Quantifying Snow–Ground Backscatter Uncertainty: A Bayesian Approach Using Multifrequency SAR and In-Situ Observations

Highlights

• This study validates the stepwise approach to estimate the snowpack bottom boundary condition by splitting snow–ground backscatter from volume backscatter in active snow microwave retrievals.
• The parsimonious three-parameter QHN frequency-independent soil reflectivity model is best suited for active snow microwave.
• There is a substantive dependence of total backscatter on ground properties at the X-band (increasing ground surface roughness reduced the simulated backscatter by ~1.5 dB across the tested range, and increasing the specular-to-total reflectivity ratio (STRR) produced an additional ~1.0 dB decrease), while there was negligible to very weak sensitivity to ground parameters at the Ku-band.
• The retrieval sensitivity to STRR is minimized in the 0.6–0.7 range and it can be fixed at 0.65 without having discernible impact.
• Backscatter uncertainty at the snow–ground interface preferentially impacts the estimation of soil dielectric properties.

Abstract

Accurate estimation of snowpack microwave backscatter is critical for retrieving key physical properties of snow, such as snow depth (SD) and snow water equivalent (SWE), typically modeled using radiative transfer models (RTM). Among the various sources of uncertainty in RTM simulations, snow–ground reflectivity—used as a boundary condition—plays a critical role in influencing the accuracy of simulated backscatter. This study leverages high-resolution X- and Ku-band synthetic aperture radar (SAR) backscatter aircraft measurements using SWESARR and SnowSAR from NASA’s SnowEx campaigns, co-located with in situ snow pit observations in Grand Mesa, Colorado, and uses a Bayesian MCMC parameter optimization model with RTM framework to estimate the key ground parameters such as surface roughness, moisture content, and specular-to-total reflectivity ratio (STRR) governing the estimation of the snow–ground reflectivity and quantify the uncertainties associated with them. At the X-band, increasing ground surface roughness reduced the simulated backscatter by ~1.5 dB across the tested range, increasing the STRR produced an additional ~1.0 dB decrease while the dielectric properties of the ground are highly sensitive to the moisture content of frozen soil, and increasing the moisture content even by 2% increased the backscatter by 2–3 dB. The retrieval sensitivity to the STRR is minimized in the 0.6–0.7 range and it can be fixed at 0.65 without having discernible impact. The Bayesian inversion reveals that the extreme parameter values act as diagnostic indicators of unmodeled complexity rather than retrieval failures, with representativeness error often dominating over instrument noise. The study provides a robust methodology for the estimation of the snow–ground backscatter boundary condition for forward modeling, ultimately aiding SWE and SD retrieval from active microwave observations. While this study relied on Grand Mesa, the framework developed here is general and, along with the model uncertainty, is directly transferable and broadly applicable to other snow-dominated mountain regions where active microwave observations can be used for snowpack monitoring.

1. Introduction

Seasonal snowpack is a vital component of the Earth’s climate system as it provides freshwater supply to almost one-sixth of the population [1,2] and significantly influences soil moisture, surface runoff, and hence the hydrologic cycle [3,4,5]. Because the snowpack has high albedo, it reflects much of the incoming solar radiation and strongly affects the Earth’s energy balance [6,7]. Thus, it is critical to accurately map the snowpack and have precise estimates of snow mass properties such as snow water equivalent (SWE) and snow depth (SD). Since the availability of in situ data is limited and even unavailable over vast regions of the planet, mapping snow mass properties using remotely sensed information is of great importance. Many studies have used remotely sensed satellite data to map and predict SWE, SD, and other snowpack physical properties [8]. Brightness temperature from passive microwave data has been previously used for these retrievals [9,10,11]. The increasing availability of multifrequency Synthetic Aperture Radar (SAR)—including X, Ku, C, S, and L-band—enables snow mapping at very high spatial resolutions (10s of meters), which is critical for capturing its inherent spatial variability. When integrated with physical models via data assimilation, these detailed observations can effectively constrain simulations of multiscale snowpack dynamics, which is essential for predicting snowmelt and snow water resources.

RTMs like the Microwave Emission Model of Layered Snowpacks (MEMLS) [12,13], Dense Media Radiative Transfer (DMRT) [14], and Snow Microwave Radiative Transfer (SMRT) [15] are used to calculate the total backscatter from snow surfaces using physical estimates of the snow depth, density, grain size, temperature and dielectric properties of the ground as the boundary condition. Typically, the physical properties of snow are simulated using physics-based models (PBMs) like the multilayer snow hydrology model (MSHM) [16,17], SNOWPACK [18], and CROCUS [19]. The estimation of backscatter from coupled PBM-RTM models (i.e., forward modeling) is impacted by various sources of uncertainty. These include errors in input weather forcing data, uncertainty in model parameters, and structural errors in the models themselves due to missing processes (e.g., wind redistribution) and empirical parameterizations (e.g., microphysics). The fundamental objective is to improve the estimation of backscatter that reaches to the satellite. The total snowpack backscatter consists of three major components: backscatter at the snow–air interface that is negligible for dry snow conditions, volume backscatter, and backscatter at the snow–ground interface. Singh et al. (2024) [20] modified Pan et al. (2024) [21] Bayesian snow retrieval algorithm by introducing a PBM to derive snowpack priors and by splitting the retrieval into two steps (snow–ground backscatter first, and volume backscatter second) to better constrain the retrieval by improving the snowpack bottom boundary condition and by reducing the number of physical parameters being estimated at each step. However, the study did not include an explicit evaluation of intermediate estimates of snow–ground backscatter and ground parameters.

In this work, the focus is on the characterization of parameter uncertainty and RTM sensitivity to the physical parameterizations and parameters used to describe snow–ground backscatter interactions. For this purpose, data from NASA SnowEx field campaigns, and in particular snow pit data consisting of SWE, SD, grain size, and other snow microstructure properties and their stratigraphy are imported to the RTM to directly estimate backscatter from the snowpack, thus reducing uncertainties through the forcing data and the PBM. These direct forward estimates of snowpack backscatter are subsequently confronted against NASA’s SnowEx airborne X- and Ku-band SAR measurements using SWESARR and SnowSAR over regions of Colorado, USA toward improving the estimates of RTM parameters, thus reducing the uncertainty in the total backscatter calculation.

The total snowpack backscatter that reaches back to the satellite depends upon many factors including the physical properties of the snowpack (e.g., snow grain size, snow liquid water content, snow density, and snow depth), ground boundary conditions (e.g., snow–ground reflectivity which in turn depends on the dielectric constant, soil temperature, volumetric moisture content of soil, surface roughness) as well as sensor properties (e.g., frequency, polarization, viewing geometry) [22,23]. By using the SnowEx pit data to describe the snowpack, the main source of uncertainty is the boundary condition at the bottom of the snowpack proper, i.e., the calculation of snow–ground reflectivity.

To calculate the ground reflectivity, Wang and Chaudhary (1981) [24] proposed a semi-empirical model (hereafter referred to as the QHN model) using three free parameters, roughness height (HR), a polarization mixing parameter (QR), and a parameter accounting for the angular dependency of the reflectivity (NR). Wëgmuller and Mätzler (1999) [25] showed that there is a strong correlation between the vertical (V-Pol) and horizontal polarization (H-Pol) reflectivity and proposed a reflectivity model (hereafter referred to as the WM99 model) based on previous work by Mo and Schmugge (1987) [26]. They calculated H-Pol reflectivity using states such as soil temperature, soil roughness, and soil moisture, and, in a second step, the V-Pol reflectivity can be estimated from the modeled H-Pol reflectivity. Moreover, there are numerical models like NMM3D (Numerical Maxwell Model in 3D), which is a full-wave electromagnetic solver used to model rough surface scattering by solving Maxwell’s equations in three dimensions based on the Method of Moments (MoM) as in [14,27]. Although accurate when compared to other soil reflectivity models, NMM3D has a very high computational cost, so it is challenging to implement at a large scale. All these reflectivity models require the knowledge of the soil dielectric constant, which depends on the soil states and properties like moisture content, texture, bulk density, temperature, organic content, etc., and the frequency of the sensor. Dobson et al. (1985) used these parameters to compute the soil permittivity by treating the soil as a mixture of bound and free water in a dielectric matrix [28,29]. Nevertheless, the moisture content of frozen soil is difficult to calculate and to address this challenge, Wu et al. (2022) modified the Dobson model using semi-empirical equations for the moisture content of frozen soil [30].

All these models require the specification of many parameters that are difficult to observe or estimate, like specular reflectivity for the snow–ground interface and the surface roughness of the soil, and a wide range of values have been assumed across various studies. For example, [31] constrained STRR to the range 0.25–0.75, [32] fixed STRR at 0.9 and ground permittivity ϵ_g at 4, and [33] specified frozen soil permittivity as ϵ_g = 5 + i0.5. Whereas specific values may be optimum for local applications, it is difficult to apply them generally, especially in remote places where no ancillary data are available and thus local conditions are not known. There is, therefore, a critical need to develop a robust general methodology to estimate these parameters to improve the estimation of snow–ground reflectivity. Ref [20] treated them as parameters in a Bayesian framework (Base-AM) using an iterative Monte Carlo Markov Chain algorithm to retrieve SWE and SD from SAR backscatter at the X- and Ku-bands using the dielectric constant from the Dobson model. SWE and SD retrievals are tied to the volume backscatter component, and in order to derive the volume backscatter from the total backscatter measurements, it is critical to have accurate estimates of snow–ground backscatter as well as the uncertainties associated with it.

In this study, we aim to improve the estimation of the total backscatter of the snow–ground system by quantifying the uncertainty in snow–ground backscatter estimates by evaluating soil reflectivity models and constraining their most sensitive parameters. The use of in situ data for snowpack properties eliminates the errors that propagate through the PBM and enables us to target the uncertainties in snow–ground reflectivity. Sensitivity analysis of different soil reflectivity models and evaluation against the measured SAR values provide support for selecting the best-suited model to represent the bottom boundary condition for the snowpack. Moreover, it is possible to infer a range for each of the uncertain parameters. These ranges and the mean value of roughness height, STRR of the soil, and frozen moisture content (Mv) were then used as priors in the Bayesian MCMC optimization model, as in [20], to optimize the ground backscatter and estimate values to describe the dielectric behavior of frozen soil. Constraining these parameters and their uncertainties provides the robust boundary conditions necessary to improve the accuracy of radiative transfer models for snowpack remote sensing.

2. Materials and Methods

2.1. Study Area

The study region is Grand Mesa, Colorado, a plateau that is 2000 m above adjacent low-lying areas and is surrounded by ridges up to 500 m in elevation (Figure 1). Grand Mesa has an alpine climate, experiencing snowfall throughout the year except during July and August. Land cover is heterogeneous, with grasslands in the west and a mix of evergreen and deciduous forests to the east. It has been a key site for NASA’s SnowEx campaigns, offering valuable in situ and remote sensing data for studying snow accumulation, melt dynamics, and snow–ground interactions. The following sections describe these datasets, their preprocessing, and the modeling framework used in this study.

2.2. Data

2.2.1. SAR Backscatter (SnowSAR and SWESARR)

During SnowEx’17, airborne microwave backscatter measurements were made in Grand Mesa on 21 February 2017 at 1 m resolution using SnowSAR. The SnowSAR instrument is a dual-frequency (X and Ku band) radar. A total of six flight lines were completed, two short ones on sloped, densely forested terrain and four long lines on the plateau. The flights took place in the early afternoon between 18:00 and 21:00 GMT (12:00–15:00 MST). SnowSAR data quality control measures included filtering based on aircraft attitude to mitigate the impact of turbulence in some of the segments, beam incidence angle (θ₀) or antenna pattern, and signal-to-noise ratio of the backscatter coefficients. Processing of the original airborne SAR measurements and quality control indicate that only the co-pol X-band HH- and VV-pol and Ku-band VV-pol measurements are adequate for retrieval [20]. Geolocation was verified against corner reflector targets and geographic features.

During SnowEx’20, the SWESARR (version 3) instrument provided X-band VV-polarized airborne backscatter measurements at 1 m resolution over Grand Mesa on 11–12 February 2020, across six flights. The flights took place in the late afternoon between 17:00 and 18:00 GMT (10:00–11:00 MST) on the 11th and between 18:30 and 19:30 GMT (11:30–12:30 MST) on the 12th.

Manickam and Barros 2020 [34] performed a scaling analysis of Sentinel-1 C-band and UAVSAR L-band SAR backscatter over Grand Mesa and found that the scaling behavior at small scales (<100 m) shows negligible temporal sensitivity and the spectral slope is consistent with the SRTM DEM at the same scales for the C- and L-band for snowpacks in open areas. This independence of frequency suggests that the snow–ground boundary condition governs the backscatter scaling behavior for dry snow conditions and there is, therefore, a physical basis to explore multifrequency SAR data for retrieving snow properties without extensive calibration using ground observations. For this study, both the SWESARR and SNOWSAR data were aggregated to 30 m resolution by simple averaging of all SWESARR measurements within each pixel to reduce the variance in the data. All the information about the SAR data is summarized in

Table 1. Information of the SAR flights used in this study (SnowSAR and SWESARR—where “F” is frequency, “b” is band and “ΔS” is resolution).

NSIDC SAR Data File Naming Convention	Flight Name (Used in the Study)	Date	Time (GMT)	Band	Pol	ΔS (m)
20170221181138<F>G_<b>.nc	181138	21-02-2017	18:11:38	X, Ku	VV, HH	1
20170221184320<F>G_<b>.nc	184320	21-02-2017	18:43:20	X, Ku	VV, HH	1
20170221185902<F>G_<b>.nc	185902	21-02-2017	18:59:02	X, Ku	VV, HH	1
20170221202338<F>G_<b>.nc	202338	21-02-2017	20:23:38	X, Ku	VV, HH	1
20170221172126<F>G_<b>.nc	172126	21-02-2017	17:21:26	X, Ku	VV, HH	1
20170221173206<F>G_<b>.nc	173206	21-02-2017	17:32:06	X, Ku	VV, HH	1
GRMST1_27401_20007_005_200211_09225VV_XX_01.tif	005	11-02-2020	17:01:07	X	VV	1
GRMST1_27702_20007_009_200211_09225VV_XX_01.tif	009	11-02-2020	17:25:17	X	VV	1
GRMST1_27503_20007_012_200211_09225VV_XX_01.tif	012	11-02-2020	17:50:03	X	VV	1
GRMST1_27502_20008_025_200212_09225VV_XX_01.tif	025	12-02-2020	19:02:37	X	VV	1
GRMST1_27021_20008_021_200212_09225VV_XX_01.tif	021	12-02-2020	18:38:38	X	VV	1
GRMST1_27403_20008_029_200212_09225VV_XX_01.tif	029	12-02-2020	19:26:28	X	VV	1

, and the flight lines are mapped in Figure 2a.

2.2.2. Snow Pit Data

SnowEx pit measurements are available in 2017 [35] and 2020 [36]. Each snow pit dataset (see Figure 2 for locations) includes the vertical profile of temperature, stratigraphy, grain size, grain type, wetness, snow depth, snow density, and snow water equivalent (SWE).

Table 2. Co-located snow pits with the observed SAR data that are used in this study (* represents pits whose stratigraphy data were missing and were reconstructed using the nearby pit).

NSDIC Pit Name	Pit Name (Used in the Study)	Latitude	Longitude	Date	Local Time
28S	A1	39.0122478	−108.1379938	25-02-2017	11:00
78N	A2	39.04342878	−107.9202531	25-02-2017	15:10
92E	A3	39.0510518	−107.885109	22-02-2017	10:00
92W	A4	39.0510159	−107.8876494	22-02-2017	13:25
KC1C	A5	39.01363394	−108.1838735	20-02-2017	10:30
MTR4_0000	A6	39.0300503	−108.0331353	24-02-2017	10:15
MTR4_0800	A7	39.03005659	−108.0332395	24-02-2017	10:09
MTR4_1390	A8	39.03005509	−108.0332972	24-02-2017	10:00
MTR4_2000	A9	39.03005329	−108.0333664	24-02-2017	10:08
MTR4_2500	A10	39.03005179	−108.0334241	24-02-2017	10:00
KC1S *	A11	39.01344468	−108.1838766	20-02-2017	12:45
KC1N *	A12	39.01381389	−108.1838816	20-02-2017	13:00
67N *	A13	39.03245119	−108.0291492	22-02-2017	12:20
KC1W *	A14	39.01362669	−108.1841388	20-02-2017	13:46
MTR4_4500 *	A15	39.03005478	−108.0336552	24-02-2017	10:00
KC1E *	A16	39.01363219	−108.1836079	20-02-2017	12:30
1S1	B1	39.02119889	−108.20559	29-01-2020	09:05
1S2	B2	39.019948	−108.203396	08-02-2020	09:37
2S3	B3	39.021089	−108.202889	29-01-2020	10:35
2S4	B4	39.017951	−108.201292	05-02-2020	09:30
2S7	B5	39.01866002	−108.197788	08-02-2020	11:35
3S5	B6	39.01911256	−108.1986242	29-01-2020	12:10

provides all the relevant information for each snow pit. Because there are multiple flight lines, there are more than one backscatter measurement for some pits, and consequently distinct forward model simulations were conducted for the same pixels. Backscatter measurements and simulations at pit locations were organized by flight line and viewing angle and each given a reference number as presented in Table 2 to simplify the notation.

2.3. Methods

The RTM used in this study is the Microwave Emission Model of Layered Snowpack 3 and Active (MEMLS3&a) ([12,13], see also Section 2.3.2). The snow pit profile measurements of temperature, stratigraphy, grain size, grain type, wetness, SD, snow density, and SWE were given as input to the MEMLS along with the snow–ground reflectivity (X-band and frequency-independent) estimated using both WM99 and QHN. By comparing the estimated backscatter for different sets of parameters against the co-located SAR backscatter, the best-suited model was selected for this study.

The ground parameters for which the in situ measurements or direct calculations are not available, thus generating uncertainty in the estimates, are STRR, surface roughness, and moisture content. For the preliminary sensitivity analysis, soil moisture content was calculated using the modifications from [30] and a sensitivity analysis of backscatter to a range of surface roughness and STRR values was conducted. These backscatter estimates were compared against the SAR measurements averaged to 30 m resolution to derive the parameter range for which the calculated total backscatter is in good agreement with the observed total backscatter. The sensitivity analysis provided a feasible range for STRR and surface roughness of each pit and insights into the change in backscatter due to changing parameters.

Next, the range for each parameter was used to construct priors for input to the Bayesian optimization model. Separately, the ground truth snow pit data with imposed nil snow–ground reflectivity were used in MEMLS to estimate the volume backscatter, which was subtracted from the observed total backscatter to infer the contribution of ground backscatter (taken as the “measured” ground backscatter) to be used in the multi-step implementation of BASE-AM as described by [20] as the observed value, accounting for 0.5 dB error for instrument bias. This resulted in a set of parameters for each case of co-located snow pits and SAR pixels. The posterior distribution was then used for quantification of error associated with each parameter and the possible factors contributing to high positive or negative bias relative to the estimates of “measured” ground backscatter were explored. Figure 3 depicts the detailed workflow of the methodology used in this study.

2.3.1. Co-Locating Pits and SAR Measurements

To ensure a precise spatial match among SAR observations and in situ snow measurements, only the snow pits within the spatial and temporal extent of SAR acquisitions were used. The total observed backscatter at each pit location was then extracted from the co-located SAR pixel as described above. There were no snow pit measurements along the SAR flight lines on the exact day of the flights, and thus snow pit data were surveyed within a few days of the flights assuming that the snowpack does not change significantly in the absence of snowstorms or other precipitation events from one day to another in the winter. Precipitation data from the SNOTEL station at Mesa Lakes were used to identify the period of time with minimal or no snowfall before and after the SAR flights (Figure S9). Only snow pits excavated during this temporal window and located within the SAR flightlines were considered for analysis to minimize the influence of fresh snow accumulation on backscatter.

Furthermore, since this study focuses on understanding the processes at the snow–ground interface, snow pits within a 90 m radius of forested pixels were excluded to reduce confounding effects from vegetation. Based on these spatial, temporal, and environmental constraints, a total of 32 snow pits met the selection criteria—26 from the 2017 SnowEx campaign and 6 from the 2020 campaign. Stratigraphy data were unavailable for 16 of these pits in 2017. Of these, 6 pits were in spatial proximity to the pits with complete stratigraphic profiles. Based on the assumption that the vertical stratigraphy of snow grain size is spatially homogeneous among nearby pits, the grain size profiles for these 6 pits were reconstructed using data from adjacent sites. This allowed for the consideration of total 22 pits in the final analysis: 16 pits from SnowEx’17 with co-located VV- and HH-polarized X-band and VV-polarized Ku-band SnowSAR measurements, and 6 pits from SnowEx’20 with co-located VV-polarized X-band SWESARR measurements (Figure 2b,c). Details for all snow pits are provided in Table 2.

2.3.2. Models

• MEMLS3&a snow backscattering model

The radiative transfer model employed in this study to simulate snow–ground backscatter is the Microwave Emission Model for Layered Snowpacks 3 and Active (MEMLS3&a, hereafter MEMLS) based on the improved Born approximation [12,13]. The model assumes a Lambertian distribution for the diffuse part of the bistatic scattering coefficient. MEMLS uses key snowpack properties—including snow depth, SWE, correlation length, temperature, and liquid water content—and sensor parameters (frequency, polarization, incidence angle) to estimate the backscattered signal. The total snow reflectivity computed by passive MEMLS (r) is decomposed into a specular component ($r_s$) and a diffuse component ($r_d)$. The specular term is derived from the specular portion of the soil reflectivity, attenuated by snow absorption and scattering effects as the signal propagates through each snow layer (see Equation (14) in [12]). The diffuse term ($r_d=r-r_s)$ is then converted into the diffuse component of the backscattering coefficient (σ_d) using the Lambertian assumption

$${\sigma }_d^0=4r_d{\mu }_0^2$$

(1)

where μ₀ = cos (θ₀) and θ₀ is the incidence angle. The specular part of backscatter is calculated using the specular part of reflectivity (r_s) (see Equation (9) in [12]). Finally, the total backscatter is calculated using

$${{\sigma }_{pp}^{\prime }}^0=\left\{\begin{array}{c}\left(1-Q\right){\sigma }_{d,v}^0+{\sigma }_s^0 p=p^{\prime }=v \\ \left(1-Q\right){\sigma }_{d,h}^0+{\sigma }_s^0 p=p^{\prime }=h \\ {\displaystyle \frac{Q\left({\sigma }_{d,v}^0+{\sigma }_{d,h}^0\right)}{2}} p=v, p^{\prime }=h or p=h and p^{\prime }=v \end{array}\right.$$

(2)

where Q is the cross-polarization factor. As with most radiative transfer models, MEMLS requires the specification of snow–ground reflectivity as a lower boundary condition, which is calculated using the soil reflectivity models described next.

b.

Soil reflectivity models

The soil reflectivity models are used to determine the snow–ground reflectivity based on multiple factors, including the dielectric constant of the soil, which is estimated using the Dobson model [28,29]. Because the frozen soil moisture content required by the Dobson model is difficult to measure and was not available from the SnowEx pits, we used the method of [30] to estimate it for constructing parameter priors. This prior, along with the priors of other parameters, is then used for Bayesian optimization [20,21].

The soil reflectivity models used in this study are Wang and Chaudhary model (1981), also referred to as QHN model [24], and Wëgmuller and Mätzler model (1999), hereafter referred to as WM99 [25]. The QHN model is a semi-empirical model that uses three parameters to quantify the impact of surface heterogeneity and anisotropy on the Fresnel coefficients at the snow–ground interface: roughness height (HR), a polarization mixing parameter (QR), and a parameter accounting for the angular dependency of the reflectivity (NR).

$$\begin{array}{c}{{\mathsf{\Gamma }}_{\mathrm{p}}=\left[\right(1-Q_R)\mathsf{\Gamma }}_{\mathrm{P}}^{Fresnel}+Q_R{\mathsf{\Gamma }}_{\mathrm{q}}^{Fresnel}]\mathrm{e}\mathrm{x}\mathrm{p}(-H_R{\cos }^{{\mathrm{N}}_{\mathrm{Rp}}}{\theta }_0)\\ H_R={\left({\displaystyle \frac{a_1\sigma }{a_2\sigma +a_3}}\right)}^6\end{array}$$

(3)

where p is the polarization (can be V or H), ${\mathsf{\Gamma }}_{\mathrm{H}}$ and ${\mathsf{\Gamma }}_{\mathrm{V}}$ are the effective the H-pol and V-pol reflectivity at the snow–ground interface, ${\mathsf{\Gamma }}_{\mathrm{V}}^{Fresnel}$ and ${\mathsf{\Gamma }}_{\mathrm{H}}^{Fresnel}$ are the V-pol and H-pol Fresnel, ${\theta }_0$ is the incidence angle, and a₁, a₂, a₃, Q_R, H_R, and N_R are parameters of the model.

WM99, based on Mo and Schmugge (1987) [26], first estimates the effective H-pol reflectivity using soil temperature, soil moisture, and soil roughness, and in a second step, the V-Pol reflectivity is estimated from the modeled H-Pol reflectivity:

$$\begin{array}{c}{\mathsf{\Gamma }}_{\mathrm{H}}= {\mathsf{\Gamma }}_{\mathrm{H}}^{Fresnel}\exp -A_0\left(k{\sigma }^{A_1}\right)\\ A_1=A_2{\cos }^{A_3}{\theta }_0\\ {\mathsf{\Gamma }}_{\mathrm{V}}= {\mathsf{\Gamma }}_H{\left(cos{\theta }_0\right)}^{\beta }\end{array}$$

(4)

where $A_o, { A}_1, { A}_2, { A}_3, \beta$ are the parameters, $k$ is the wavenumber, $\sigma$ is the ground roughness, while other variables follow the notation described for Equation (3).

The fundamental formulations of the QHN and WM soil models are similar, with both describing soil reflectivity for realistic ground conditions as an attenuation of the Fresnel reflectivity that depends on the incidence angle and surface roughness. However, the QHN model introduces a cross-polarization mixing parameter that represents physically meaningful polarization coupling arising from surface roughness and subsurface heterogeneity. This formulation allows for QHN to explicitly account for polarization mixing when estimating both VV and HH snow–ground reflectivity. The calculations in these models as described in Equations (3) and 4 include constant parameter values that are critical for the ground reflectivity calculations. Montpetit et al. (2015) [37] tested these models against laboratory experiments for different frequencies and provided a set of parameters that best fit the equations for different frequencies and also a set of frequency-independent parameters (

Table 3. Values of parameters for the soil dielectric models—WM99 and QHN—as proposed by [37] for frequency-independent (fi) and X-band (10.65 GHz).

Wëgmuller and Mätzler (1999)—WM99
f (GHz)		A0			A2		A3		β		Bias			Std
WM99fi (All)		0.039			0.872		−0.016		2.140		−0.002			0.058
10.65		0.080			0.935		0.302		1.890		−0.012			0.052
Wang and Chaudhary (1981)—QHN
f (GHz)	a1		a2	a3		Q		NV		NH		Bias	Std
QHNfi (All)	0.887		0.796	3.517		0.075		1.503		0.131		−0.003	0.042
10.65	0.880		0.838	3.280		0.657		3.209		0.178		0.012	0.047

). They found out that the calibrated WM99 and QHN models yielded similar RMSE, and thus QHN is recommended due to fewer parameters to calibrate. We used the X-band and the frequency-independent parameters of both models to compare them and choose the best-suited model for this study.

c.

Bayesian estimation of soil parameters

In a Bayesian retrieval framework, the probability of a geophysical variable x (the posterior distribution) is determined based on prior knowledge of x (the prior distribution), indirect measurements D, and a physical model M(η)— in this case, a snow radiative transfer algorithm—characterized by physical parameters η and statistical error parameters ζ. Given a prior of the parameters P(n) and the likelihood of the observations P(y|n), the posterior probability of the parameters is given by

$$P \left(\mathsf{\eta }|y\right)\propto P\left(y|\mathsf{\eta }\right)\times P\left(\mathsf{\eta }\right)$$

(5)

In the context of Bayesian inference, the goal is to characterize P(η|y), the posterior probability of physical parameters conditional on measurements informed by the a priori parameter probabilities P(η), which is derived in detail in [38]. This implies maximizing the second term in Equation (5), the posterior of the backscatter conditional on physical parameters η, which is achieved by evaluating how well model simulations, M(η), match the observations y, weighted by the prior knowledge P(η). Building on a Bayesian SWE retrieval framework developed for passive microwave data (Pan et al., 2017 [38]), Ref. [21] adapted the approach to active microwave observations. In this approach, snow backscatter is forward-modeled using MEMLS, and unknown geophysical parameters (η) are inferred via Markov Chain Monte Carlo (MCMC) sampling (Metropolis et al., 1953 [39]). The sampler explores the posterior (P(η|y)) by proposing parameter updates and accepting them according to likelihood ratios derived from the mismatch between simulated and observed backscatter, iterating until convergence. The information about prior distributions and MCMC details for this study are presented in Table S1. Also, the parameters in the prior distribution were assumed to be independent, since insufficient data were available to reliably characterize correlations among them.

2.4. Quantification of Error

When using a Bayesian retrieval framework, quantifying the uncertainties is a crucial diagnostic step and the primary reason for adopting a probabilistic approach. Unlike deterministic inversion methods that provide single “best-fit” values, Bayesian inference produces full posterior distributions of parameters and simulated backscatter, thereby allowing for us to assess the robustness of the retrieval. In this study, where parameters such as surface roughness, volumetric soil moisture, and STRR are difficult to measure directly and often vary across scales, rigorous error quantification is essential. Posterior distributions provide insights into both the central tendency of parameter estimates and their spread. Such analysis not only improves confidence in the optimized values but also provides insights into how readily these parameter ranges generalize to other snow-covered regions.

Based on the specified priors and calculated likelihoods during the optimization of observed ground backscatter, the Bayesian framework generates approximately 18,000 posterior samples for each measurement (after discarding burn-in iterations). These samples represent sets of model parameters and the corresponding backscatter estimates, forming the posterior distribution. To quantify error ranges and potential bias in parameter estimation and backscatter calculations, we compute summary statistics including the posterior mean, median, standard deviation, and the 95% highest density interval (HDI).

To assess the reliability of the MCMC sampling, we calculate the Monte Carlo Standard Error (MCSE) and compare it with the posterior standard deviation. For well-converged chains, the MCSE should be substantially smaller than the standard deviation, ensuring that sampling variability does not dominate the posterior uncertainty. Additionally, we compute the split R-hat (Gelman–Rubin statistic), where values close to 1 indicate good mixing and convergence of the chains across independent runs. Together, these diagnostics confirm that the posterior samples provide a robust representation of parameter uncertainties, enabling reliable inference of snow–ground backscatter and associated model parameters.

3. Results

3.1. Soil Reflectivity Model

We evaluated backscatter using four soil reflectivity configurations derived from the WM99 and QHN models, each with frequency-independent (fi) and frequency-dependent (X) parameters (Table 3). Among these, the QHN-fi configuration produced the lowest snow–ground reflectivity and consequently the lowest simulated backscatter, followed by WM-X, WM-fi, and QHN-X (Figure A5). The reflectivity given by WM-X and WM-fi are very close, and even the QHN-X reflectivity is close to both.

Figure 4a shows the bias in calculated backscatter averaged for the range of roughness values for each observation. In the preliminary calculations of this study, we can see that we are overestimating for many pits, i.e., there are more pits with positive bias than negative. Since QHN-fi results in lower backscatter as compared to the other three models, and thus smaller bias, it emerges as the best-suited model from parameterizing soil dielectric properties for this study. QHN requires fewer parameters to calibrate [37], and using frequency-independent parameters ensures that the uncertainties associated with the model parameters can be easily utilized in other studies involving multifrequency SAR. Thus, QHN-fi is used for further analysis, which is also consistent with [21], who used it with the Dobson model for calculating soil permittivity.

Using the backscatter from QHN-fi as the target variable, we calculated RMSE backscatter over a range of surface roughness values averaged for each pit. Figure 4b shows that the choice of soil model holds RMSE around 1 dB in the final calculation. Note that if in situ measurements are available, then using QHN-fi as target is not necessary, and the suitability of QHN-fi itself can be assessed.

3.2. SnowSAR Bias Sources—Surficial Melt

Assuming the snowpack to be dry, the model was initialized with zero liquid water content (LWC). However, since the SnowSAR observations are taken in the early afternoon, solar radiation can drive some surficial melting in the snowpack, which can substantially modify the dielectric properties of the top layer of the snowpack [40,41]. Ref. [11] studied the effect of LWC in the snowpack using passive microwave remote sensing and showed that even small increases in LWC elevate surface reflectivity and alter emissivity. Apart from that, consistent positive biases in Ku-VV (≈5–6 dB across pits) pointed to inadequate representation of near-surface dielectric properties and microphysics, given Ku’s shallower penetration depth and stronger sensitivity to the uppermost layers. To test this hypothesis, the backscatter sensitivity to liquid water content at the top of the snowpack was examined by specifying LWC values in the 0.01–0.06% range in the top 1 cm of the pit snowpacks to emulate surficial melt at mid-day.

Figure 5 shows that the backscatter decreases with increasing LWC, and the magnitude of decrease in the backscatter varied among different pits depending on the microstructure. Volume backscatter from pits with higher correlation length (coarser grains) was less affected by the LWC, while there was a significant decrease in the backscatter with very low correlation length. Moreover, sensitivity to LWC is larger for the Ku-band compared to the X-band. The X-band backscatter in some pits was not impacted by small amounts of surficial melting up to a certain threshold value, while at the Ku-band the backscatter decreases monotonically with LWC. This contrast is consistent with band-dependent scattering mechanisms, with the X-band retaining comparatively greater volume-scattering contributions and Ku-band being more dominated by near-surface/surface scattering.

To reconcile model and observations, we applied a surficial LWC of 0.0001 to the top 1 cm for all 2017 pits. This successfully corrected the Ku-VV bias while maintaining accurate X-band simulations, accounting for mid-day melt process not captured in the snow pit data.

3.3. Sensitivity Analysis of Ground Parameters

MEMLS with the QHN-fi to estimate the reflectivity at the snow–ground interface was used to estimate the backscatter for both X- and Ku-bands, for each co-located snow pit in 2017 and 2020 (Table 2, Figure 2). For sensitivity analysis, the surface roughness was classified into smooth (0 cm), medium (0.9 cm) and rough (1.2 cm) as in [42]. An example showing the transmissivity, reflectivity and interface reflectivity for each snow pit layer estimated using the MEMLS model and the corresponding attenuation for the snowpack can be seen in Figure S10. The attenuation in the Ku-band is very high as compared to the X-band, consistent with lower penetration depths in the Ku-band as compared to the X-band as expected. Due to the low penetration depth, Ku-band backscatter exhibits negligible to very weak sensitivity to ground parameters (Figure 6) and thus it cannot be used in the stepwise Bayesian retrieval to infer snow–ground properties. In contrast, there is a clear dependence of total backscatter on ground properties at the X-band, underscoring the need to characterize these parameters robustly. Specifically, increasing ground surface roughness reduced the simulated backscatter by ~1.5 dB across the tested range, and increasing the STRR produced an additional ~1.0 dB decrease (Figure 7, Figure 8 and Figure 9). The estimated backscatter varied for different pits depending on snowpack stratigraphy. Across sites, simulated backscatter overestimated observations for some pits and underestimated them for most, indicating uncertainty in either the soil moisture prior or the snowpack characterization using the pit observations. Significant variations in measured backscatter for some pits between near-simultaneous acquisitions suggest other variability sources, including (i) line-of-sight perturbations from nearby vegetation or other land cover (e.g., partial canopy intrusion), (ii) sub-pixel heterogeneity, and (iii) uncertainty in the in situ snow pit data (disturbance, representativeness, or measurement error), among other factors discussed in this study.

Assuming an instrument error of 0.5 dB for SAR data as in [20], we defined acceptable ground parameter intervals as those for which the simulated total backscatter lay within ±0.5 dB of the co-located SAR measurement (visualized using Figures S1–S3). These intervals were then used as priors in the retrieval algorithm. The volume backscatter of the in-situ snowpack was estimated through forward simulations using MEMLS and subtracted from the total observed backscatter to obtain the “measured” ground backscatter estimate that was used as an observation in the Bayesian optimization algorithm. Observations for which the forward simulation of volume backscatter was greater than the total observed backscatter were eliminated from the study, indicating an error in the observed SAR pixel. This constraint led to the exclusion of five observations out of the total 20 observations from 2020 and two observations out of 25 observations from 2017. For the Ku-band, the simulated volume backscatter for all the pits was very close to or greater than the observed total backscatter indicating very low to no contribution of ground backscatter. Moreover, since we had dual-polarization HH and VV for 2017 SNOWSAR flights and VV for 2020 SWESARR flights, optimization was conducted for both single-pol VV as well as dual-pol VV and HH to compare the results.

3.4. Bayesian Parameter Estimation

3.4.1. Dual Polarization

SnowSAR from 2017 had VV and HH polarization acquisitions for the X-band; hence, the co-located pits from 2017 were used for dual-polarization optimization. The BASE-AM optimization yielded posterior distribution of the parameters and the estimated backscatter that are synthesized in Figure 10. The split Gelman Rubin statistic (R-hat) for these samples was around 1, indicating convergence in the chains (

Table A1. Monte Carlo Standard Error (MCSE) and split Gelman–Rubic statistic (R-Hat) for each parameter for the MCMC simulations with VV backscatter as observation.

Pit	Angle	Soil Moisture (MCSE)	Soil Moisture (Rhat)	STRR (MCSE)	STRR (Rhat)	Surface Roughness (MCSE)	Surface Roughness (Rhat)	VV Backscatter (MCSE)	VV Backscatter (Rhat)
B1	40.25	6.00 × 10−5	1.00026	0.00235	1.01104	0.00012	1.00173	0.01006	1.00305
B1	42.45	0.00033	1.00179	0.00266	1.00625	0.00013	1.00181	0.007	1.00438
B1	42.75	0.00029	1.00009	0.00229	1.00449	8.00 × 10−5	1.0014	0.00736	1.00132
B1	44.5	0.00041	1.00547	0.00302	1.01021	0.00017	1.00154	0.00751	1.00003
B2	39.95	0.00042	1.00152	0.00301	1.00886	0.00018	0.99995	0.00767	1.00044
B2	43.75	9.00 × 10−5	0.99998	0.0019	1.00956	5.00 × 10−5	0.99995	0.0096	1.00591
B2	45.05	0.00035	0.99995	0.0025	1.00624	9.00 × 10−5	1.00022	0.00647	1.00217
A1	32	0	1.00004	0.00187	1.00702	1.00 × 10−5	1.00007	0.01	1.00696
A1	54	3.00 × 10−5	1.00012	0.00195	1.00801	4.00 × 10−5	0.99995	0.01247	1.00698
B3	42.05	0.00046	1.00512	0.00321	1.01218	0.00018	1.00017	0.00824	0.99995
B3	42.65	4.00 × 10−5	0.99998	0.00192	1.00801	4.00 × 10−5	0.99997	0.01174	1.00631
B3	44.45	0.00038	1.00121	0.00263	1.00872	0.00016	0.99997	0.00644	1.00059
B4	43.75	9.00 × 10−5	0.99998	0.0019	1.00956	5.00 × 10−5	0.99995	0.0096	1.00591
B4	46.8	2.00 × 10−5	1.00013	0.00189	1.01086	3.00 × 10−5	0.99999	0.01206	1.00957
B4	47.95	0.00033	0.99998	0.00268	1.0085	0.00016	1.00153	0.00628	1.00186
B5	41.9	0.00031	0.99995	0.00243	1.00282	8.00 × 10−5	1.00027	0.0065	1.00094
A13	44	0.00057	1.00167	0.00327	1.01397	0.00016	1.00024	0.00857	1.00036
A13	51	0.00033	1.00039	0.00281	1.01232	0.00015	1.00079	0.00643	1.00073
A5	42	0.00033	1.00029	0.00233	1.01348	0.00011	1.0009	0.00746	1.00178
A5	49	0.00034	1.00003	0.00254	1.01057	9.00 × 10−5	1.00092	0.00673	1.00169
A16	42	0.00034	1.00004	0.0025	1.00345	8.00 × 10−5	1.00016	0.00642	1.00052
A16	49	6.00 × 10−5	0.99995	0.00192	1.00722	5.00 × 10−5	0.99995	0.01122	1.0048
A12	43	0.00034	1.00002	0.00266	1.00781	0.00016	1.00179	0.0063	1.00119
A12	49	0.00017	0.99999	0.00214	1.00868	6.00 × 10−5	1.00042	0.00819	1.00242
A11	41	0.00033	1.00011	0.0026	1.01033	0.00011	1.00046	0.00698	1.00194
A11	49	6.00 × 10−5	0.99995	0.00192	1.00722	5.00 × 10−5	0.99995	0.01122	1.0048
A14	42	0.00033	1.00029	0.00233	1.01348	0.00011	1.0009	0.00746	1.00178
A14	49	0.00017	0.99999	0.00214	1.00868	6.00 × 10−5	1.00042	0.00819	1.00242
A6	37	0.00016	1.00001	0.00215	1.0094	6.00 × 10−5	1.00032	0.00868	1.00343
A6	48	0.00033	1.00085	0.00272	1.00078	0.00015	1.00061	0.00641	1.00117
A7	37	8.00 × 10−5	1.00075	0.0024	1.00759	0.00011	1.00056	0.00969	1.00168
A8	37	0.00016	1.00001	0.00215	1.0094	6.00 × 10−5	1.00032	0.00868	1.00343
A8	48	0.00035	0.99996	0.00265	1.00425	0.00016	1.00015	0.0065	1.00074
A9	37	0.00016	1.00001	0.00215	1.0094	6.00 × 10−5	1.00032	0.00868	1.00343
A9	48	0.00024	1.0001	0.00229	1.00639	7.00 × 10−5	1.00013	0.00748	1.00165
A10	37	0.00016	1.00001	0.00215	1.0094	6.00 × 10−5	1.00032	0.00868	1.00343
A10	48	0.00024	1.0001	0.00229	1.00639	7.00 × 10−5	1.00013	0.00748	1.00165
A15	37	0.00016	1.00001	0.00215	1.0094	6.00 × 10−5	1.00032	0.00868	1.00343
A15	48	3.00 × 10−5	1.00019	0.00185	1.00859	4.00 × 10−5	0.99996	0.01184	1.00769

). Examples of the posterior distribution histogram for each parameter are shown in Figure S7.

The surface roughness varied from smooth (0 cm) to medium (0.9 cm) as classified by [42]. STRR showed the most consistent behavior across all the pits with low variance, a bell-shaped histogram, and a mean of around 65–70%. Soil moisture was the most dominant ground parameter controlling the simulated total backscatter. The soil moisture prior is characterized by high uncertainty. Mechanistically, soil moisture modulates the real part of the soil permittivity (ε) and losses. The retrieved permittivity for most of the pits was between 3.3 to 4, consistent with slightly moist frozen soil, except for some anomalies where the retrieval bias was relatively high in the backscatter. The estimated soil moisture content for some pits (A11, A14, A15, A16) was exceptionally high (~0.095), corresponding to a permittivity of around 4, and for others was low as 0.025 for A7. Analysis of the posterior distribution of backscatter revealed that VV backscatter is in better agreement with the observations than the HH backscatter. Apart from some pits, both VV and HH backscatter posterior mean values are very close to the observed backscatter. The contribution of ground backscatter at the X-band is higher for HH than VV polarization. The average bias in the VV backscatter was less than 1 dB for almost all the observations; however, five observations showed bias greater than 1 dB, which were analyzed to understand the various sources that can affect the analysis of the snow–ground system using remotely sensed satellite data.

When we separate the observations with bias less than 1 dB, the STRR posterior spans 0.60–0.72 with a mean ≈0.65. This narrow dispersion aligns with prior studies that treat STRR as approximately constant (≈0.65–0.70). The sensitivity analysis shows that varying STRR from 0.60 to 0.70 changes the simulated backscatter by only ~0.25 dB, which is well below the adopted SAR radiometric uncertainty (±0.5 dB). Accordingly, fixing STRR = 0.65 is justified and simplifies the inversion without materially affecting fit quality.

3.4.2. Single Polarization

In addition to the snow pits in the previous analysis, the pits and observations from 2020 were also used to optimize the single-polarization VV backscatter (Figure 11). The pits from 2020 showed similar results for STRR, most of them being in the range of 60–75%, supporting the conclusion that STRR can be held constant around 0.65. Most of the pits had relatively higher soil moisture content, resulting in soil permittivity closer to 4, while a few were relatively drier with soil permittivity around 3.5. The surface roughness for 2020 pits was medium to rough, contrasting with smooth values in 2017. For problematic pits (A6, A7, A13) where dual-polarization observations were inconsistent, the single-polarization (VV) inversion reduced bias by 1–2 dB. The adjustment came primarily from surface roughness and STRR, while soil moisture remained stable—a physically plausible result given the soil temperature is very low; the soil is frozen and therefore soil dielectric properties should not change.

For locations where and when the retrievals exhibit large bias, the single-polarization case is more robust because it avoids the “ambiguity” of conflicting HH/VV signals. The results with all the observations can be seen in Figure S8. We then investigated every pit with high bias and examined potential reasons for the error that can be found in the discussion section.

3.5. Uncertainty Quantification

In this study, we report the mean, median, standard deviation, 95% highest density interval (HDI) of the posterior MCMC chain of each parameter, and the corresponding backscatter. Moreover, we investigated the Monte Carlo Standard Error (MCSE), which is very low (<<standard deviation), indicating that it can be ignored (Table A1). The mean and median of STRR were very close, while the posteriors of surface roughness and soil moisture were skewed (Figure S7). Across both single- and dual-polarization inversions, the posterior for STRR was highly consistent, with a mean of ~65% and a small standard deviation (4–5%) (

Table 4. Mean, median, 95% HDI, and SD in the posterior distribution of each observation for STRR.

Pit	Angle (θ0)	STRR Mean (%)	Median (%)	HDI_L (%)	HDI_U (%)	SD (%)
B1	42.45	68.81	68.84	59.85	77.77	4.53
B1	42.75	65.8	65.86	56.93	74.49	4.45
B1	44.5	72.97	72.98	63.54	82.8	4.89
B2	43.75	62.59	62.6	55.03	70.59	3.96
B2	45.05	66.29	66.34	57.46	75.14	4.47
B3	42.05	73.32	73.34	63.36	83.12	5.06
B3	42.65	59.81	59.81	52.11	67.46	3.93
B3	44.45	70.87	70.91	61.63	80.04	4.64
B4	43.75	62.59	62.6	55.03	70.59	3.96
B4	46.8	55.7	55.65	48.53	63.57	3.82
B4	47.95	70.9	70.93	61.67	80.09	4.65
B5	41.9	65.93	65.97	57.27	75.11	4.47
A13	44	73.29	73.29	63.38	83.2	5.04
A13	51	71.09	71.14	61.53	80.49	4.75
A5	42	67.41	67.43	58.86	76.09	4.41
A5	49	66.29	66.3	57.61	75.56	4.55
A16	42	65.96	65.97	56.86	74.61	4.49
A16	49	61.17	61.16	53.38	68.72	3.92
A12	43	70.09	70.1	60.74	79.32	4.61
A12	49	64.48	64.55	56.18	72.54	4.16
A11	41	67.71	67.67	58.87	76.52	4.51
A11	49	61.17	61.16	53.38	68.72	3.92
A14	42	67.41	67.43	58.86	76.09	4.41
A14	49	64.48	64.55	56.18	72.54	4.16
A6	37	64.08	64.17	55.74	72.31	4.18
A6	48	72.19	72.23	62.82	81.42	4.7
A7	37	76.66	76.67	68.09	85.42	4.4
A8	37	64.08	64.17	55.74	72.31	4.18
A8	48	71.14	71.28	61.7	79.89	4.64
A9	37	64.08	64.17	55.74	72.31	4.18
A9	48	65.07	65.13	56.65	73.84	4.37
A10	37	64.08	64.17	55.74	72.31	4.18
A10	48	65.07	65.13	56.65	73.84	4.37
A15	37	64.08	64.17	55.74	72.31	4.18
A15	48	58.37	58.34	50.99	66.13	3.86

). The resulting backscatter uncertainty (~0.125 dB) is well below the instrument uncertainty, strongly supporting the use of a fixed STRR value of 0.65 as a robust model simplification to reduce the number of free parameters.

For surface roughness, the standard deviation of the posterior distribution was high as can be seen in

Table 5. Mean, median, 95% HDI, and SD in the posterior distribution of each observation for surface roughness (SR).

Pit	Angle (θ0)	SR_Mean (cm)	Median (cm)	HDI_L (cm)	HDI_U (cm)	SD (cm)
B1	42.45	0.69	0.72	0	1.54	0.52
B1	42.75	0.39	0.32	0	1.13	0.41
B1	44.5	1.38	1.42	0	2.18	0.53
B2	43.75	0.23	0	0	0.8	0.3
B2	45.05	0.45	0.41	0	1.23	0.44
B3	42.05	1.36	1.4	0	2.19	0.55
B3	42.65	0.17	0	0	0.68	0.25
B3	44.45	1.06	1.13	0	1.88	0.54
B4	43.75	0.23	0	0	0.8	0.3
B4	46.8	0.12	0	0	0.56	0.2
B4	47.95	1.07	1.12	0	1.9	0.56
B5	41.9	0.4	0.34	0	1.13	0.41
A13	44	1.38	1.43	0	2.19	0.53
A13	51	1.06	1.13	0	1.87	0.55
A5	42	0.52	0.52	0	1.3	0.47
A5	49	0.45	0.41	0	1.23	0.44
A16	42	0.4	0.33	0	1.13	0.41
A16	49	0.21	0	0	0.77	0.28
A12	43	0.9	0.96	0	1.73	0.55
A12	49	0.32	0.19	0	1	0.37
A11	41	0.55	0.56	0	1.35	0.48
A11	49	0.21	0	0	0.77	0.28
A14	42	0.52	0.52	0	1.3	0.47
A14	49	0.32	0.19	0	1	0.37
A6	37	0.25	0	0	0.86	0.32
A6	48	1.23	1.26	0	2.02	0.52
A7	37	1.83	1.82	1.1	2.56	0.38
A8	37	0.25	0	0	0.86	0.32
A8	48	1.04	1.1	0	1.85	0.54
A9	37	0.25	0	0	0.86	0.32
A9	48	0.37	0.27	0	1.09	0.4
A10	37	0.25	0	0	0.86	0.32
A10	48	0.37	0.27	0	1.09	0.4
A15	37	0.25	0	0	0.86	0.32
A15	48	0.15	0	0	0.65	0.24

. However, the smaller the mean surface roughness, i.e., the smoother the surface, the lower is the standard deviation in the posterior distribution. The standard deviation was around 0.2 cm for a mean surface roughness of 0.25 cm, which can lead to an uncertainty of 0.15 dB, and the standard deviation went up to 0.55 cm for surface roughness greater than 1 cm, which can lead to an uncertainty of around 0.3 dB.

The prior of soil moisture was given a range from 0.01 to 0.095 m³/m³ assuming frozen soil conditions during the accumulation season, which resulted in a standard deviation of around 0.008 for most of the pits (

Table 6. Mean, median, 95% HDI, and SD in the posterior distribution of each observation for soil moisture content.

Pit	Angle (θ0)	Mv_Mean	Median	HDI_L	HDI_U	SD
B1	42.45	0.064	0.064	0.046	0.082	0.009
B1	42.75	0.084	0.084	0.069	0.095	0.009
B1	44.5	0.038	0.038	0.02	0.053	0.01
B2	43.75	0.093	0.095	0.081	0.095	0.005
B2	45.05	0.08	0.079	0.065	0.095	0.01
B3	42.05	0.031	0.031	0.02	0.048	0.01
B3	42.65	0.094	0.095	0.087	0.095	0.003
B3	44.45	0.054	0.053	0.037	0.072	0.009
B4	43.75	0.093	0.095	0.081	0.095	0.005
B4	46.8	0.095	0.095	0.093	0.095	0.001
B4	47.95	0.053	0.053	0.036	0.071	0.009
B5	41.9	0.082	0.081	0.066	0.095	0.01
A13	44	0.037	0.037	0.02	0.052	0.01
A13	51	0.052	0.052	0.036	0.069	0.008
A5	42	0.071	0.071	0.057	0.095	0.009
A5	49	0.081	0.08	0.066	0.095	0.01
A16	42	0.082	0.081	0.066	0.095	0.01
A16	49	0.094	0.095	0.086	0.095	0.003
A12	43	0.058	0.058	0.041	0.075	0.009
A12	49	0.09	0.095	0.075	0.095	0.007
A11	41	0.069	0.069	0.051	0.088	0.009
A11	49	0.094	0.095	0.086	0.095	0.003
A14	42	0.071	0.071	0.057	0.095	0.009
A14	49	0.09	0.095	0.075	0.095	0.007
A6	37	0.09	0.095	0.075	0.095	0.007
A6	48	0.045	0.045	0.03	0.064	0.009
A7	37	0.021	0.02	0.02	0.029	0.003
A8	37	0.09	0.095	0.075	0.095	0.007
A8	48	0.053	0.053	0.035	0.068	0.009
A9	37	0.09	0.095	0.075	0.095	0.007
A9	48	0.088	0.091	0.072	0.095	0.008
A10	37	0.09	0.095	0.075	0.095	0.007
A10	48	0.088	0.091	0.072	0.095	0.008
A15	37	0.09	0.095	0.075	0.095	0.007
A15	48	0.094	0.095	0.09	0.095	0.002

). This change of 0.008 in the soil moisture content can change the real part of the dielectric constant from 3 to 3.16, leading to a change in reflectivity from 0.047 to 0.051. Soil moisture was the most sensitive and least constrained parameter as it is difficult to obtain its in-situ value or estimate it (e.g., it is not part of the suite of measurements at the snow pits); hence, it is characterized with a less confident prior. Consequently, its posterior distribution should be interpreted not as a precise estimate of in-situ moisture, but as an effective, representative value of the dielectric properties of the ground that compensates for unmodeled physics and aggregate uncertainties within the snow–soil system to achieve the optimal total backscatter, which is elaborated on in the Discussion Section.

Figure 12 shows the uncertainty decomposition analysis, which quantifies the relative contributions of STRR and surface roughness variations to the total uncertainty in X-band ground backscatter (X-VV) as a function of moisture content for MCMC samples generated to optimize 200 X-VV synthetic observations. For each moisture content bin, we isolated the uncertainty attributable to each parameter by filtering the MCMC samples to hold one parameter constant (within ±20% of its standard deviation from mode) while allowing the other to vary, then computing the standard deviation of backscatter in the filtered subset. For very dry and very wet soil, the total uncertainty is controlled by STRR, while for most of the soil moisture values, the contribution of uncertainty due to surface roughness is higher. The overlap between regions reflects the correlation between STRR and surface roughness, where their combined effect is less than the sum of individual effects due to partial cancellation when parameters co-vary.

4. Discussion

This study presents a robust methodology for estimating the snow–ground reflectivity and the parameters involved; however, we assume a simple snow–ground system with no vegetation. Factors such as the forest cover and sub-grid-scale heterogeneities such as submerged vegetation and landform impact the observed SAR backscatter on the one hand, and measurement errors or insufficient sampling of the in-situ properties of the snowpack at the pits lead to uncertainty in the calculation of snowpack backscatter, as well as the model parameters. Consequently, pits with high bias were examined in detail to get a better understanding of the factors that should be taken care of while performing such a study at the pit scale.

There were cases where the sensitivity analysis revealed abnormally high bias (3–4 dB) for some observations (

Table 7. Mean, median, 95% HDI, SD, and bias in the posterior distribution of each observation for VV backscatter.

Pit	Angle (θ0)	VV_Mean	Median	HDI_L	HDI_U	SD	Bias	Obs_VV
B1	42.45	−16.11	−16.11	−16.97	−15.21	0.45	0.32	−16.42
B1	42.75	−14.49	−14.49	−15.35	−13.65	0.44	−0.35	−14.15
B1	44.5	−19.64	−19.64	−20.6	−18.71	0.49	1.17	−20.8
B2	43.75	−13.93	−13.9	−14.61	−13.27	0.35	−0.72	−13.21
B2	45.05	−15.41	−15.4	−16.28	−14.54	0.45	0.55	−15.95
B3	42.05	−19.63	−19.63	−20.58	−18.67	0.49	0.96	−20.59
B3	42.65	−13.35	−13.34	−13.93	−12.75	0.3	−0.84	−12.51
B3	44.45	−17.86	−17.86	−18.79	−16.98	0.46	0.71	−18.57
B4	43.75	−13.93	−13.9	−14.61	−13.27	0.35	−0.25	−13.68
B4	46.8	−14.05	−14.04	−14.59	−13.54	0.27	−1.98	−12.06
B4	47.95	−18.84	−18.84	−19.75	−17.93	0.46	0.27	−19.11
B5	41.9	−14.45	−14.44	−15.33	−13.61	0.44	−0.31	−14.14
A13	44	−19.62	−19.62	−20.6	−18.71	0.49	1.22	−20.84
A13	51	−19.83	−19.83	−20.74	−18.95	0.46	0.62	−20.45
A5	42	−15.28	−15.28	−16.14	−14.43	0.44	0.37	−15.65
A5	49	−16.42	−16.42	−17.29	−15.5	0.45	−0.09	−16.33
A16	42	−14.46	−14.45	−15.33	−13.59	0.44	0.31	−14.77
A16	49	−15.14	−15.13	−15.78	−14.55	0.32	−0.3	−14.85
A12	43	−16.95	−16.94	−17.86	−16.06	0.46	0.87	−17.82
A12	49	−15.66	−15.64	−16.47	−14.92	0.4	0.15	−15.81
A11	41	−15.22	−15.22	−16.08	−14.34	0.44	0.66	−15.88
A11	49	−15.14	−15.13	−15.78	−14.55	0.32	−0.7	−14.44
A14	42	−15.28	−15.28	−16.14	−14.43	0.44	−0.05	−15.23
A14	49	−15.66	−15.64	−16.47	−14.92	0.4	−0.63	−15.04
A6	37	−12.73	−12.71	−13.51	−12.01	0.39	0.22	−12.95
A6	48	−19.73	−19.72	−20.68	−18.82	0.47	0.65	−20.38
A7	37	−20.29	−20.3	−21.12	−19.42	0.43	0.84	−21.13
A8	37	−12.73	−12.71	−13.51	−12.01	0.39	−0.09	−12.64
A8	48	−18.84	−18.84	−19.74	−17.91	0.47	0.33	−19.18
A9	37	−12.73	−12.71	−13.51	−12.01	0.39	0.06	−12.79
A9	48	−15.58	−15.56	−16.39	−14.74	0.42	0.3	−15.87
A10	37	−12.73	−12.71	−13.51	−12.01	0.39	0.16	−12.89
A10	48	−15.58	−15.56	−16.39	−14.74	0.42	0.27	−15.84
A15	37	−12.73	−12.71	−13.51	−12.01	0.39	−0.08	−12.65
A15	48	−14.59	−14.58	−15.16	−14.04	0.29	−1.31	−13.28

). This was associated with an error in the observation, as SAR data from another flight on the same day had different backscatter for the same location. If the incidence angle is too low or too high, the presence of nearby trees might cause disturbances in the measured backscatter signal, hence hindering the data. Also, the pit data are available at point scale while the SAR data were aggregated to 30 m from 1 m, thus averaging pixels with forest cover or other types of heterogeneity. Pits A2, A3, and A4, being in the proximity of thick forest cover, showed such behavior. Additionally, there was high bias in some of the data points where the pit was located on the edge of the SAR flights such as the case for pit B1 with flight 012, and B2 with flight 005. One of the pits, A1, had very high observed total backscatter as compared to the estimate based on pit data. While analyzing the LULC map, the pit is located very close to a lake that might be a contributing factor, since we averaged the nearby pixels to get a 30 m resolution backscatter.

Some pits even had high bias after the Bayesian optimization, and their detailed analysis revealed some more factors that might be affecting the results. High bias in backscatter observations resulted in extreme soil moisture content estimates (A11, A14, A15, A16, B3, B4 with very high soil moisture and A7 with very low moisture content), and hence the corresponding dielectric constant. The sensitivity of LWC to backscatter for these pits revealed that the pits with excessive soil moisture content, that is, the pits with negative bias, are the pits where the backscatter was underestimated and did not need any representation of LWC in the snowpack (Figures S5 and S6). When a pit is dug for in-situ data collection, there might be small disturbances in the snowpack, leading to characterization errors in the snowpack profile. Pits with low extreme soil moisture corresponding to high bias are the pits that required LWC greater than 0.0001 and hence are compensating with low soil moisture content to reduce the backscatter. Also, presence of even a small layer of light-absorbing particles (LAPs) like dirt that is unreported in the snow pit data and not accounted for in the models can be a contributing factor for it. Therefore, excessive (unphysical) moisture values in the posterior distribution that are inconsistent with the frozen soil conditions generally expected during the accumulation under deep snow indicate that the model compensates for missed snowpack properties or other errors, such as measurement errors, rather than reflecting true ground conditions. Thus, the retrieved values should be interpreted as an “effective” dielectric proxy that accounts for snowpack complexity not explicitly captured by the model.

Subsurface heterogeneity near pit sites—submerged litter, debris, dense grass, and roots— can affect the dielectric constant of the frozen soil, altering backscatter and biasing retrievals. In our dataset, a single SAR snapshot limits our ability to separate these effects from snow/soil state. Also, even without precipitation, wind redistribution, sublimation and temperature-driven snow metamorphism can alter the snow microstructure. Owing to limited temporal sampling in the SAR data, however, we assume that the snowpack remains stable during non-precipitating periods and in the absence of warming events. Any residual misrepresentation of snowpack evolution is furthermore implicitly accounted for by the estimated model parameters. However, if there are repeated flight overpasses over a region as obtained from an operational satellite mission, then a time-series of observations is available that can be used to retrieve the boundary conditions before the accumulation season and improve the determinacy of the snowpack retrieval. In future field campaigns, characterization of soil and physical ground conditions at the pit locations should be considered to provide physical constraints to the boundary condition in the model.

This study demonstrates that the stepwise separation of backscatter at the snow–ground interface from the volume backscatter enables the estimation of realistic bottom boundary conditions to improve the retrieval of snow mass from volume backscatter proposed by [20]. The methodology is general and can be applied anywhere at any time. While it provides valuable insights into the physical parameters governing the snow–ground system, the specific parameters are inherently local to the region of study and different values should be expected elsewhere. Because our primary objective was to examine processes at the snow–ground interface, we employed a simplified system representation that excluded vegetation and forest cover as in [20]. A second limitation concerns scale and representativeness. The scale gap between in situ pits and SAR pixel resolution emerges as a primary constraint in the evaluation of retrievals. The SAR data at high resolution (1 m) have very high variance. This variance decreases with decreased resolution (Figure 13), which in turn increases the scale gap between the snow pit point-scale measurements and the SAR pixel-scale backscatter resulting in a loss of heterogeneity, handicapping representativeness.

5. Conclusions

Accurate estimates of snowpack using remote sensing, especially active microwave SAR, have various sources of uncertainty, like the quality of input forcing data, and the parameters and constants used in their empirical or semi-empirical equations of both the PBM and RTM. Here, we focused on understanding and quantifying the error in the boundary conditions of the RTM, i.e., in the estimation of snow–ground backscatter, which serves as a major source of uncertainty. This study used Ku-band VV polarization backscatter to estimate the LWC in the snowpack and X-band VV and HH backscatter to estimate the ground parameters affecting the snow–ground backscatter. Moreover, the QHN model with frequency-independent parameters from [37] was used with the Dobson model to calculate the snow–ground reflectivity. The sensitivity analysis of 2017 Ku-band measurements revealed the presence of surficial melting since the SAR measurements were taken in the early afternoon. Consequently, a LWC of 0.0001 was added to the top 1 cm of the snowpack. Due to shallow penetration, Ku-band is more sensitive to the uppermost layers and surface processes while the ground parameters do not affect the total backscatter. For the X-band, the contribution of ground backscatter is higher in HH than VV polarization.

The sources of uncertainty are many, from uncertainty in the snowpack profile, unreported data concerning the presence of dust, depth hoar, or surficial melting, to uncertainty in the SAR data due to subscale heterogeneity or interference from vegetation. The optimized parameters confirmed that the retrieval sensitivity to the specular-to-total reflectivity ratio (STRR) is minimized in the 0.6–0.7 range and it can be fixed at 0.65. Assuming STRR to be a constant value is also a valid assumption if the study knows the underlying uncertainty associated with it. Irrespective of the observed backscatter in the optimization, STRR did not vary much and was found in 60–70% in the feasible ranges of ground backscatter for the X-band. For very low values of ground backscatter, the surface roughness was around 1.2 cm (rough), and it was in the range of 0 cm (smooth) to 0.9 cm (medium) in the feasible range of backscatter. Soil moisture content, the parameter with the most impact on the estimated backscatter, takes a range of values from 2.5% (real part of permittivity = 2.6) if the ground backscatter is around −20 dB to 9.5% (real part of permittivity = 4.05) for ground backscatter around −15 dB. As discussed earlier, this parameter compensates for incomplete information or measurement errors at the snow pits, which in turn impact volume backscatter.

Overall, we demonstrated and independently validated a Bayesian methodology to constrain the critical snow–ground boundary condition in active microwave snow retrievals. By providing a principled way to estimate ground parameter uncertainties, this approach directly supports more efficient and accurate large-scale SWE and SD retrievals from SAR. This study also investigated the uncertainties associated with the parameters that depend upon the value of observed backscatter. Using both the VV and HH backscatter and only VV polarization for optimization provided good results with low bias. The pits with high bias were used to explore the factors affecting the accuracy of the forward simulation. Even when using the in-situ snowpack vertical profile, there are some uncertainties related to the characterization of snow layers (e.g., dry snow, surficial melt, depth hoars) that can contribute to the bias in the study. This approach’s key strength is its ability to compensate for imperfect snowpack information through parameter estimation, making it robust and practical for real-world applications where model and data uncertainties are unavoidable. Moreover, retrieval of SD and SWE from backscatter using data assimilation [43,44] requires the uncertainties associated with all the parameters, where the uncertainties of ground parameters can be obtained from this methodology.

Optimizing the parameters for 200 X-VV synthetic ground backscatter X-VV values with a fixed 65% STRR and 45 degrees incidence angle revealed that the bias emerges when the observation is too low or too high. Thus, if the SAR measurements display anomalous behavior (too high or too low), the parameters will reflect excessive moisture and surface roughness if we cannot simulate the snowpack accurately. For instance, depth hoar and iced snow will have a very bright observed SAR pixel, while wet snow and LAPs like dust in the snow layer will have relatively darker pixels. If these properties are not accounted for, the parameters attain extreme values to compensate for the lack of information.

Table 8. Contribution of the ground backscatter and response of the BASE-AM model for different snowpack classifications.

Type	Structure	Total Backscatter		Ground Backscatter Component		BASE-AM Observation
Fresh snow	Low density (<200 kg/m3), small grains, fluffy, homogeneous	Low	Weak volume scattering because grains are much smaller than the wavelength (Rayleigh regime).	High	Low density, tiny grains → weak volume; waves reach ground easily	Low observed SAR, overestimating volume, underestimating ground backscatter
Depth Hoar (Large Grains, Faceted Snow)	Coarse grains (1–3 mm), low density but with strong internal contrasts	High	X-band is very sensitive here because grain size approaches or exceeds the Rayleigh-to-Mie transition relative to wavelength. Stronger volume scattering than other dry types → higher backscatter.	Low	Penetration OK, but strong volume scattering from large grains masks ground	High observed SAR, underestimating volume, overestimating ground backscatter
Wet Snow (Moisture in Pores, LWC > ~0.5%)	Presence of liquid water between grains, even in small fractions	Very low	Strong absorption and attenuation → backscatter drop sharply. Surface scattering dominates, but the wet snowpack looks darker overall (−15 to −25 dB). Even a thin wet layer on top masks deeper scattering.	Very low	Liquid water strongly attenuates → ground largely invisible	Low observed SAR, overestimating volume, highly underestimating ground backscatter
Snow with Light Absorbing Particles (Dust, Soot, Organic Matter)	Like dry snow but with LAP inclusions	Low	LAPs change dielectric properties slightly and can increase absorption.	Low	LAPs raise absorption slightly → less penetration, hence less ground share	Low observed SAR, overestimating volume backscatter, underestimating ground backscatter
Icy or Crusted Snow	Ice lenses, melt-freeze crusts, hard refrozen surfaces	Very high	Very strong surface scattering at X-band (specular if smooth, diffuse if rough). Appears bright regardless of underlying snow.	Very low	Crust/ice lenses reflect at shallower depths → cut off penetration	Very high observed SAR, highly underestimating volume backscatter, highly overestimating ground backscatter

and Figure 14 summarize the response of the BASE-AM model towards various snowpack structure classifications.