retrieval from ACTIVE Microwave Sensors
The active microwave soil moisture products utilized in the generation of the C3S soil moisture datasets are obtained from external operational sources as follows:
- ERS-1 AMI surface soil moisture products have been generated at TU Wien (2013) utilizing change detection method described in Wagner et al. 1999b.
- ERS-2 AMI surface soil moisture data sets stem from reprocessing activities which have been carried out within ESA's SCIRoCCo project3 (Crapolicchio et al., 2016). The ERS-2 data set used in all ESA CCI SM versions is the ERS.SSM.H.TS 25 km soil moisture time series product (ESA, 2017).
- Metop ASCAT surface soil moisture data sets stem from the EUMETSAT Satellite Application Facility on Support to Operational Hydrology and Water Management (H SAF).
A detailed overview of the retrieval methodology employed in the generation of the Surface Soil Moisture products from the ERS-1 AMI instrument is provided in Wagner et al. 1999b, for the Surface Soil Moisture products from the ERS-2 AMI instrument please refer to Crapolicchio et al. 2004, and for the ASCAT derived products an overview of the retrieval methodology can be found in H-SAF 2018c.
3 https://earth.esa.int/eogateway/activities/scirocco (URL last accessed 25/03/2025)
Surface Soil Moisture Merging Strategy
This chapter is largely based upon Dorigo et al. (2024).
Principle of the merging process
The generation of the long-term soil moisture data set involves three steps (as detailed in Figure 11): (1) merging the original passive microwave soil moisture products into one product, (2) merging the original active microwave soil moisture products into one product, and (3) merging all original active and passive microwave soil moisture products into one. The input datasets considered for generating the merged soil moisture product are outlined in Figure 1.
- Scatterometer-based soil moisture products
- Sensors: ERS-1/2 and Metop-A/B/C ASCAT
- Retrieval method: TU Wien change detection method (Wagner et al. 1999b; H-SAF 2018c)
- Time span: 1991 – now
- Radiometer-based soil moisture products
- Sensors: SMMR, SSM/I, TRMM, AMSR-E, AMSR2, WindSat, SMOS, SMAP, FengYun 3B/C/D, GPM
- Retrieval method: VUA-NASA LPRM v6 and v7 model (Owe et al. 2008; van der Schalie et al. 2016)
- Time span: 1978 – now
- Modelled 0 – 10 cm soil moisture from the Noah land surface model of the Global Land Data Assimilation System version 2.0 and v2.1 (GLDAS; Rodell et al., 2004).
- Time span: 1948 – 2010 and 2000 - Present (0.25-degree resolution)
The homogenized and merged product presents surface soil moisture with a global coverage and a spatial resolution of 0.25°. The time period spans the entire period covered by the individual sensors, i.e. 1978 – now, while measurements are provided at a 1-day sampling.
Figure 11: Overview of the merging approach from original products to the final blended ACTIVE, PASSIVE, and COMBINED microwave surface soil moisture product (Adapted from Liu et al. 2012)
Overview of processing steps
The level 2 surface soil moisture products derived from the active and passive remotely sensed data undergo a number of processing steps in the merging procedure (see Figure 12 for an overview):
- Spatial resampling and temporal resampling (including flagging and cross-flagging of observations)
- Rescaling passive and active level 2 observations into radiometer and scatterometer climatologies (for the PASSIVE and ACTIVE product), and separately rescaling all level 2 observations into a common model-based climatology (for the COMBINED product)
- Triple collocation analysis (TCA)-based error characterisation of all rescaled level 2 products. This step is performed on a seasonality basis, meaning that variations in uncertainties of different sensors within a year (e.g., due to vegetation dynamics) are captured.
- Polynomial regression between VOD and error estimates to fill spatial gaps where errors could not be reliably retrieved i.e., where TCA is deemed unreliable
- Merging rescaled passive and active time series into the PASSIVE, ACTIVE, and COMBINED products, respectively. This step is performed on a seasonality basis, meaning that intra-annually varying biases are corrected.
- Break correction algorithm applied to the merged COMBINED product (Preimesberger et al., 2021)
Figure 12: Overview of the processing steps in the C3S product generation: The merging of two or more data sets is done by weighted averaging and involves overlapping time periods, whereas the process of joining data sets only concatenates two or more data sets between the predefined time periods. *The [SSM/I, TMI] period is specified not only by the temporal, but also by the spatial latitudinal coverage. The numbers in the figure correlate to steps applied to the different satellites.
Methodology
In this section, the algorithms of the scaling and merging approach are described. Notice that several algorithms, e.g. rescaling, are used in various steps of the process, but will be described only once.
Spatial Resampling
The sensors used for the different merged products have different technical specifications (Table 2, Table 3). Obvious are the differences in spatial resolution and crossing times. Both elements need to be brought into a common reference before the actual merging can take place.
The final merged products are provided on a regular grid with a spatial resolution of 0.25° in both latitude and longitude extension. This is a trade-off between the higher resolution scatterometer data and the generally coarser passive microwave observations without leading to any under-sampling. The same resolution is often adopted by land surface models.
For the LPRM passive data, nearest neighbor resampling is performed on the radiometer input data sets to bring them into the common regular grid. Following this resampling technique, each grid point in the reference (regular grid) data set is assigned to the value of the closest grid point in the input dataset. In general, the nearest neighbor resampling algorithm can be applied to data set with regular degree grid.
For the active microwave data sets, where equidistant grid points are defined by the geo-reference location of the observation, the hamming window function is used to resample the input data to a 0.25° regular grid. The search radius is a function of latitude of the observation location, as the distance between two regular grid points reduces as the location tends towards the poles. In contrast, the active microwave data set uses the discrete global grid (DGG), where the distance between every two points is the same. This main difference between the DGG (active) and the targeted regular degree grid is rectified by using a hamming window with search radius dependent on the latitude for the spatial resampling of the active microwave data.
Table 2: Major characteristics of passive microwave instruments used C3S SM
Passive microwave products | ||||||||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|
SMMR | SSM/I(4) | TMI | AMSR-E | AMSR2 | Windsat | MIRAS | SMAP | GMI | MWRI | MWRI | MWRI | |
Platform | Nimbus 7 | DMSP | TRMM | Aqua | GCOM-W1 | Coriolis | SMOS | SMAP | GPM | FY-3B | FY-3C | FY-3D |
Product | LPRM (VanderSat) | LPRM (VanderSat) | LPRM (VanderSat) | LPRM (VanderSat) | LPRM (VanderSat) | LPRM (VanderSat) | LPRM (VanderSat) | LPRM (VanderSat) | LPRM (VanderSat) | LPRM (VanderSat) | LPRM (VanderSat) | LPRM (VanderSat) |
Product Source | NASA, Tape derived | NASA EarthData, XCAL calibrated with GPM | NASA EarthData, XCAL calibrated with GPM | JAXA, G-portal | JAXA, G-portal | Bespoke order | CATDS | NASA EarthData | NASA EarthData, XCAL calibrated with GPM | nsmc | nsmc | nsmc |
Algorithm Product version | LPRM v7.0 (2) | LPRM v7.0 (2) | LPRM v7.0 (2) | LPRM v7.0 (2) | LPRM v7.0 (2) | LPRM v7.0 (2) | LPRM v06.2 (2, 3) | LPRM v06.2 (2, 3) | LPRM v7.0 (2) | LPRM v7.0 (2) | LPRM v7.0 (2) | LPRM v7.0 (2) |
Time period used | 11/1978–8/1987 | 09/1987– 12/2007 | 01/1998– 12/2013 | 07/2002– 10/2011 | 05/2012– Present | 10/2007–7/2012 | 01/2010–Present | 04/2015-Present | 03/2014 – Present | 06/2011 – 08/2019 | 09/2013 – 02/2020 | 07/2012 – 08/2019 |
Channel used for soil moisture | 6.6 GHz | 19.3 GHz | 10.7 GHz | 6.9/10.7 GHz | 6.925/10.65 GHz | 6.8/10.7 GHz | 1.4 GHz | 1.4GHz | 10.7 GHz | 10.7 GHz | 10.7 GHz | 10.7 GHz |
Original spatial resolution(1) (km2) | 150×150 | 69 × 43 | 59 × 36 | 76 × 44 | 35 x 62 | 25 x 35 | 40 km | 38 x 49 | 19x32 | 51 x 85 | 51 x 85 | 51 x 85 |
Spatial coverage | Global | Global | N40o to S40o | Global | Global | Global | Global | Global | N70o to S70o | Global | Global | Global |
Swath width (km) | 780 | 1400 | 780/897 after boost in Aug 2001 | 1445 | 1450 | 1025 | 600 | 1000 | 931 | 1400 | 1400 | 1400 |
Equatorial crossing time | Descending: | Descending: | Varies (non polar-orbiting) | Descending: | Descending 01:31 | Descending 6:03 | Ascending 6:00 | Descending 06:00 | Varies (non polar-orbiting) | Descending: | Descending: | Descending: |
Unit | m3m-3 | m3m-3 | m3m-3 | m3m-3 | m3m-3 | m3m-3 | m3m-3 | m3m-3 | m3m-3 | m3m-3 | m3m-3 | m3m-3 |
(1) For passive microwave instruments, this stands for the footprint spatial resolution.
(2) LPRM v6.1 references: van der Schalie et al. (2016, 2017, 2018), van der Vliet (2020)
(3) LPRM v6.2 consists of a temporal extension of LPRMv6.1, including day-time retrievals.
(4) Data from SSMI/S F08, F11, F13 satellites are used
Table 3: Major characteristics of active microwave instruments and model products used in C3S SM
Active microwave products | Model product | ||||||
|---|---|---|---|---|---|---|---|
AMI-WS | AMS-WS | ASCAT | ASCAT | ASCAT | GLDAS-2-Noah | GLDAS-2-Noah | |
Platform | ERS1/2 | ERS2 | Metop-A | Metop-B | Metop-C | — | — |
Product | SSM Product (TU WIEN, 2013) | SSM Product (Crapolicchio et al., 2016) | H 119 (H-SAF 2018a and 2018b) | H 16 (H-SAF 2018a and 2018b) | H 104 (H-SAF 2018a and 2018b) | — | — |
Algorithm Product version | TU WIEN Change Detection (2) | TU WIEN Change Detection (2) | TU WIEN Change Detection (2) | WARP (H SAF) | WARP (H SAF) | V2.0 | V2.1 |
Time period used | 7/1991– 12/2006 | 5/1997– 2/2007 | 1/2007– | 07/2015–Present | 11/2018–Present | 1/1948– 12/2010 | 1/2000– present |
Channel used for soil moisture | 5.3 GHz | 5.3 GHz | 5.3 GHz | 5.3 GHz | 5.3 GHz | — | — |
Original spatial resolution(1) (km2) | 50 × 50 | 25 x 25 | 25 × 25 | 25 × 25 | 25 × 25 | 25 × 25 | 25 × 25 |
Spatial coverage | Global | Global | Global | Global | Global | Global | Global |
Swath width (km) | 500 | 500 | 1100 (550×2) | 1100 (550×2) | 1100 (550×2) | — | — |
Equatorial crossing time | Descending: | Descending 10:30 | Descending: | Descending: | Descending: | — | — |
Unit | Degree of saturation (%) | Degree of saturation (%) | Degree of saturation (%) | Degree of saturation (%) | Degree of saturation (%) | kg m-2 | kg m-2 |
(1) For active microwave instruments, this stands for the footprint spatial resolution.
(2) TU Wien change detection algorithm references for AMI-WS: Wagner et al. (1999)
Temporal Resampling
The temporal sampling of the merged product is 1 day. The reference time for the merged dataset is set at 0:00 UTC. For each day starting from the time frame center at 0:00 UTC observations within ±12 hours are considered.
The temporal resampling strategy first searches for the valid observation that is closest to the reference time. In the case that there are only invalid observations, which are flagged other than "0" (zero), within this time frame, the closest measurement among these invalid observations is selected. If there are no measurements available at all within a time frame, no value is assigned to that day. This strategy results in data gaps when no observations within ±12 hours from the reference time are available.
Starting from v202212, day-time observations are available from the passive sensors (LPRMv7). While it is planned in future dataset versions to achieve a sub-daily temporal resolution, the temporal resampling at the current stage applies indistinctly to day- and night-time observations.
Flagging
During the temporal resampling stage, flagging is applied to the datasets where relevant information is available. The key flags set during this process are 'frozen', 'high VOD' and 'Other' and these flags are propagated through the entire processing chain to the final product.
The ASCAT and ERS products include a Surface State Flag (SSF) which effectively encodes information about whether or not the surface is frozen or snow-covered. In the ESA CCI SM / C3S SM product, those soil moisture values where Bit 1 (indicating frozen conditions) in the binary representation of the SSF bitflag is active are used to flag the observation as frozen. The ASCAT and ERS products do not provide information on high VOD.
The LPRMv6.1 (and following) products provide a FLAGS field which provides information on high VOD, frozen conditions, and the performance of the LPRM algorithm. The thresholds above which VOD is considered 'high' are set based on the saturation point in the VOD signal for each sensor and band. This is the point at which the VOD value is considered to equal 100% vegetation signal. Secondly, the frozen/snow flag was applied using the new approach by Van der Vliet et al. (2020), which derives the frozen/snow conditions from Ku-, K- and Ka-band observations. In addition to this, from LPRMv7 onwards a flag for barren grounds and desert areas is included (see section 3.1.5.3). This is implemented as an advisory flag as of C3S SM v202212. Including it as a critical flag would have a big impact on the soil moisture availability in desert-prone regions. Therefore, more validation is needed to establish whether the optional usage of the barren ground flag or a more conservative version thereof (as a critical flag) is suitable in C3S SM. As of v202312, the barren ground flag is only activated at locations / times where the majority of available L3 observations are classified respectively.
A cross-flagging approach is implemented for frozen soils. This means that any frozen flags provided in any of the datasets are effectively transferred to all of the datasets. It works by reading in all of the flag data for all of the datasets, determining if the frozen flag is set in any of them and if it is, applying it to all relevant observations in all of the sensors. The same information is then also used to detive the Freeze/Thaw stand-alone product since version v202505 (chapter 3.4).
Rescaling
Due to different observation frequencies, observation principles, and retrieval techniques, the contributing soil moisture datasets are available in different observation spaces. Therefore, before merging can take place at either level, the datasets need to be rescaled into a common climatology. All soil moisture observations of each product are rescaled to the climatology of a different reference, namely AMSRE, ASCAT or GLDAS for the passive, active or combined product respectively.
Scaling is performed by using CDF matching which is a well-established method for calibrating datasets with deviating climatologies (Drusch et al. 2005; Liu et al. 2007; Liu et al. 2011; Reichle et al. 2004, Moesinger et al. 2020). CDF-matching is applied for each grid point individually and based on piece-wise linear matching. This variation of the CDF-matching technique proved to be robust also for shorter time periods (Liu et al. 2011). The matching is shown by means of an example for a grid point centred at 41.375 oN, 5.375 oW. Figure 13 shows for this location the time series of soil moisture estimates from GLDAS-Noah, AMSR-E and ASCAT, respectively. CDF-matching for this time series is performed in the following way:
- For the time-collocated data points, CDFs (Figure 14) are computed. In the passive product AMSR2 is scaled using the parameters derived from the last 3 years of AMSRE and first 3 years of AMSR2. SMAP is then scaled to the scaled AMSR2.
- If more than 400 time-collocated data points exist, for each CDF curve the 0, 5, 10, 20, 30, 40, 50, 60, 70, 80, 90, 95 and 100 percentiles are identified. Else evenly spaced percentile bins are generated such that each of them contains at least 20 observations.
- Use the n percentiles of the CDF curves to define n-1 segments. The CDF curves of these circled values are shown in Figure14(a), (b) and (c).$$slope_i = \frac{pref_{i+1} - pref_i}{psrc_{i+1} - psrc_i} \quad Eq. 17$$ $$intercept_i = pref_i - (psrc_i \ast slope_i) \quad Eq. 18$$where i=1…12, is the number of the segments, and pref is the percentile of the GLDAS-Noah data (reference), and pscr is the percentile of either AMSR-E or ASCAT data (source) respectively.
- An exception is the first and the last segment. Instead of using the first and last percentile for interpolation, the slope is derived using least squares regression. This is more robust to outliers.
- The n percentile values from the AMSR-E and ASCAT CDF curves are plotted against those of Noah (Figure 14(d) and (e)) and scaling linear equations (e.g., slope and intercept) between two consecutive percentiles are computed.
- The obtained linear equations are used to scale all observations of the target data set (i.e., also the time steps that do not have a corresponding observation in the reference data set) to the climatology of the reference data set (Figure 14(f)).$$sm_r = slope_i \ast sm + intercept_i \quad Eq. 19$$where smr is the rescaled soil moisture and sm is the original soil moisture value. slopei and intercepti are chosen depending on the sm value and its corresponding i-percentile. The AMSR-E and ASCAT values outside of the range of CDF curves can also be properly rescaled, using the linear equation of the closest value.
Figure 13: Time series of soil moisture estimates from (a) Noah, (b) AMSR-E and (c) ASCAT for a grid cell (centred at 41.375° N, 5.375° W) in 2007. Circles represent days when Noah, AMSR-E and ASCAT all have valid estimates. (Figure taken from Liu et al. 2011)
Figure 14: Example illustrating how the cumulative distribution function (CDF) matching approach was implemented to rescale original AMSR-E and ASCAT against Noah soil moisture product in this study. (a, b, c) CDF curves of AMSR-E, Noah and ASCAT soil moisture estimates for the grid cell shown in Fig. 2. (d) Linear regression lines of AMSR-E against Noah for 12 segments. (e) Same as (d), but for ASCAT and Noah. (f) CDF curves of Noah (black), rescaled AMSR-E (blue) and rescaled ASCAT (red) soil moisture products. (Figure taken from Liu et al. 2011)
Intra-annual bias correction
From version v202212 on, the source and reference samples used in the scaling procedure are first divided into 366 subsets corresponding to the data points belonging to each day of the year. The scaling parameters are then calculated and applied separately to each subset, effectively providing a seasonality and thus accounting for non-stationary biases between the different sensors (or between a sensor and the reference model). These biases are generated by the different effect that the seasonally variable environmental conditions exert on the retrieval. One of such effects is for instance the vegetation state which impacts differently the scatterometric and radiometric datasets.
As the time series are subset into smaller samples, it can occur that the calculation of scaling parameters relies on too few observations, leading to overfitting. To avoid this, the usual threshold of a minimum of 20 points is used, below which the parameters are not calculated. In this case, the global time series parameters are used, allowing to prevent data loss.
Rescaling of Active Datasets
Different sensor specifications between ERS1/2 and ERS2 (e.g. spatial resolution) need to be compensated for using scaling. The CDF curves for ERS2 are calculated based on the overlap with ERS1/2. Rescaling ERS2 against ERS1/2 and then joining them generates the AMI-WS active data set, which is subsequently scaled to the Metop-A ASCAT data (ACTIVE product) or the GLDASv2.1 data (COMBINED product) (see Figure 12).
For the ACTIVE product, the limited overlap between AMI-WS ERS1/2 and Metop-A ASCAT in time (i.e., a few months) rules out the global adjustment method based on the information of their overlapping period. However, as retrievals from Metop-A ASCAT and AMI-WS capture similar seasonal cycles (Liu et al., 2011), we assume that their dynamic ranges are identical and, therefore, can use non-overlapping observations for the rescaling (i.e. the entire time period for each sensor).
It was noticed that the soil moisture (and backscatter) signal from Metop-B ASCAT is characterized by a positive bias on a global level. This has a detrimental effect particularly on the soil moisture trends from the ACTIVE product. To correct for this, Metop-B ASCAT is scaled to the reference of Metop-A ASCAT leading to a homogenization of the data record, as shown in Figure 15.
Figure 15: Comparison of global and hemispheric averages of soil moisture from ASCAT before (left) and after rescaling of Metop-B ASCAT on Metop-A ASCAT.
Rescaling of Passive Datasets
The seasonal cycle associated with the SSM/I dataset is deemed to be unreliable and therefore, for all CCI products, the SSM/I seasonal cycle is replaced with that from AMSR-E. The high frequency variations (anomalies) associated with SSM/I are scaled to those from AMSR-E prior to recombining the decomposed signal. An example of the SSM/I decomposition and rescaling is shown in Figure 16.
For the PASSIVE product, all datasets with the exception of SMAP are rescaled to AMSR-E. Where sufficient overlap is available, this is utilised; for all other cases (except AMSR2), the entire time period of AMSR-E and the sensor being scaled is utilised. For AMSR2, data in the last three years of AMSR-E and the first three years of ASMR2 are used, i.e. 2008-10-04 to 2015-07-01. SMAP is rescaled to AMSR2 which has already been rescaled to AMSR-E.
Figure 16: Example illustrating how (a) the TMI was rescaled against AMSR-E, (b-e) the SSM/I anomalies were rescaled against AMSRE-E anomalies, reconstructed and merged with rescaled TMI and AMSR-E, and (f) the SMMR was rescaled and merged with the others. The grid cell is centred at 13.875°N, 5.875°W (Image courtesy Liu et al., 2012).
Rescaling in the COMBINED product
For generating the combined product, all passive and active level 2 data sets are rescaled against GLDASv2.1, with the exception of ERS1/2, ASCAT and SSMI which are discussed above.
Error characterization
Errors in the individual active and passive products are characterized by means of triple collocation analysis. These errors are used both for estimating the merging parameters and for characterizing the errors of the merged product (see section 3.3.6).
Triple collocation analysis is a statistical tool that allows estimating the individual random error variances of three data sets without assuming any of them acting as supposedly accurate reference (Gruber et al. 2016a, 2016b). This method requires the errors of the three data sets to be uncorrelated, therefore triplets always comprise of (i) an active data set, (ii) a passive data set, and (iii) the GLDAS-Noah land surface model, which are commonly assumed to fulfil this requirement (Dorigo et al. 2010). Error variance estimates are obtained as:
where σε 2 denotes the error variance; σ2 and σ denote the variances and covariances of the data sets; and the superscripts denote the active (a), the passive (p), and the modelled (m) data sets, respectively. For a detailed derivation see Gruber et al. (2016b).
The error estimates detailed above represent the average random error variance of the entire considered operational time period of a sensor, which is commonly assumed to be stationary. The soil moisture uncertainties of the three products (ACTIVE, PASSIVE, and COMBINED) have been determined until v202212 through the above equations, which caused the uncertainty estimates provided with the product to apply to an entire merging period and not vary with every (observation) timestamp. However, a seasonal characterisation of the error is fundamental to understand the error structure in EO-based soil moisture estimates and its coupling with temporally dynamic scene characteristics (Zwieback et al., 2018) and can ultimately benefit in wide variety of studies where observation reliability is highly valued, spanning from model assimilation to seasonal yield forecasts. For this reason, a new approach is used since v202312, where TCA is performed using moving temporal subsets as also described in Chapter 3.3.3.4. Each subset comprise all the observations included in a 3-month window centred on each month of the year, therefore providing an error estimate that is representative of the relative month. The comparison between a static and seasonal approach is illustrated below (Figure 17).
Figure 17: Comparison between the static uncertainty (v202212 and before) and the seasonal uncertainty (monthly resolution, v202312 and following) characterization with TCA for ASCAT and AMSR2. On the background, VOD from VODCA C-Band (Moesinger et al., 2020) is shown.
As expected, the error structure and the relative performance between the two sensors is reflecting the seasonal vegetation patterns (Dorigo et al., 2010). The relative weights of the sensors change accordingly throughout the year, as given by Eq. 22-23.
Error gap-filling
TCA does not provide reliable error estimates in all regions, mainly if there is no significant correlation between all members of the triplet, which often happens for example in high-latitude areas or in desert areas. TCA error estimates are therefore disregarded where the Pearson correlation between any of the data sets is deemed insignificant (i.e., p-value < 0.05).
In these areas, error estimates are derived by deriving a Signal-to-Noise Ratio (SNR)-VOD regression model per land cover class and using this to determine the SNR based on the VOD at each location where SNR could not be retrieved:
Where the subscript denotes the spatial location; and the parameters ai are derived from a global polynomial regression between VOD and TCA based error estimates at locations where they are considered reliable (i.e., all data sets are significantly correlated). For TMI and WINDSAT, third order polynomials (N=3) are used and for all other sensors second order polynomials (N=2) are used, which was empirically found to provide the best regression results.
Merging
The merging procedure consists of (1) merging the original passive microwave product into the PASSIVE product, (2) merging the original active microwave products into the ACTIVE product, and (3) merging the original active and passive microwave products into the COMBINED product. The merging periods are shown in Figure 1 and listed in Table 4, Table 5, Table 6.
Note that in C3S SM only daytime retrievals are used for all operational passive sensors also included in the ICDR products (SMOS, SMAP, AMSR2, GPM).
Table 4: Passive sensors used in the PASSIVE product (sensors marked with * in the last merging period are used in the ICDR).
Time Period | Passive Sensors (mode: ascending (a) or descending (d)) |
|---|---|
01/11/1978 – 31/07/1987 | SMMR (a/d) |
01/09/1987 – 31/12/1997 | SSM/I (a/d) |
01/01/1998 – 18/06/2002 | SSM/I (a/d), TMI (a/d) |
19/07/2002 – 30/09/2007 | AMSR-E (a/d), TMI (a/d) |
01/10/2007 – 14/01/2010 | AMSR-E (a/d), WindSat (a/d), TMI (a/d) |
15/01/2010 – 31/55/2011 | AMSR-E (a/d), WindSat (a/d), SMOS (a/d), TMI (a/d) |
31/05/2011 – 04/10/2011 | AMSR-E (a/d), WindSat (a/d), SMOS (a/d), TMI (a/d), FY-3B (a/d) |
05/10/2011 – 30/06/2012 | WindSat (a/d), SMOS (a/d), TMI (a/d), FY-3B (a/d) |
01/07/2012 – 28/09/2013 | SMOS (a), AMSR2 (d), TMI (a/d), FY-3B (a/d) |
29/09/2013 – 28/02/2014 | SMOS (d), AMSR2 (d), TMI (a/d), FY-3B (a/d), FY-3C (a/d) |
01/03/2014-30 - 09-2014 | SMOS (a), AMSR2 (d), TMI (a/d), FY-3B (a/d), FY-3C (a/d), GPM (d) |
01/10/2014 – 30/03/2015 | SMOS (a), AMSR2 (d), FY-3B (a/d), FY-3C (a/d), GPM (d) |
31/03/2015 – 31/12/2018 | SMOS (a), AMSR2 (d), FY-3B (a/d), FY-3C (a/d), GPM (d), SMAP (d) |
01/01/2019 – 19/08/2019 | SMOS (a), AMSR2 (d), FY-3B (a/d), FY-3C (a/d), FY-3D (a/d), GPM (d), SMAP (d) |
20/08/2019 – 04/02/2020 | SMOS (a), AMSR2 (d), FY-3C (a/d), FY-3D (a/d), GPM (d), SMAP (d) |
04/02/2020 – Present | SMOS* (a), AMSR2* (d), FY-3D (a/d), GPM* (d), SMAP* (d) |
Table 5: Active sensors used in the ACTIVE product (sensors marked with * in the last merging period are used in the ICDR).
Time Periods | Active Sensors |
|---|---|
05/08/1991 – 19/05/1997 | ERS1/2 (AMI-WS) |
20/05/1997 – 17/02/2003 | ERS2 (AMI-WS) |
18/02/2003 – 31/12/2006 | ERS1/2 (AMI-WS) |
01/01/2007 – 20/07/2015 | Metop-A ASCAT |
20/07/2015 – 07/11/2018 | Metop-A ASCAT, Metop-B ASCAT |
08/11/2018 – 15/11/2021 | Metop-A ASCAT, Metop-B ASCAT, Metop-C ASCAT |
16/11/2021 – Present | Metop-B ASCAT*, Metop-C ASCAT* |
Table 6: Sensors used in the COMBINED product (sensors marked with * in the last merging period are used in the ICDR).
Time Periods | Active Sensors | Passive Sensors (mode: ascending (a) or descending (d)) |
|---|---|---|
01/11/1978 – 31/07/1987 | N/A | SMMR (a/d) |
01/09/1987 – 05/08/1991 | N/A | SSM/I (a/d) |
05/08/1991 – 31/12/1997 | AMI-WS | SSM/I (a/d) |
01/01/1998 – 18/06/2002 | AMI-WS | SSM/I (a/d). TMI (a/d |
19/07/2002 – 31/12/2006 | AMI-WS | AMSR-E (a/d), TMI (a/d) |
01/01/2007 – 30/09/2007 | Metop-A ASCAT | AMSR-E (a/d), TMI (a/d) |
01/10/2007 – 14/01/2010 | Metop-A ASCAT | AMSR-E (a/d), WindSat (a/d) , TMI (a/d) |
15/01/2010 – 31/55/2011 | Metop-A ASCAT | AMSR-E (a/d), WindSat (a/d), SMOS (a), TMI (a/d) |
31/05/2011 – 04/10/2011 | Metop-A ASCAT | AMSR-E (a/d), WindSat (a/d), SMOS (a), TMI (a/d). FY-3B (a/d) |
05/10/2011 – 30/06/2012 | Metop-A ASCAT | WindSat (a/d), SMOS (a), TMI (a/d), FY-3B (a/d) |
01/07/2012 – 28/09/2013 | Metop-A ASCAT | SMOS (a), AMSR2 (d), TMI (a/d), FY-3B (a/d) |
29/09/2013 – 28/02/2014 | Metop-A ASCAT | SMOS (a), AMSR2 (d), TMI (a/d), FY-3B (a/d), FY-3C (a/d) |
01/03/2014-30 - 09-2014 | Metop-A ASCAT | SMOS (a), AMSR2 (d), TMI (a/d), FY-3B (a/d), FY-3C (a/d), GPM (d) |
01/10/2014 – 20/07/2015 | Metop-A ASCAT | SMOS (a), AMSR2 (d), FY-3B (a/d), FY-3C (a/d), GPM (d) |
20/07/2015– 08/11/2018 | Metop-A ASCAT, Metop-B ASCAT | SMOS (a), AMSR2 (d), FY-3B (a/d), FY-3C (a/d), GPM (d) |
09/11/2018 – 31/12/2018 | Metop-A ASCAT, Metop-B ASCAT, Metop-C ASCAT | SMOS (a), AMSR2 (d), FY-3B (a/d), FY-3C (a/d), GPM (d), SMAP (d) |
01/01/2019 – 19/08/2019 | Metop-A ASCAT, Metop-B ASCAT, Metop-C ASCAT | SMOS (a), AMSR2 (d), FY-3B (a/d), FY-3C (a/d), FY-3D (a/d), GPM (d), SMAP (d) |
20/08/2019 – 04/02/2020 | Metop-A ASCAT, Metop-B ASCAT, Metop-C ASCAT | SMOS (a), AMSR2 (d), FY-3C (a/d), FY-3D (a/d), GPM (d), SMAP (d) |
04/02/2020 – 15/07/2021 | Metop-A ASCAT, Metop-B ASCAT, Metop-C ASCAT | SMOS (a), AMSR2 (d), FY-3D (a/d), GPM (d), SMAP (d) |
16/11/2021– Present | Metop-B ASCAT*, Metop-C ASCAT* | SMOS* (a), AMSR2* (d), FY-3D (a/d), GPM* (d), SMAP* (d) |
Weight estimation
The merging is performed by means of a weighted average which takes into account the error properties of the individual data sets that are being merged:
Where Θm denotes the merged soil moisture product; Θi are the soil moisture products that are being merged, and wi are the merging weights.
Per definition, the optimal weights for a weighted average are determined by the error variances of the input data sets and write as follows:
where j denote the index of the respective data sets; i is the data set for which the weight is being calculated; and N is the total number of data sets which are being averaged. The required error variances are calculated using Eq. 20. Notice that error covariance terms are neglected as they cannot be estimated reliably.
It should be mentioned that the above definition of the weights based on error variances assumes all data sets to be in the same data space. However, data sets usually vary in their signal variability due to algorithmic differences, varying signal frequencies, etc. Therefore, conceptually, it is more appropriate to define relative weights in terms of the data sets SNR properties rather than of their error variance (Gruber et al., 2017). Nevertheless, the actual merging requires a harmonization of the data sets into a common data space, which in the case of the CCI SM data set is done using the CDF matching approach described in Section 3.3.3.4 . Therefore, the calculation of the weights using Eq. 23 suffices, keeping in mind that they represent the rescaled error variances of rescaled data sets.
Notice that soil moisture estimates of the various sensors are not available every day, hence there are certain dates during the overlapping periods on which not all data sets provide a valid estimate to calculate the weighted average. In such cases, the weights are re-distributed amongst the remaining data sets, again based on their relative SNR properties.
However, this re-distribution of weights could significantly worsen data quality on these days because of the increasing contribution of measurements which initially would have had a low weight due to their (relatively) low SNR. Therefore, soil moisture estimates in the merged product on days where not all data sets provide valid estimates are set to NaN values (Not a Number), if the sum of the initial weight of the remaining data sets is lower than 1/(2N) where N is the total number of data sets that are potentially available for the corresponding merging period. This threshold has been derived empirically to provide a good trade-off between temporal measurement density and average data quality.
Similar to the generation of the PASSIVE product, relative weights at each time step are derived from the TCA- or VOD-regression based error estimates for each individual sensor. Depending on how many sensors are available within a particular period, a (1/2N) threshold for the minimum weight of a particular sensor was applied if not all sensors provide a soil moisture estimate at that day.
Break detection and correction
In C3S v202312, break detection and correction methods are introduced to the COMBINED product. These methods use reanalysis soil moisture as a reference to detect inhomogeneities in the merged satellite records.
Breaks may occur as a result of merging different sensor combinations over time, as shown in Figure 18. Such breakpoints may therefore appear between periods with different input sensors. Structural inhomogeneities may affect statistics such as trends and changes in extreme values (percentiles) and therefore should not only be detected but also corrected.
Figure 18: Potential break times in the ESA CCI SM v04.4 (COMBINED) product corresponding to changeovers in the blended sensors, building the homogeneous (sensor) sub-periods (HSP).
Based on the work of Su et al. (2016), a procedure has been developed at TU Wien to test for potential inhomogeneities in the ESA CCI SM CDR using the Fligner-Killeen test for homogeneity of variances and Wilcoxon rank-sums test for shifts in population mean ranks (Preimesberger et al., 2021). For the product provided in v202312, ERA5 is used as the reference dataset.
To adjust detected breaks in the data set, Quantile Category Matching (QCM) is used. This method uses split-fitted differences in empirical CDFs of the candidate and reference SM values (between quantile categories, i.e. average SM within a number of quantile ranges) before and after a break. The values after the break are used to find corrections for quantiles of satellite measurements before the break.
Adjustment is performed iteratively, with the goal that across each detected break, changes in C3S SM means and variances are matched to follow changes within the reference data set (relative bias correction) and homogenized observation series (with respect to the reference data set) are derived.
The results of the correction performed on v04.4 of the ESA CCI SM dataset are shown in Figure 19. Figure 20 shows the longest homogenous period, i.e. the maximum period over which no break was detected, of available data both before (top) and after (bottom) correction using the QCM method.
Figure 19: Results of the inhomogeneity testing (between HSP3 and HSP4) before any correction methods have been applied (top) with the results of the testing after the QCM correction method is applied (bottom). Adapted from Preimesberger et al. (2021)
Figure 20: Longest homogenous period in ESA CCI SM v04.4 (COMBINED) before adjustment (top) and after adjustment (bottom) using the QCM method. Dark green indicates areas which are permanently masked in C3S SSM due to dense vegetation. Taken from Preimesberger et al. (2021).
Freeze/Thaw classification algorithm
The majority of land in the Northern Hemisphere is affected by seasonal freeze/thaw processes (Zhang et al., 2003). The dielectric properties of water change significantly under frozen conditions, as the dielectric constant decreases sharply (Jin et al., 2015), resulting in a received microwave signal similar to that of dry (unfrozen) soils. This leads to a "false" reduction in retrieved soil moisture, where the retrieval algorithm incorrectly indicates dry conditions, meaning that currently no soil moisture retrieval is possible under snow and ice cover (Dorigo et al., 2017; Ulaby et al., 1982). To address this ambiguity, it is essential to have information on the freeze/thaw state of the soil to flag and mask the affected measurements. This is currently done for both active and passive retrieval models used in C3S SM, and unreliable data points from measurements taken under frozen soil conditions are therefore excluded from all C3S SM products. This information is also provided to users of satellite soil moisture data to transparently communicate the reason for data gaps.
Until now, this information has only been provided as binary-encoded values in the “flag” variable of the merged satellite soil moisture products. However, data on the surface state and temporal dynamics of freeze/thaw events themselves are crucial for a wide range of applications, including research on climate change, hydrology, ecology, and agriculture (Jin et al., 2015). Changes in the timing, duration, and extent of frozen ground, particularly in response to climate warming, have profound impacts on plant growth, infrastructure stability, and the exchange of greenhouse gases between the land surface and the atmosphere (Jin et al., 2015).
As of version v202505, C3S SM therefore provides a separate, daily global Freeze/Thaw record, which integrates land surface temperature and surface state data from all available satellites into a single consistent record.
Methodology
Flagging of frozen soil observations in active measurements is based on surface state information provided by EUMETSAT H SAF. A data point is classified as ‘frozen’ when the surface state flag indicator (SSF) is not equal to 1 (unfrozen), which includes temporarily frozen soils, permanent ice, and melting water on the surface. As the retrieval of active sensor data falls outside the scope of the C3S SM merging framework, we refer the reader to Naeimi et al. (2012) and H SAF (2018c) for further details.
Here, we focus on the methodology applied to classify frozen soils in passive (radiometer) retrievals via the LPRM model, developed as part of the CCI and C3S SM programs. Ku-, K-, and Ka-band brightness temperature data are consistently available over the entire C3S SM data record period from various sensors (compare Figure 1). To utilize this, van der Vliet et al. (2020) developed a decision tree based on data from these frequency bands. Prior to this, all pixels where the surface temperature was observed to be at or below 274.15 °K were assigned a frozen data flag, determined using the method described by Holmes et al. (2009). However, as this approach was insufficiently accurate in detecting the transition to snow-covered and frozen conditions, the methodology introduced by Van der Vliet et al. (2020) was adopted. This method employs three frequencies (Ku-, K-, and Ka-band) to reliably flag these conditions, using a decision tree based on vertical brightness temperatures (Tb) at 18.7 GHz, 23.8 GHz, and 36.5 GHz.
This algorithm is applied to all passive sensors, except for the L-band sensors (SMAP and SMOS), which do not carry instruments capable of measuring K-band brightness temperatures (van der Schalie et al., 2021). The resulting classification data are used to flag retrievals in the C3S SM products.
The classification data from both active and passive sensors are subsequently used to derive the Freeze/Thaw product. Consistent with the current cross-flagging approach implemented in the C3S SM merging framework for soil moisture (Section 3.3.3.3), a data point is classified as frozen if the frozen soil classification from at least one available sensor on a given day is positive. However, it is well known that classification results can vary between different sensors and their respective overpasses (e.g., during daytime and nighttime). Such differences may arise due to diurnal freeze/thaw dynamics, particularly in transitional zones and periods where soil moisture conditions shift between frozen and unfrozen states. The current binary classification is therefore considered conservative in identifying soils as “frozen.” To provide additional information on the level of agreement between sensors, the product includes the total number of available sensors, the number of sensors detecting frozen soils, and an agreement index (equal to 1 if all sensors yield the same classification result), alongside the binary freeze/thaw classification.
Based on the evaluations performed by van der Vliet et al. (2020), who compared their classification results to in situ measurements from the SNOTEL (Leavesley et al., 2008; Schaefer et al., 2001) and SCAN Network (Schaefer et al., 2007)4, a median classification accuracy of ~78 % with respect to available in situ data is expected, which is in line with the classification accuracy for (meta)data provided with SMAP Soil moisture and above the accuracy of SMOS classifications (van der Vliet et al., 2020). The evaluation also considered the spatial patterns of accuracy, and it was found that no south-to-north degradation pattern in accuracy was present for the K-band flags.
4 For more information on SNOTEL and SCAN networks, see: https://www.nrcs.usda.gov/programs-initiatives/sswsf-snow-survey-and-water-supply-forecasting-program/national-water-and (URL last accessed 25/03/2025)
Root Zone Soil Moisture algorithm
Satellite surface soil moisture products ameliorate the sparseness of field measurements but are inherently limited to observing the near-surface layer, while water available in the unobserved root zone controls critical processes like evapotranspiration and plant water uptake. For this purpose, a long-term global root zone soil moisture (RZSM) dataset is developed from the C3S SSM COMBINED product , based on the infiltration formulation (Pasik et al., 2023), recently published as a science product within the ESA CCI+ Phase 1 New R&D on CCI Essential Climate Variables (ECVs) Soil Moisture CCN3 project (Stradiotti et al., 2024).
The RZSM product uses the latest C3S SSM COMBINED surface product as input and applies an infiltration model, calibrated for three depth layers (0-10 cm, 10-40 cm, 40-100 cm), to the surface data globally. Note that Pasik et al. (2023) have calibrated an additional layer (100-200 cm). However, as the validation found a poor agreement between predictions and both in situ and model reference data, we omit the fourth layer in the C3S RZSM product.
Methodology
The model approximates the soil moisture content up to 2 meters in depth by smoothing and delaying surface observations via a one-parameter (T) exponential filter (EF) method. EF is a two-layer water-balance model relying on the assumption that the fluxes between the remotely sensed surface layer and the root zone reservoir below are proportional to the difference in SM content between both layers, while the infiltration rate is assumed to be constant (Pasik et al., 2023). The recursive formulation of the method is given in Eq. 24.
RZSM estimates are therefore based on a weighted average of the new Surface Soil Moisture (SSM) input and past EF outputs (RZSM(tn-1)), with more recent calculations receiving higher weights on a time-scale dictated by the method’s only parameter - T (temporal length, typically in days). The weights are controlled by the term gain (Kn) ranging between 0 and 1 and calculated as in Eq. 25.
Timestamps (in days) of the newest and last available SSM observations, are represented by tn and tn-1 respectively. Parameter T controls the level of smoothing and delaying of the SSM to the RZSM. T ranges from 0 to 100, with higher values reducing the influence of SSM on RZSM. Each soil depth is assigned a distinct T value. The calibration process for the T parameter is detailed in the next chapter.
At model initialization and in presence of persistent data gaps - when no preceding estimates are available, the calculation is started with Kn set to 1 and equating model output to its first input. Thus, we allow a one-year adjustment period for Kn to reach equilibrium.
T-parameter calibration
The parameter T controls the smoothing and delay of SSM in relation to RZSM. It ranges from 0 to 100, with higher values reducing the influence of SSM on RZSM. Since temporal soil moisture dynamics decrease with depth, T tends to increase accordingly (Paulik, et al., 2014; Wang, et al., 2017). The limited sensitivity of the EF to variations in T due to environmental factors (Albergel, et al., 2008; Brocca, et al., 2011; Grillakis et al., 2021) warrants using a single value of T to represent a particular soil depth in global applications (Pasik et al., 2023). As a result, Pasik et al., (2023) have defined T for four depth layers: 0–10 cm, 10–40 cm, 40–100 cm, and 100–200 cm. However, as Pasik et al. (2023) noted a poor performance of their data in the 100-200 cm layer, this one is excluded from the C3S RZSM datasets. The chosen layers are in line with other RZSM datasets (Rodell, et al., 2004; Muñoz Sabater, et al., 2021) and facilitating potential data assimilation.
To calibrate the infiltration parameter T, Pasik et al. (2023) used in situ data from the ISMN (Dorigo et al., 2021). ISMN data from the 2001-2020 period was used, where the mean sensor measuring depth did not exceed 2 meters. All measurements were resampled to mean daily values to match the temporal resolution of the satellite-based products. Furthermore, ISMN time series flagged as "good" (Dorigo, et al., 2013) and having at least 100 matching observations with the CCI SSM product were considered.
Pasik et al. (2023) compared the results of 100 different T-value realisations of the infiltration model applied to satellite soil moisture time series with the available in situ root zone SM time series and found that the optimal T-value (Topt in terms of maximising correlation with the in situ data) increases with infiltration depth as shown in Figure 21. Based on 3901 available ISMN time series representing 67 unique measuring depths, median Topt values of 6, 15, and 48 days were obtained to represent RZSM product layers 1-3, respectively.
In addition to the three described depth layers, C3S SM also provides a single RZSM estimate for the 0-1 m layer. Therefore, a weighted average of the three layers (relative weights correspond to layer width) is computed for each grid cell where data is available for all layers.
Figure 21: Topt values calibrated with 3901 in situ time series and binned according to RZSM layers 1–4. Median values (represented by orange lines) from each bin were used to compute a global RZSM product.
Median absolute deviations (MAD(Topt)) were used to estimate RZSM uncertainties. Note that layer 4 is not used in C3S RZSM due to the low expected performance (Pasik et al., 2023). Figure taken from Pasik et al. (2023).
Uncertainty estimation
The C3S satellite RZSM product comes with temporally dynamic uncertainty estimates computed by means of an error propagation scheme (De Santis & Biondi, 2018) adapted to the EF from a Gaussian random error propagation approach (Taylor, 1997; Pasik et al., 2023). In this method the uncertainty of the RZSM estimates σ(RZSMn) is affected by (i) uncertainties in the SSM input data (Δ), (ii) the Jacobian term (∂ RZSMn )⁄( ∂ T), representing the sensitivity of RZSM to parameter T, (iii) noise in the T parameter σ(T) and (iv) structural uncertainty of the EF model σ(EF).
Uncertainties of the input satellite SSM data are considered by the term Δ, which also takes into account the effect of prolonged input data gaps. The Jacobian term helps quantify how much recent changes in SSM influence the deeper RZSM, while also reflecting the impact of missing data. Higher Jacobian values occur when there are significant changes in SSM, such as during rapid wetting (e.g., rainfall) or drying (e.g., drought). Lower values mean that RZSM is less affected by short-term fluctuations in SSM. If there are gaps in the input SSM data, the uncertainty naturally increases, as the model has less information to rely on.
The T parameter noise threshold (σ(T)) is calculated with the median absolute deviation, MAD(Topt ). It is found to be 4, 10, and 32 for the RZSM depth layers 1–3, respectively (see Figure 21).
The EF model structural error σ(EF) is estimated for each RZSM layer. In order to exclude the representativeness error from the analysis, σ(EF) is calculated based on in situ rather than remotely sensed data. In situ data is selected for stations that operate sensors both at the surface and in the root zone. At these stations, the RZSM estimates are derived from the in situ SSM measurements using the EF method and then compare them to the actual in situ RZSM station measurements. For this analysis, the T value was optimized for each station and depth individually to minimize its influence on the estimation of σ(EF). The σ(EF) was then estimated for each location by taking the unbiased root-mean-square difference (ubRMSD) of two in situ time series. Note that “unbiased”, in this case, refers not only to a correction for bias in the mean but also to a correction for bias in variance, which also constitutes an unintended systematic component in the RMSE (Gupta et al., 2009). Time series with negative correlation between EF-based RZSM estimates and in situ RZSM measurements were disregarded. This resulted in σ(EF) or soil layers 1-4 shown in Figure 22.
Figure 22:The ubRMSD between propagated RZSM from in situ SSM using the EF model and measurements of RZSM at the same location and the same depth, calculated with 4239 different time series.
The median ubRMSD value for each bin (represented by orange lines and annotated) represent σ(EF) for the respective Topt. Note that layer 4 is not used in C3S SM due to the low expected performance (Pasik et al., 2023). Figure taken from Pasik et al. (2023).
Note that in situ measurement errors were assumed to be negligible and thus did not influence ubRMSD estimates, which likely causes model structural uncertainties to be overestimated. Also, structural uncertainties are assumed to be constant in time. An increase in σ(EF) corresponds to the growing distance between the surface and the root zone measurements, demonstrating the decreasing coupling strength between both layers. Note that σ(EF) shows significant variability within RZSM layers, which is likely, at least to some degree, related to variations in local conditions. However, as with the T-parameter optimization, we estimate structural uncertainties based only on a limited number of in situ stations and therefore use the median to extrapolate globally.
The discussed individual components that contribute to the uncertainty estimates for RZSM layer 1-3 are then applied for each satellite grid cells as shown in Eq. 26.
Near real time (NRT) mode of the processor
The processing steps described in the previous sections work on the complete time series of the datasets. This is not feasible during NRT production of the products. Figure 23 gives an overview of the NRT processing chain. The parameters for CDF scaling and the characterised errors are precomputed during generation of the CDR and then used directly in the ICDR processing. The same applies to the infiltration model parametes for RZSM. This speeds up the processing and results in a consistent time series based on stable merging parameters. At the moment it is only possible to use night-time retrievals from passive sensors in the ICDR generation.
Figure 23: Overview of NRT processing chain. Scatterometer-derived soil moisture is provided directly by EUMETSAT H SAF (central blue parallelograms), while soil moisture from raw radiometer measurements is derived within C3S using the LPRM algorithm (central red parallelograms). All input products are spatially resampled to the C3S SM data grid before Freeze/Thaw classification (purple parallelogram) and the generation of SSM ICDRs (ACTIVE, PASSIVE, COMBINED; blue, red, green parallelograms). For SSM, pre-computed scaling and merging parameters are applied to harmonize and combine data from individual sensors. RZSM ICDRs (orange parallelogram) use the COMBINED SSM data as input and incorporate stored infiltration information from previous ICDRs to produce consistent records over time.
Changelog
Table 7 provides an overview of the differences between different versions of the product up-to, and including, the current version v202505. For a full list of all records provided in this version, see Table "List of datasets covered by this document".
Table 7: Changes in the product between versions.
Version | Product Changes |
|---|---|
v202505 | CDF matching scaling now uses a dynamic window size. First version of the Freeze/Thaw and RZSM product included. |
v202312 | Artificial breaks in the COMBINED product are now removed using the Quantile Category Matching method described in Preimesberger et al. (2021). |
v202212 | The PASSIVE and COMBINED product now include SM data from FengYun 3B/C/D and GPM, which are derived using v7 of the Land Parameter Retrieval Model (LPRM). TMI is extended to 2015, and scatterometer derived SM from ASCAT-C using the Water Retrieval Package (WARP) is included for the first time. This version also includes day-time observations for all passive data, a new approach to estimate intra-annual changes in error estimates for single sensors, updated flagging of frozen soils in active and passive data, cross flagging of frozen soils between active and passive data, and the first optional flag (i.e. soil moisture values are provided when this flag is active; users can decide whether to use them or not) in the product: for grid cells dynamically classified as "bare ground". |
v202012 | The PASSIVE and COMBINED product now include SM data from SMAP brightness temperature measurements derived through the LPRM v6 retrieval model. Intercalibration of AMSRE and AMSR2 observations, that lead to a negative break in PASSIVE SM in the past has been corrected. The CDF matching method has been updated. LPRM v6 is now used to derive SM for all decommissioned passive sensor products. |
v201912 | Product algorithm same as v201812. Product extended to 2019-12-31. |
v201812 | Product algorithm updated and now based on ESA CCI SM v4.4 rather than v4.3 applied to version v201806. Product extended to 2018-12-31. |
v201806 | The combined product is now generated by merging all active and passive L2 products directly, rather than merging the generated active and passive products. Spatial gaps in TC-based SNR estimates now filled using a polynomial SNR_VOD regression. sm_uncertainties now available globally for all sensors except SMMR. A p-value based mask used to exclude unreliable input data sets in the combined product has been modified and it is also applied to the passive product. Masking of unreliable retrievals is undertaken prior to merging. |
v201801 | Updated CDR includes SMOS data from the end of 2016 onwards. SMOS is also included in the ICDRs produced from January 2018 onwards. CDR produced until 2017-12-31; ICDR produced from 2018-01-01. |
v201706 | First release of the dataset. CDR produced until 2017-06-30; ICDR produced from 2017-07-01. |
Output data
Table 8, Table 9, and Table 10 list the output fields generated by the processing system and available to data users of the SSM, RZSM, and F/T products, respectively. Detailed information about each field and the file format are provided in the related Product User Guide and Specification (PUGS) document.
Table 8 : Overview of output data fields in the SSM products (ACTIVE, PASSIVE, COMBINED). More information is given in the netCDF attributes of each data file.
Plots show COMBINED data at 2023-07-01 opened in the free Panoply netcdf data viewer.
Field name | Description | Visualised in Panoply |
|---|---|---|
sm |
| |
sm_uncertainty |
| |
flag |
| |
freqbandID |
| |
mode |
| |
sensor |
| |
dnflag |
| |
t0 |
|
Table 9 : Overview of output data fields in the RZSM product. Plots show data at 2023-07-01 as opened in the free Panoply netcdf viewer.
Field name | Description | Visualised in Panoply |
|---|---|---|
rzsm_1 |
| |
rzsm_2 |
| |
| rzsm_3 |
| |
| rzsm_1m |
| |
| uncertainy_1 |
| |
| uncertainy_2 |
| |
| uncertainy_3 |
|
Table 10 : Overview of output data fields in the Freeze/Thaw product. Plots show data at 2023-03-01 as opened in the free Panoply netcdf viewer.
Field name | Description | Visualised in Panoply |
|---|---|---|
ft |
| |
| ft_agreement |
| |
| sensor_count |
| |
| sensor_count_frozen |
| |
| dnflag |
| |
| mode |
| |
| sensor |
|
References
Albergel, C., Rüdiger, C., Pellarin, T., Calvet, J.-C., Fritz, N., Froissard, F., Suquia, D., Petitpa, A., Piguet, B., and Martin, E. (2008): From near-surface to root-zone soil moisture using an exponential filter: an assessment of the method based on in-situ observations and model simulations, Hydrol. Earth Syst. Sci., 12, 1323–1337, https://doi.org/10.5194/hess-12-1323-2008 (URL resource last accessed 25/03/2025).
Ashcroft, P. and Wentz, F. (2000). Algorithm Theoretical Basis Document: AMSR Level-2A Algorithm, Revised 03 November. Santa Rosa, California USA: Remote Sensing Systems. https://eospso.gsfc.nasa.gov/sites/default/files/atbd/atbd-amsr-level2A.pdf (URL resource last accessed 25/03/2025)
Attema, E., & Ulaby, F. (1978). Vegetation modeled as water cloud. Radio Science, 13, 357-364
Balsamo, G., Albergel, C., Beljaars, A., Boussetta, S., Brun, E., Cloke, H., Dee, D., Dutra, E., Muñoz-Sabater, J., Pappenberger, F., de Rosnay, P., Stockdale, T., and Vitart, F. (2015), “ERA-Interim/Land: a global land surface reanalysis dataset”, Hydrol. Earth Syst. Sci., vol. 19, pp. 389-407, doi: 10.5194/hess-19-389-2015.
Balsamo, G., S. Boussetta, P. Lopez, L. Ferranti (2010), Evaluation of ERA-Interim and ERA-Interim-GPCP-rescaled precipitation over the U.S.A., ERA Report Series, n. 5, pp10.
Bartalis, Z., Wagner, W., Naeimi, V., Hasenauer, S., Scipal, K., Bonekamp, H., Figa, J., & Anderson, C. (2007). Initial soil moisture retrievals from the METOP-A Advanced Scatterometer (ASCAT). Geophy. Res. Lett, 34, L20401
Beaudoing, H. and Rodell M., NASA/GSFC/HSL (2016), GLDAS Noah Land Surface Model L4 3 hourly 0.25 x 0.25 degree V2.1, Greenbelt, Maryland, USA, Goddard Earth Sciences Data and Information Services Center (GES DISC), 10.5067/E7TYRXPJKWOQ
Bennartz, R., and Michelson, D.B. (2012), Validation of AMSR-E and AMSU/HSB level 1 brightness temperatures and level 2 cloud and precipitation parameters, NAG5--12579, Meteorological and Hydrological Institute, Report, March 2004 https://pubs.ssec.wisc.edu/research_Resources/publications/pdfs/METPUBS/MET_Publication_No_04_03_B1.pdf (URL resource last accessed 25/03/2025)
Bevington, P.R., & Robinson, D.K. (2002). Data reduction and error analysis for the physical sciences. (3th ed.). Boston: McGraw-Hill Science/Engineering/Math
Bevis, M., Businger, S., Herring, T., Rocken, C., Anthes, R., & Ware, R. (1992). GPS Meteorology: Remote Sensing of Atmospheric Water Vapor Using the Global Positioning System. Journal of Geophysical Research, 97, null-15801
Brocca, L., Hasenauer, S., Lacava, T., Melone, F., Moramarco, T., Wagner, W., Dorigo, W., Matgen, P., Martínez-Fernández, J., Llorens, P., Latron, J., Martin, C., & Bittelli, M., 2011. Soil moisture estimation through ASCAT and AMSR-E sensors: An intercomparison and validation study across Europe. Remote Sensing of Environment, 115(12), pp. 3390-3408. https://doi.org/10.1016/j.rse.2011.08.003. Available at: https://www.sciencedirect.com/science/article/pii/S0034425711002756 (URL resources last accessed 25/03/2025)
CATDS SMOS L3 soil moisture retrieval processor Algorithm Theoretical Baseline Document (ATBD) (2013), https://labo.obs-mip.fr/wp-content-labo/uploads/sites/18/2013/08/ATBD_L3_rev2_draft.pdf (URL resource last accessed 25/03/2025)
CATDS LEVEL 3 DATA PRODUCT DESCRIPTION Soil Moisture and Brightness Temperature (2014), https://www.cen.uni-hamburg.de/en/icdc/data/land/docs-land/so-tn-cb-ca-0001-3a.pdf (URL resource last accessed 25/03/2025)
Chan, S., Dunbar, R. S. (2020), Soil Moisture Active Passive (SMAP) Mission Level 3 Passive Soil Moisture Product Specification Document Version 7.0. online: https://nsidc.org/sites/default/files/psd_spl3smp_v7.pdf (URL resource last accessed 25/03/2025)
Crapolicchio, R., A. Bigazzi, G. De Chiara, X. Neyt, A. Stoffelen, M. Belmonte, W. Wagner, C. Reimer (2016) The scatterometer instrument competence centre (SCIRoCCo): Project's activities and first achievements, Proceedings European Space Agency Living Planet Symposium 2016, 9-13 May 2016, Prague, Czech Republic, 9-13.
Crow, W.T., Wagner, W., & Naeimi, V. (2010). The impact of radar incidence angle on soil moisture retrieval skill. IEEE Geoscience and Remote Sensing Letters, 7, 501-505
Dee, D.P. et al., 2011. The ERA-Interim reanalysis: configuration and performance of the data assimilation system. Quarterly Journal of the Royal Meteorological Society, 137(656), pp.553–597
De Jeu R.A.M, T.R.H. Holmes, R. M. Parinussa, M Owe (2014), A spatially coherent global soil moisture product with improved temporal resolution, Journal of Hydrology 516, 284-296.
De Nijs, A.H., Parinussa, R.M., De Jeu, R.A.M., Schellekens, J. and Holmes, T.R. (2015), “A methodology to determine radio-frequency interference in AMSR2 observations”, IEEE Transactions on Geoscience and Remote Sensing, vol. 53, no. 9, pp. 5148-5159.
De Santis, D., & Biondi, D. (2018). Error propagation from remotely sensed surface soil moisture into soil water index using an exponential filter. In G. L. Loggia, G. Freni, V. Puleo, & M. D. Marchis (Ed.), HIC 2018: 13th International Conference on Hydroinformatics. 3, pp. 520–525. EasyChair. doi:https://doi.org/10.29007/kvhb (URL resource last accessed 25/03/2025)
Dobson, M.C., Ulaby, F.T., Hallikainen, M.T., & Elrayes, M.A. (1985). Microwave dielectric behavior of wet soil. Part II: Dielectric mixing models. IEEE Transactions on Geoscience and Remote Sensing, 23, 35-46
Dorigo, W.A., et al. (2011) "The International Soil Moisture Network: A data hosting facility for global in situ soil moisture measurements", Hydrology and Earth System Sciences 15 (5), pp. 1675-1698
Dorigo, W.A., Xaver, A., Vreugdenhil, M., Gruber, A., Hegyiová, A., Sanchis-Dufau, A.D., Zamojski, D., Cordes, C., Wagner, W. and Drusch, M. (2013), Global Automated Quality Control of In Situ Soil Moisture Data from the International Soil Moisture Network. Vadose Zone Journal, 12: 1-21 vzj2012.0097. https://doi.org/10.2136/vzj2012.0097 (URL resource last accessed 25/03/2025)
Dorigo, W.A., Scipal, K., Parinussa, R.M., Liu, Y.Y., Wagner, W., De Jeu, R.A.M., and Naeimi, V. (2010), “Error characterisation of global active and passive microwave soil moisture datasets”, Hydrology and Earth System Sciences, vol. 14, pp. 2605 – 2616, doi: 10.5194/hess-14-2605-2010.
Dorigo, W., Wagner, W., Albergel, C., Albrecht, F., Balsamo, G., Brocca, L., Chung, D., Ertl, M., Forkel, M., Gruber, A., et al. (2017), “ESA CCI Soil Moisture for improved Earth system understanding: state-of-the art and future directions”, Remote Sensing of Environment, https://doi.org/10.1016/j.rse.2017.07.001 (URL resource last accessed 25/03/2025)
Dorigo, W., Himmelbauer, I., Aberer, D., Schremmer, L., Petrakovic, I., Zappa, L., Preimesberger, W., Xaver, A., Annor, F., Ardö, J., Baldocchi, D., Bitelli, M., Blöschl, G., Bogena, H., Brocca, L., Calvet, J.-C., Camarero, J. J., Capello, G., Choi, M., Cosh, M. C., van de Giesen, N., Hajdu, I., Ikonen, J., Jensen, K. H., Kanniah, K. D., de Kat, I., Kirchengast, G., Kumar Rai, P., Kyrouac, J., Larson, K., Liu, S., Loew, A., Moghaddam, M., Martínez Fernández, J., Mattar Bader, C., Morbidelli, R., Musial, J. P., Osenga, E., Palecki, M. A., Pellarin, T., Petropoulos, G. P., Pfeil, I., Powers, J., Robock, A., Rüdiger, C., Rummel, U., Strobel, M., Su, Z., Sullivan, R., Tagesson, T., Varlagin, A., Vreugdenhil, M., Walker, J., Wen, J., Wenger, F., Wigneron, J. P., Woods, M., Yang, K., Zeng, Y., Zhang, X., Zreda, M., Dietrich, S., Gruber, A., van Oevelen, P., Wagner, W., Scipal, K., Drusch, M., and Sabia, R. (2021): The International Soil Moisture Network: serving Earth system science for over a decade, Hydrol. Earth Syst. Sci., 25, 5749–5804, https://doi.org/10.5194/hess-25-5749-2021 (URL resource last accessed 25/03/2025)
Dorigo, W., Stradiotti, P., Preimesberger, W., Kidd, R., van der Schalie, R., Frederikse, T., Rodriguez-Fernandez, N., & Baghdadi, N. (2024). ESA Climate Change Initiative Plus - Soil Moisture Algorithm Theoretical Baseline Document (ATBD) Supporting Product Version 09.0. Zenodo. https://doi.org/10.5281/zenodo.13860922 (URL resource last accessed 25/03/2025)
Drusch, M., Wood, E., & Gao, H. (2005). Observation operators for the direct assimilation of TRMM microwave imager retrieved soil moisture. Geophysical Research Letters, 32, L15403
Entekhabi, D., Das, N., Njoku, E.G.,Yueh, S., Johnson, J., Shi, J.(2014) Algorithm Theoretical Basis Document L2 & L3 Radar/Radiometer Soil Moisture, L2 & L3 Radar/Radiometer Soil Moisture,
ESA (2017) ERS-2 SCATTEROMETER Surface Soil Moisture Time Series in High Resolution - ERS.SSM.H.TS (25 km Time-Series product), SCI-MAN-16-0047-v02 https://earth.esa.int/eogateway/documents/20142/37627/scirocco-pum-ts.pdf (URL resource last accessed 25/03/2025)
FAO/IIASA/ISRIC/ISS-CAS/JRC, 2009. Harmonized World Soil Database (version 1.1). FAO, Rome, Italy and IIASA, Laxenburg, Austria
Fu, C. C., D. Han, S. T. Kim, and P. Gloersen (1988). User's guide for the Nimbus- 7 Scanning Multichannel Microwave Radiometer (SMMR) CELL-ALL tape. NASA Reference Publication #1210, National Aeronautics and Space Administration, Washington, D.C.
Fung, A.K. (1994). Microwave scattering and emission models and their applications. Boston: Artech House
Gaiser, P.W., K. M. St. Germain, E. M. Twarog, G. A. Poe, W. Purdy, D. Richardson, W. Grossman, W. L. Jones, D. Spencer, G. Golba, J. Cleveland, L. Choy, R. M. Bevilacqua and P. S. Chang (2004), "The WindSat spaceborne polarimetric microwave radiometer: Sensor description and early orbit performance," IEEE Trans. Geosci. Remote Sens., vol. 42, 2347-2360, http://www.emc.ncep.noaa.gov/mmb/data_processing/satellite_ingest.doc/File_Format.doc/windsatdocjan06-1.pdf (URL resource last accessed 25/03/2025)
Gloersen, P., D. J. Cavalieri, A. T. C. Chang, T. T. Wilheit, W. J. Campbell, O. M. Johannessen, K. B. Katsaros, K. F. Kunzi, D. B. Ross, D. Staelin, E. P. L. Windsor, F. T. Barath, P. Gudmansen, E. Langham, and R. Ramseier (1984). A summary of results from the first Nimbus-7 SMMR observations. J. Geophys. Res. 89, 5335-5344.
GPM Science Team (2022), GPM GMI XCAL Common Calibrated Brightness Temperatures L1BASE 1.5 hours 13 km V07, Greenbelt, MD, USA, NASA Goddard Earth Science Data and Information Services Center (GES DISC), 10.5067/GPM/GMI/BASE-XCAL/07
Gruber, A., Dorigo, W., Crow, W., and Wagner, W. (2017), “Triple Collocation-Based Merging of Satellite Soil Moisture Retrievals”, IEEE trans. geosc. rem. sens., DOI: 10.1109/TGRS.2017.2734070
Gruber, A., Su, C.H., Crow, W.T., Zwieback, S., Dorigo, W.A., & Wagner, W. (2016a). Estimating error cross-correlations in soil moisture data sets using extended collocation analysis. Journal of Geophysical Research: Atmospheres, 121(3), 1208-1219.
Gruber, A., Su, C.H., Zwieback, S., Crow, W.T., Wagner, W., & Dorigo, W. (2016b). Recent advances in (soil moisture) triple collocation analysis. International Journal of Applied Earth Observation and Geoinformation, 45, 200-211.
Gruber, A., De Lannoy, G., Albergel, C., lL-yaari, A., Brocca, L., Calvet, J. C., Colliander, A., Cosh, M., Crow, W., Dorigo, W., Draper, C., Hirschi, M., Kerr, Y., Konings, A., Lahoz, W., Mccoll, K., Montzka, C., Munoz-Sabater, J., Peng, J., Reichle, R., Richaume, P., Rüdiger, C., Scanlon, T., Van Der Schalie, R., Wigneron, J. P. & Wagner, W. (2020). Validation practices for satellite soil moisture retrievals: What are (the) errors? Remote Sensing of Environment, 244, 111806.
Grillakis, M. G., Koutroulis, A. G., Alexakis, D. D., Polykretis, C., & Daliakopoulos, I. N. (2021). Regionalizing Root-Zone Soil Moisture Estimates From ESA CCI Soil Water Index Using Machine Learning and Information on Soil, Vegetation, and Climate. Water Resources Research, 57(5), e2020WR029249. doi:10.1029/2020WR029249
Gupta, H. V., Kling, H., Yilmaz, K. K., and Martinez, G. F. (2009): Decomposition of the mean squared error and NSE performance criteria: Implications for improving hydrological modelling, J. Hydrol., 377, 80–91, https://doi.org/10.1016/j.jhydrol.2009.08.003 (URL resource last accessed 25/03/2025)
Hersbach, H, Bell, B, Berrisford, P, et al. The ERA5 global reanalysis. Q J R Meteorol Soc. 2020; 146: 1999–2049. https://doi.org/10.1002/qj.3803 (URL resource last accessed 25/03/2025)
H SAF (2018a). ASCAT Surface Soil Moisture CDR2017 time series 12.5 km sampling – Metop (H113), EUMETSAT SAF on Support to Operational Hydrology and Water Management. http://dx.doi.org/10.15770/EUM_SAF_H_0005 (URL resource last accessed 25/03/2025)
H SAF (2018b). ASCAT Surface Soil Moisture CDR2017-EXT time series 12.5 km sampling – Metop (H114), EUMETSAT SAF on Support to Operational Hydrology and Water Management. https://navigator.eumetsat.int/product/EO:EUM:DAT:0108?query=H114&s=advanced (URL resource last accessed 25/03/2025)
H SAF (2018c) Algorithm Theoretical Baseline Document (ATBD), Metop ASCAT Soil Moisture Data Records v0.7 (H113) https://hsaf.meteoam.it/CaseStudy/GetDocumentUserDocument?fileName=ASCAT_SSM_CDR_ATBD_v0.7.pdf&tipo=ATBD (URL resource last accessed 25/03/2025)
Hillburn KA, and CL Shie, (2011) Decadal trends and variability in special sensor microwave imager (SSM/I) Brightness Temperatures and Earth Incidencs angle, NASA RSS Technical Report 092811
Holmes, T.R.H., De Jeu, R.A.M., Owe, M., & Dolman, A.J. (2009). Land surface temperature from Ka band (37 GHz) passive microwave observations. Journal of Geophysical Research -Atmospheres, 114
Hsieh, C.-Y., Fung, A.K., Nesti, G., Sieber, A.J., & Coppo, P. (1997). A further study of the IEM surface scattering model. IEEE Transaction on Geoscience and Remote Sensing, 35, 901-909
Jin, R.; Zhang, T.; Li, X.; Yang, X.; Ran, Y. Mapping Surface Soil Freeze-Thaw Cycles in China Based on SMMR and SSM/I Brightness Temperatures from 1978 to 2008. Arctic Antarct. Alp. Res. 2015, 47, 213–229.
Kerr, Y.H., Waldteufel, P., Wigneron, J.P., Delwart, S., Cabot, F., Boutin, J., Escorihuela, M.J., Font, J., Reul, N., Gruhier, C., Juglea, S.E., Drinkwater, M.R., Hahne, A., Martin-Neira, M., and Mecklenburg, S. (2010), “The SMOS mission: New tool for monitoring key elements of the global water cycle”, Proceedings of the IEEE, vol. 98, no. 5, doi: 10.1109/JPROC.2010.2043043.
Kottek, M., Grieser, J., Beck, C., Rudolf, B., & Rubel, F. (2006). World Map of the Köppen-Geiger climate classification updated. Meteorologische Zeitschrift, 15, 259-263
Leavesley, G. H., David, O., Garen, D. C., Lea, J., Marron, J. K., Pagano, T. C., Perkins, T. R., and Strobel, M. L. (2008): A Modeling Framework for Improved Agricultural Water Supply Forecasting
Lehner, B. & Döll, P., 2004. Development and validation of a global database of lakes, reservoirs and wetlands. Journal of Hydrology, 296(1-4), pp.1–22
Li, L., Njoku, E.G., Im, E., Chang, P.S., and St. German, K. (2004), “A preliminary survey of radio-frequency interference over the U.S. in Aqua AMSR-E data”, IEEE Trans. Geosc., vol. 42, no. 2, pp. 380 – 390, doi: 10.1109/TGRS.2003.817195.
Liu, Y., de Jeu, R.A.M., van Dijk, A.I.J.M., & Owe, M. (2007). TRMM-TMI satellite observed soil moisture and vegetation density (1998-2005) show strong connection with El Nino in eastern Australia. Geophysical Research Letters, 34, Art. No. L15401
Liu, Y.Y., Dorigo, W.A., Parinussa, R.M., De Jeu, R.A.M., Wagner, W., McCabe, M.F., Evans, J.P., & Van Dijk, A.I.J.M. (2012). Trend-preserving blending of passive and active microwave soil moisture retrievals. Remote Sensing of Environment, 123, 280-297
Liu, Y.Y., Parinussa, R.M., Dorigo, W.A., de Jeu, R.A.M., Wagner, W., van Dijk, A., McCabe, F.M., & Evans, J.P. (2011). Developing an improved soil moisture dataset by blending passive and active microwave satellite-based retrievals. Hydrology and Earth System Sciences, 15, 425-436
Meesters, A., De Jeu, R.A.M., & Owe, M. (2005). Analytical derivation of the vegetation optical depth from the microwave polarization difference index. IEEE Geoscience and Remote Sensing Letters, 2, 121-123
Mo, T., Choudhury, B.J., Schmugge, T.J., Wang, J.R., & Jackson, T.J. (1982). A model for microwave emission from vegetation-covered fields. Journal of Geophysical Research-Oceans and Atmospheres, 87, 1229-1237
Mironov, V.L., Dobson, M.C., Kaupp, V.H., Komarov, S.A., & Kleshchenko, V.N. (2004). Generalized refractive mixing dielectric model for moist soils. IEEE Transactions on Geoscience and Remote Sensing, 42, 773-785
Moesinger, L., Dorigo, W., de Jeu, R., van der Schalie, R., Scanlon, T., Teubner, I., and Forkel, M. (2020): The global long-term microwave Vegetation Optical Depth Climate Archive (VODCA), Earth Syst. Sci. Data, 12, 177–196, https://doi.org/10.5194/essd-12-177-2020 (URL resource last accessed 25/03/2025)
Muñoz-Sabater, J., Dutra, E., Agustí-Panareda, A., Albergel, C., Arduini, G., Balsamo, G., Boussetta, S., Choulga, M., Harrigan, S., Hersbach, H., Martens, B., Miralles, D. G., Piles, M., Rodríguez-Fernández, N. J., Zsoter, E., Buontempo, C., and Thépaut, J.-N. (2021): ERA5-Land: a state-of-the-art global reanalysis dataset for land applications, Earth Syst. Sci. Data, 13, 4349–4383, https://doi.org/10.5194/essd-13-4349-2021 (URL resource last accessed 25/03/2025)
Naeimi, V., Bartalis, Z., and Wagner, W., (2009). ASCAT soil moisture: An assessment of the data quality and consistency with the ERS scatterometer heritage. Journal of Hydrometeorology, 10(2), pp.555-563.
Naeimi, V., Paulik, C., Bartsch, A., Wagner, W., Kidd, R., Park, S.E., Elger, K. and Boike, J., 2012. ASCAT Surface State Flag (SSF): Extracting information on surface freeze/thaw conditions from backscatter data using an empirical threshold-analysis algorithm. IEEE Transactions on Geoscience and Remote Sensing, 50(7), pp.2566-2582.
Newell, D., Draper, D.,Figgins, D., Berdanier, B., Kubitschek, M., Holshouser, D., Sexton, A. , Krimchansky, S., Wentz, F., Meissner, T., "GPM microwave imager key performance and calibration results," 2014 IEEE Geoscience and Remote Sensing Symposium, 2014, pp. 3754-3757, doi: 10.1109/IGARSS.2014.6947300.
Njoku, E. (1996). Nimbus-7 SMMR Pathfinder brightness temperatures. Boulder, CO: National Snow and Ice Data Center
Njoku, E. G., B. Rague, And K. Flemming (1995): Nimbus-7 Scanning Multichannel Microwave Radiometer (SMMR): Brightness Temperature Data (SMMR Level 1B Pathfinder). JPL Publication, Jet Propulsion Laboratory, Pasadena, CA. 'User's Guide for the Scanning Multichannel Microwave Radiometer Instrument First Year Antenna Temperature Data Set', Systems & Applied Sciences Corporation, August 1982, NASA Contract NAS5-27393. 'Nimbus-7 SMMR Pathfinder Brightness Temperatures', NSIDC Dataset Guide Documentation.
O'Neill, P. E., S. Chan, E. G. Njoku, T. Jackson, R. Bindlish, and J. Chaubell. 2020a. SMAP L3 Radiometer Global Daily 36 km EASE-Grid Soil Moisture, Version 7. Boulder, Colorado USA. NASA National Snow and Ice Data Center Distributed Active Archive Center.
O'Neill, P. E., R. Bindlish, S. Chan, J. Chaubell, E. Njoku, and T. Jackson. 2020b. SMAP Algorithm Theoretical Basis Document: Level 2 & 3 Soil Moisture (Passive) Data Products, Revision F, August 31, 2020, SMAP Project, JPL D-66480, Jet Propulsion Laboratory, Pasadena, CA. (see https://nsidc.org/sites/nsidc.org/files/technical-references/L2_SM_P_AR_R17_Aug2020_clean_final.pdf (URL resource last accessed 25/03/2025)
O’Neill, P. E., S. Chan, R. Bindlish, M. Chaubell, A. Colliander, F. Chen, S. Dunbar, T. Jackson, J. Peng, M. Cosh, T. Bongiovanni, J. Walker, X. Wu, A. Berg, H. McNairn, M. Thibeault, J. Martínez-Fernández, Á. González-Zamora, E. Lopez-Baeza, K. Jensen, M. Seyfried, D. Bosch, P. Starks, C. Holifield Collins, J. Prueger, Z. Su, R. van der Velde, J. Asanuma, M. Palecki, E. Small, M. Zreda, J. Calvet, W. Crow, Y. Kerr, S. Yueh, and D. Entekhabi. 2020c. Calibration and Validation for the L2/3_SM_P Version 7 and L2/3_SM_P_E Version 4 Data Products, SMAP Project, JPL D-56297, Jet Propulsion Laboratory, Pasadena, CA. (see https://nsidc.org/sites/nsidc.org/files/technical-references/L2_SM_P_AR_R17_Aug2020_clean_final.pdf, (URL resource last accessed 25/03/2025)).
Owe M., R. de Jeu and J. Walker, "A methodology for surface soil moisture and vegetation optical depth retrieval using the microwave polarization difference index," in IEEE Transactions on Geoscience and Remote Sensing, vol. 39, no. 8, pp. 1643-1654, Aug. 2001. doi: 10.1109/36.942542
Owe, M., de jeu, R., & Holmes, T. (2008). Multisensor historical climatology of satellite-derived global land surface moisture. Journal of Geophysical Research-Earth Surface, 113, F01002
Owe, M., & Van de Griend, A.A. (1998). Comparison of soil moisture penetration depths for several bare soils at two microwave frequencies and implications for remote sensing. Water Resour. Res., 34, 2319-2327
Parinussa, R, TRH Holmes and RAM de Jeu (2012), Soil moisture retrievals from the WindSat spaceborne polarimetric microwave radiometer. IEEE Trans. Geosci. Remote Sens., DOI: 10.1109/TGRS.2011.2174643
Parinussa, R.M., Meesters, A., Liu, Y.Y., Dorigo, W., Wagner, W., & de Jeu, R.A.M. (2011). Error Estimates for Near-Real-Time Satellite Soil Moisture as Derived From the Land Parameter Retrieval Model. IEEE Geoscience and Remote Sensing Letters, 8, 779-783
Parinussa, R. M., R. H. Thomas, N. W. Holmes, A. D. Wouter, A. M. Richard, and R. A. de Jeu. (2014). “A Preliminary Study toward Consistent Soil Moisture from AMSR2.” Journal of Hydrometeorology 16 (2): 932–947. doi:10.1175/JHM-D-13-0200.1
Parinussa RM, De Jeu RAM, Van der Schalie R, Crow WT, Lei F, Holmes TRH. A Quasi-Global Approach to Improve Day-Time Satellite Surface Soil Moisture Anomalies through the Land Surface Temperature Input. Climate. 2016; 4(4):50. https://doi.org/10.3390/cli4040050 (URL resource last accessed 25/03/2025)
Pasik, A., Gruber, A., Preimesberger, W., De Santis, D., and Dorigo, W. (2023): Uncertainty estimation for a new exponential-filter-based long-term root-zone soil moisture dataset from Copernicus Climate Change Service (C3S) surface observations, Geosci. Model Dev., 16, 4957–4976, https://doi.org/10.5194/gmd-16-4957-2023 (URL resource last accessed 25/03/2025).
Paulik, C., Dorigo, W., Wagner, W., & Kidd, R. (2014). Validation of the ASCAT Soil Water Index using in situ data from the International Soil Moisture Network. International Journal of Applied Earth Observation and Geoinformation, 30, 1-8.
Peplinski, N.R., Ulaby, F.T., & Dobson, M.C. (1995). Dielectric properties of soils in the 0.3-1.3 GHz range. IEEE Transactions on Geoscience and Remote Sensing, 33, 803-807
Preimesberger, W., Scanlon, T., Su, C. -H., Gruber, A. and Dorigo, W., Homogenization of Structural Breaks in the Global ESA CCI Soil Moisture Multisatellite Climate Data Record, in IEEE Transactions on Geoscience and Remote Sensing, vol. 59, no. 4, pp. 2845-2862, April 2021, doi: 10.1109/TGRS.2020.3012896
Preimesberger, W. et al. (2023) C3S Soil Moisture Version v202312: Product Quality Assurance Document. Document ref: C3S2_312a_Lot4.WP2-PDDP-SM-v2_202306_SM_PQAD-v5_i1.1. Available online: SM v202312: Product Quality Assurance Document (PQAD) (URL resource last accessed 25/03/2025)
Reichle, R.H., Koster, R.D., Dong, J., & Berg, A.A. (2004). Global Soil Moisture from Satellite Observation, Land Surface Models, and Ground Data: Implications for Data Assimilation. Journal of Hydrometeorology, 5, 430-442
Rodell, M. et al., 2004. The Global Land Data Assimilation System. Bulletin of the American Meteorological Society, 85, pp.381–394.
Rui, H., Beaudoing, H., Loeser, C. and Li, B. (2018). README Document for NASA GLDAS Version 2 Data Products. [online] Hydro1.gesdisc.eosdis.nasa.gov. Available at: https://hydro1.gesdisc.eosdis.nasa.gov/data/GLDAS/README_GLDAS2.pdf. (URL resources last accessed 25/03/2025).
Schaefer, G.L.; Paetzold, R.F. SNOTEL (SNOwpack TELemetry) and SCAN (soil climate analysis network). In Automated Weather Stations for Applications in Agriculture and Water Resources Management: Current Use and Future Perspectives; University of Nebraska: Lincoln, NE, USA, 2001; Volume 1074, pp. 187–194
Schaefer, G., Cosh, M., and Jackson, T. (2007): The USDA natural resources conservation service soil climate analysis network (SCAN), Journal of Atmospheric and Oceanic Technology - J ATMOS OCEAN TECHNOL, 24, 2073 – 2077.
Schmugge, T.J., O'Neill, P.E., & Wang, J.R. (1986). Passive microwave soil moisture research. IEEE Transaction on Geoscience and Remote Sensing, GE-24, 12-22
Schneeberger, K., Schwank, M., Stamm, C., de Rosnay, P., Matzler, C., & Fluhler, H. (2004). Topsoil structure influencing soil water retrieval by microwave radiometry. Vadose Zone Journal, 3, 1169-1179
Seto, S.; Takahashi, N.; Iguchi, T. Rain/No-Rain Classification Methods for Microwave Radiometer Observations over Land Using Statistical Information for Brightness Temperatures under No-Rain Conditions. J. Appl. Meteorol. 2005, 44, 1243–1259.
Stradiotti, P., & Preimesberger, W. (2024). ESA CCI SM RZSM Long-term Climate Record of Root-Zone Soil Moisture from merged multi-satellite observations (9.1). TU Wien. doi:10.48436/rvjsz-e8y12
Su, C.-H., Ryu, D., Dorigo, W., Zwieback, S., Gruber, A., Albergel, C., Reichle, R. H., and Wagner, W. (2016), Homogeneity of a global multisatellite soil moisture climate data record, Geophys. Res. Lett., 43, 11,245–11,252, doi:10.1002/2016GL070458.
Taylor, J. R. (1997). An introduction to error analysis: The study of uncertainties in physical measurements (2nd ed. ed.). University Science Books.
TU Wien (2013). ERS AMI-WS (ESCAT) Surface Soil Moisture Product generated from E1/2-SZ-WNF/UWI-00 dataset. Department of Geodesy and Geoinformation, TU Wien, 2013.
Ulaby, F.T., Moore, B., & Fung, A.K. (1981). Microwave Remote Sensing - Active and Passive, Vol. I: Fundamentals of Radiometry. Addison-Weslay, 56 pp
Ulaby, F.T., Moore, B., & Fung, A.K. (1982). Microwave Remote Sensing - Active and Passive, Vol. II: Radar Remote Sensing and Surface Scattering and Emission Theory. Norwood: Artech
Uppala, S.M. et al., 2005. The ERA-40 re-analysis. Quarterly Journal of the Royal Meteorological Society, 131(612), pp.2961–3012.
Van der Schalie, R., De Jeu, R.A.M., Kerr, Y.H., Wigneron, J.-P., Rodriguez-Fernandez, N.J., Al-Yaari, A., Parinussa, R.M., Mecklenburg, S., and Drusch, M. (2017), “The merging of radiative transfer based surface soil moisture data from SMOS and AMSR-E”, Remote Sensing of Environment, vol. 189, doi: http://dx.doi.org/10.1016/j.rse.2016.11.026 (URL resource last accessed 25/03/2025).
Van der Schalie, R., Kerr, Y.H., Wigneron, J.P., Rodriguez-Fernandez, N.J., Al-Yaari, and De Jeu, R.A.M. (2016), “Global SMOS Soil Moisture Retrievals from The Land Parameter Retrieval Model”, Int. J. Appl. Earth Observ. Geoinf., doi: http://dx.doi.org/10.1016/j.jag.2015.08.005 (URL resource last accessed 25/03/2025).
Van der Schalie, R., Parinussa, R.M., De Jeu, R.A.M., Kerr, Y.H., Wigneron, J.P., Rodriguez-Fernandez, N.J., Al-Yaari, A., Mecklenburg, S., and Drusch, M. (2018), “The Effect of Three Different Data Fusion Approaches on the Quality of Soil Moisture Retrievals from Multiple Passive Microwave Sensors”, Remote Sensing, vol. 10 (1), no. 107, doi: https://doi.org/10.3390/rs10010107 (URL resource last accessed 25/03/2025).
van der Schalie, R., van der Vliet M, Rodríguez-Fernández N, Dorigo WA, Scanlon T, Preimesberger W, Madelon R, de Jeu RAM. L-Band Soil Moisture Retrievals Using Microwave Based Temperature and Filtering. Towards Model-Independent Climate Data Records. Remote Sensing. 2021; 13(13):2480. https://doi.org/10.3390/rs13132480 (URL resource last accessed 25/03/2025).
Van der Vliet, Mendy, Robin van der Schalie, Nemesio Rodriguez-Fernandez, Andreas Colliander, Richard de Jeu, Wolfgang Preimesberger, Tracy Scanlon, and Wouter Dorigo (2020). Reconciling Flagging Strategies for Multi-Sensor Satellite Soil Moisture Climate Data Records. Remote Sensing 12, no. 20: 3439.
Wagner, W. (1998). Soil Moisture Retrieval from ERS Scatterometer Data. In, Institute for Photogrammetry and Remote Sensing. Vienna: Technical University of Vienna
Wagner, W., Lemoine, G., Borgeaud, M., & Rott, H. (1999a). A Study of Vegetation Cover Effects on ERS Scatterometer Data. IEEE Transactions on Geoscience and Remote Sensing, 37, 938-948
Wagner, W., Lemoine, G., & Rott, H. (1999b). A Method for Estimating Soil Moisture from ERS Scatterometer and Soil Data. Remote Sensing of Environment, 70, 191-207
Wagner, W., Noll, J., Borgeaud, M., & Rott, H. (1999c). Monitoring soil Moisture over the Canadian Prairies with the ERS Scatterometer. IEEE Trans. Geosci. Rem. Sens., 37, 206-216
Wagner, W., & Scipal, K. (2000). Large-Scale Soil Moisture Mapping in western Africa using the ERS Scatterometer. IEEE Trans. Geosci. Rem. Sens., 38, 1777-1782
Wang, J.R., & Choudhury, B.J. (1981). Remote sensing of soil moisture content over bare field at 1.4 GHz frequency. Journal of Geophysical Research-Oceans and Atmospheres, 86, 5277-5282
Wang, J.R., & Schmugge, T.J. (1980). An empirical model for the complex dielectric permittivity of soils as a function of water content. IEEE Transactions on Geoscience and Remote Sensing, 18, 288-295
Wang, T., Franz, T., You, J., Shulski, M., & Ray, R. (2017). Evaluating controls of soil properties and climatic conditions on the use of an exponential filter for converting near surface to root zone soil moisture contents. Journal of Hydrology, 548, 683-696.
Wentz, F. J. (1991), User's Manual: SSM/I Antenna Temperature Tapes (Revision 1), report number 120191, Remote Sensing Systems, Santa Rosa, CA, 73 pp. (available online: https://images.remss.com/papers/rsstech/1991_120191_Wentz_SSMI_TA_manual_rev1.pdf, URL resource last accessed 25/03/2025)
Wentz, F. J. (1993), User's Manual: SSM/I Antenna Temperature Tapes (Revision 2), report number 120193, Remote Sensing Systems, Santa Rosa, CA, 36 pp. (available online: https://images.remss.com/papers/rsstech/1993_120193_Wentz_SSMI_TA_manual_rev2.pdf, URL resource last accessed 25/03/2025)
Wentz, F. J., L. Ricciardulli, K. A. Hilburn, and C. A. Mears (2007), How much more rain will global warming bring?, Science, 317, 233-235.
WindSat Data Products Users’ Manual, Sensor & Environmental Data Records, Version 3.0, January 2006, D- 29825, JPL.
WMO (2016). The Global Observing System for Climate (GCOS): Implementation Needs GCOS-200. Available online: https://unfccc.int/files/science/workstreams/systematic_observation/application/pdf/gcos_ip_10oct2016.pdf. (URL resource last accessed 25/03/2025)
Xu, Z., Qian, J., Xian, D., Qi, Y. "Fengyun-3 Series Meteorological Satellite Data Archiving and Service System," 2016 IEEE International Geoscience and Remote Sensing Symposium (IGARSS), 2016, pp. 5477-5480, doi: 10.1109/IGARSS.2016.7730427.
Yang, H., Zou, X., Li, X.,You, R., "Environmental Data Records From FengYun-3B Microwave Radiation Imager," in IEEE Transactions on Geoscience and Remote Sensing, vol. 50, no. 12, pp. 4986-4993, Dec. 2012, doi: 10.1109/TGRS.2012.2197003.
Yang, H., Weng, F., Lv, L., Lu, N., Liu, G., Bai, M. Qian, Q., He, J., Xu, H., "The FengYun-3 Microwave Radiation Imager On-Orbit Verification," in IEEE Transactions on Geoscience and Remote Sensing, vol. 49, no. 11, pp. 4552-4560, Nov. 2011, doi: 10.1109/TGRS.2011.2148200.
Zhang, T., Barry, R.G., Knowles, K., Ling, F. & Armstrong, R.L., 2003. Distribution of seasonally and perennially frozen ground in the Northern Hemisphere. In: B. Phillips, S. Springman & L. Arenson, eds. Permafrost. Lisse: Swets & Zeitlinger, pp. 1289-1294. ISBN 90 5809 582 7.
Zwieback, S., Colliander, A., Cosh, M. H., Martínez-Fernández, J., McNairn, H., Starks, P. J., Thibeault, M., and Berg, A.: Estimating time-dependent vegetation biases in the SMAP soil moisture product, Hydrol. Earth Syst. Sci., 22, 4473–4489, 2018.











































