Introduction
Space- and airborne radar altimeters have proven to be one of the best tools for measuring surface elevation changes of large ice sheets over time (Reference Alley, Spencer and AnandakrishnanAlley and others, 2007; Reference Rignot, Box, Burgess and HannaRignot and others, 2008, Reference Rignot, Velicogna, Van den Broeke, Monaghan and Lenaerts2011; Reference Zwally and GiovinettoZwally and Giovinetto, 2011; Reference ShepherdShepherd and others, 2012). Over ice, elevation differences between two epochs yield the volume change, and after correction for density variations of the overlying firn the mass change between the two measurements can be derived.
Radar altimeters determine the range between the radar (on the air- or spacecraft) and the target (the Earth’s surface) by transmitting electromagnetic waves and recording the return power after some time delay. These waves may penetrate several meters into snow, firn and ice (Reference Arthern, Wingham and RidoutArthern and others, 2001; Reference Hawley, Morris, Cullen, Nixdorf, Shepherd and WinghamHawley and others, 2006; Reference HelmHelm and others, 2007; Reference Lacroix, Legrésy, Coleman, Dechambre and RémyLacroix and others, 2007). The degree of penetration and scattering depends on the physical properties of the material, which can vary both spatially and temporally and thus affect the received waveforms (Reference Scott, Mair, Nienow, Parry and MorrisScott and others, 2006a,Reference Scott, Nienow, Parry, Mair, Morris and Winghamb). Since radar altimeters have relatively large footprints, subsurface returns can be combined with the returns from surrounding surface topography. Thus it can be a challenge to pinpoint the surface elevation from the received waveforms (Reference Alley, Spencer and AnandakrishnanAlley and others, 2007; Reference Brenner, DiMarzio and ZwallyBrenner and others, 2007). The performance of radar altimeters is generally best in the interiors of the large ice sheets, where the surface is relatively flat and seasonal fluctuations in material properties small. Performance is reduced at the ice-sheet margins, as well as over small glaciers and ice caps characterized by steep surface slopes and large seasonal variations in material properties due to surface melting. The largest contribution to current sea-level rise, attributed to land ice melt, is from small ice caps and glaciers (Reference Lemke and SolomonLemke and others 2007; Reference MeierMeier and others 2007; Reference CogleyCogley, 2009; Reference ChurchChurch and others, 2011). Thus, there is an urgent need to improve the understanding of radar altimeter returns from ice caps and glaciers, and their seasonal variations, in order to successfully monitor these important changes. Additionally, observations from small ice caps and glaciers can improve our ability to detect changes in the ablation areas of the larger ice sheets.
While subsurface returns may raise challenges for surface retracking with radar altimeters, these waveforms provide a potential source from which subsurface information can be extracted. Reference Lacroix, Legrésy, Coleman, Dechambre and RémyLacroix and others (2007) used the European Space Agency’s (ESA) dual-frequency Envisat altimeter data to extract subsurface characteristics over the Amery Ice Shelf, Antarctica. Over the Greenland dry snow zone, Reference Hawley, Morris, Cullen, Nixdorf, Shepherd and WinghamHawley and others (2006) showed agreement between subsurface radar altimeter returns and annually resolved firn density fluctuations using ESA’s Airborne SAR/Interferometric Radar Altimeter System (ASIRAS). This system was also used by Reference HelmHelm and others (2007) to map the winter accumulation along a flight line in the percolation zone of the Greenland ice sheet.
Reference König, Wadham, Winther, Kohler and NuttallKönig and others (2002) showed that different glacier facies in Svalbard can, under certain circumstances, be classified using satellite synthetic aperture radar (SAR) imagery. Reference Hindberg, Malnes and HogdaHindberg and others (2012) studied the variability in glacier facies over the period 2002–12 using Envisat ASAR. Reference LangleyLangley and others (2007, Reference Langley2008), Brandt and others (2008) and Reference Dunse, Schuler, Hagen, Eiken, Brandt and HøgdaDunse and others (2009) compared ground-penetrating radar (GPR) and SAR backscatter to determine glacier facies. This correspondence between sounding-radar backscatter and facies gives rise to the potential of using ASIRAS backscatter to determine glacier facies.
In this study we apply methods similar to Reference HelmHelm and others (2007) to derive snow accumulation along several ASIRAS altimeter profiles crossing over Austfonna ice cap, Svalbard. The method involves tracking the last year’s summer surface (LSS), buried beneath winter snow accumulation, in the radar waveform data. We outline a robust retracking scheme that accounts for considerable variations in the retrieved waveforms from different glacier facies. Additionally, we attempt to use the characteristics of the subsurface returns to distinguish the long-term firn area from the other facies. Generally, the power of the LSS reflection is lower in the long-term firn area, as is the the abruptness of the LSS reflection, as we expect. Despite these general correlations, a quantitative classification of facies using ASIRAS remains elusive.
Field Site: Austfonna
Austfonna ice cap (8120 km2; 79.7° N, 24.0° E) on Svalbard (Fig. 1, inset) has been the focus of several studies starting as early as 1873 and summarized by Reference TaurisanoTaurisano and others (2007). The ice cap reaches a maximum elevation of 800 m a.s.l., with one dome supplying a number of drainage basins. Several methods have been applied to determine the surface mass balance (Reference Pinglot, Hagen, Melvold, Eiken and VincentPinglot and others, 2001; Reference Schuler, Loe, Taurisano, Eiken, Hagen and KohlerSchuler and others, 2007; Reference TaurisanoTaurisano and others, 2007; Reference Dunse, Schuler, Hagen, Eiken, Brandt and HøgdaDunse and others, 2009), surface elevation changes (Reference Bamber, Krabill, Raper and DowdeswellBamber and others, 2004; Reference Moholdt, Hagen, Eiken and SchulerMoholdt and others, 2010) and dynamics (Reference Bevan, Luckman, Murray, Sykes and KohlerBevan and others, 2007; Reference Dowdeswell, Benham, Strozzi and HagenDowdeswell and others, 2008). Despite a recent surface mass balance close to zero (Reference Moholdt, Hagen, Eiken and SchulerMoholdt and others, 2010), the ice cap experiences net mass loss attributed to calving and retreat of the marine ice margin (Reference Dowdeswell, Benham, Strozzi and HagenDowdeswell and others, 2008). On Austfonna, melt and rain events can occur even during winter. In summer, surface temperatures typically remain above or around freezing (T.V. Schuler and others, unpublished information). This causes extensive melting, percolation and refreezing. The firn is therefore heterogeneous and characterized by ice lenses, glands, and layers ranging in thicknesses from millimeters to >0.5 m. Thus, in most years the facies in the accumulation area of Austfonna will consist of a wet snow zone and a superimposed ice zone as defined by Reference PatersonPaterson (1994).
Fig. 1. Winter snow depth as determined by airborne altimeter data (ASIRAS), acquired between 18 and 21 April 2007. Accumulation is generally higher on the east side of the ice cap and and lower to the west. Universal Transverse Mercator (UTM) coordinates in zone 33X. Ice-cap elevation is given in 100m contour intervals. Inset: location map of Austfonna, Svalbard.
Data and Methods
Airborne altimeter data
The airborne radar altimeter data were collected at the end of April 2007 using ESA’s ASIRAS system (Reference Hawley, Morris, Cullen, Nixdorf, Shepherd and WinghamHawley and others, 2006; Reference HelmHelm and others, 2007). The instrument was operated in a non-interferometric mode at a nominal altitude of ~700 m above the surface. The instrument is a frequency-modulated nadir-viewing SAR with a 13.5 GHz center frequency (Ku band) and 1 GHz bandwidth (Reference Lentz, Braun, Younis, Fischer, Wiesbeck and MavrocordatosLentz and others, 2002).
The raw radar data were post-processed using ESA’s ASIRAS L1b processor. The processor uses Doppler frequency shift to coherently focus the beam in the along-track direction, giving an effective footprint of ~5 m along track by ~50 m across track. Positioning of the radar traces comes from differential GPS (DGPS) and an inertial navigation system. The distance between each trace recorded by ASIRAS (after post-processing) depends on aircraft speed relative to the ground, but is typically 8–10 m.
We determined the electromagnetic wave velocity in snow down to the LSS using a ground-based stepped frequency Ku-band radar (Reference BrandtBrandt and others, 2008) and from density profiles derived in pits (see next subsection).
The electromagnetic wave speed v (m s−1) is related to the real part of the dielectric permittivity ∊r (dimensionless) and the speed of light in a vacuum c (~3 × 108 m s−1) by
The relative permittivity of snow and firn is related to density ρ (kg m−3) following (Reference Kovacs, Gow and MoreyKovacs and others, 1995)
During the measurements the winter snow temperature ranged from –5°C to –23°C, fulfilling the criteria of a dry snowpack for the empirical conversion using Eqn (2). Below the LSS the propagation velocity is more spatially variable depending on the glacier zone in which the measurement is made. Because the main focus of this study is on the winter snowpack and the shape and power of the LSS reflection, we have not made further velocity corrections below the LSS. The mean density of our 14 snow pits in 2007 was 390 kg m−3, with a standard deviation of 21 kg m−3. Our resulting wave speed velocity v is (2.25 × 108) ± (0.03 × 108) m s−1, and is uniform across our survey area.
The range resolution of the altimeter, determined by the bandwidth and wave velocity of the radar (Hamran and others, 1995), is ~0.15 and ~0.11 m in air and the winter snowpack respectively. Some of the profiles from the April 2007 campaign suffer from poor data quality, mainly due to rapid and high-amplitude aircraft movements (Reference HelmHelm and others, 2007), and have been discarded.
Ground-based data
To validate the ASIRAS measurements and interpretation, we use GPR data collected at a frequency of 800 MHz in spring 2007 (Reference Dunse, Schuler, Hagen, Eiken, Brandt and HøgdaDunse and others, 2009). The GPR profiles were located using DGPS measurements and are supplemented by physical snow properties measurements in snow pits (two to four in each profile). The two-way travel time of the radar wave was converted to depth using the method described above for ASIRAS, and validated using manual snow depth soundings. Lateral variations of the average density of the entire winter snowpack were found to be small, and the related uncertainty in depth determination of the LSS is on the order of ±15 cm, which is small compared to the effective resolution of the GPR, estimated by Reference Dunse, Schuler, Hagen, Eiken, Brandt and HøgdaDunse and others (2009) to be ~0.25 m. Reference Dunse, Schuler, Hagen, Eiken, Brandt and HøgdaDunse and others (2009) compared SAR backscatter with GPR-derived glacier facies and subclassified the firn area into three zones: a long-term firn area (F1); a firn layer that originates from multiple years of accumulation but lies in a zone of recent (~10 years) variability of the firn line (F2); and a thin firn layer that apparently originates from one accumulation season only (F3). Zones F2 and F3 are either underlain by superimposed ice (SI) or ice typical of the ablation zone. A series of GPR measurements from four consecutive spring seasons enabled delineation of a multi-year sequence of glacier facies distribution.
Satellite SAR data
The SAR image used in this study is a composite multi-look two-dimensional backscatter image from the Advanced Synthetic Aperture Radar (ASAR) on board ESA’s Envisat.
In total, 75 Envisat ASAR wide swath medium-resolution (150 m) images covering Austfonna for the winter season 2006/07 were used. The images were in both HH- and VV-polarization and covered all incidence angles from 17° to 42° (400 km swath). The difference between HH and VV was investigated, and found to be insignificant compared to the temporal variability.
These scenes were calibrated and georeferenced to result in a final multi-look image with 50m pixel spacing. Each image was corrected for incidence angle variability applying the Muhleman distribution (Reference MuhlemanMuhleman, 1964) and averaged to obtain a SAR image with improved radiometric properties on which the long-term firn area is easily identified by its higher backscatter. A variety of other incidence angle corrections were tested, including correction to the mean incidence angle of 30° using linear fitting to the data itself (Reference Sabel, Bartalis, Wagner, Doubkova and KleinSabel and others, 2012) and correction using the method by Reference UlanderUlander (1996). We found only small differences in the final averaged result, and the Muhleman distribution was preferred due to its simplicity.
Here we compare the ASIRAS-derived LSS abruptness (described below) and total power with SAR images from winter 2006/07 (the same year in which our ground- and air-based data were collected). This is in contrast to Reference Dunse, Schuler, Hagen, Eiken, Brandt and HøgdaDunse and others (2009) who used a longer time series of SAR images and GPR, relating GPR-derived glacier facies with SAR backscatter.
Methods
Surface and LSS retracking
We tracked the snow surface using a simple but robust threshold retracker. Since the maximum power of each trace varies depending on permittivity contrasts, surface orientation relative to the radar beam, and other factors, we use a relative threshold for each individual radar profile. We set our threshold to 20% of the mean peak amplitude over all traces in the profile. If the retracker fails, this manifests itself as a discontinuity in the surface. In case of discontinuities in tracking position (typically only a few percent of the points in each profile), a 10% threshold retracking point was used. Traces causing anomalous surface elevations for both thresholds and traces with anomalously low maximum power (<2 × threshold) were discarded. The roll angle of the aircraft can have a significant effect on the return waveform shape and can lead to retracking errors, so we excluded any data in which the aircraft roll exceeded ±1.5°. After surface retracking, we anchor the depth scale for the radar profile to zero at the retracked surface. To save computational time and memory, the data have been decimated by a factor of two; only every other trace is used and illustrated.
Retracking of the LSS is complicated by significant spatial variations in LSS reflection power over the study area. In contrast to Reference HelmHelm and others (2007), a single threshold algorithm failed to track the LSS reflection in a consistent way. Instead we used a local peak-finding algorithm in which only local peaks separated by a minimum depth distance are picked (set to seven range bins or ~0.75 m). By setting this distance large enough, the algorithm ignores smaller peaks (likely due to ice lenses and layers within the snowpack) that may occur close to larger local peaks. The peak position (in depth) is then compared to the surrounding traces both in number of peaks detected and position of the peaks to avoid the re-tracker ‘jumping’ between the LSS reflection and another peak adjacent in depth.
Winter snow depth comparison
We calculated the difference between winter snow depth as mapped with GPR (Reference Dunse, Schuler, Hagen, Eiken, Brandt and HøgdaDunse and others, 2009) and with the ASIRAS data. For each ASIRAS-derived snow depth position, we linearly interpolated and resampled the GPR-based snow depths to the same position along the track. The spatial offset between profiles is generally less than a few tens of meters, with some exceptions.
Power and abruptness index
To determine glacier facies, we calculated the maximum peak power and an abruptness index of the LSS reflection for each waveform. The peak power of the LSS reflection P peak(x) is computed by taking the average power of the three range bins surrounding the retracked LSS point. Since the received power from the LSS depends on the reflectivity (permittivity contrast) of the interface as well as the amount of power scattered above the interface and losses due to absorption, we normalized the LSS peak power to the total received power. To determine the abruptness of the LSS peak signal, following Reference Oswald and GogineniOswald and Gogineni (2008) we calculated an abruptness index of the LSS reflection as a proxy for the shape of the waveform. The abruptness index I abr(x) at position x along the track is taken as
where 
is the aggregate reflection power over the interval from two bins above the location of maximum power to ten bins below. Thus, a well-defined peak, appearing as a spike, will have a higher abruptness index than a peak with the same maximum power but surrounded by bins with similarly high power.
Results
Winter snow depth
The winter snow depth as retrieved by ASIRAS (Fig. 1) shows an asymmetric accumulation pattern across Austfonna, with increasing snow accumulation from northwest to southeast. Comparing the airborne retracked winter snow depth with the ground-based snow depth data from Reference Dunse, Schuler, Hagen, Eiken, Brandt and HøgdaDunse and others (2009) we find a mean offset of 0.008m (ground-based minus airborne) with a standard deviation of 0.154m over the total profile length (Fig. 2). Spatially, the two methods correspond closely over most of the ice cap (Fig. 3), except for three sites at lower elevations. The lower-accumulation and -ablation sites pose some challenges to the retracking algorithm. Here reflections from within the winter snowpack are strong relative to the LSS reflection, and reflectors become more closely spaced as the snow depth decreases, confounding the LSS retracking algorithm.
Fig. 2. Histogram of the difference between winter snow depth retrieved using the airborne ASIRAS altimeter instrument and the corresponding ground-based winter snow depth measurements from Reference Dunse, Schuler, Hagen, Eiken, Brandt and HøgdaDunse and others (2009). The distribution is normal, with a mean of 0.008 m and standard deviation of 0.154 m.
Fig. 3. Winter snow depth difference (m) between the ground-based (Reference Dunse, Schuler, Hagen, Eiken, Brandt and HøgdaDunse and others, 2009) and airborne altimeter data (ASIRAS). Three representative profiles are marked A–A′, B–B′ and C–C′, and are illustrated in Figure 5. Ice-cap elevation is given in 100m contour intervals.
Glacier facies
We find the abruptness of the LSS reflection to be lower in the long-term firn area than in other glacier facies (Fig. 4). The highest abruptness (most well-defined peak) is found where the winter snowpack overlies ice and within the area over which the firn line has been fluctuating over recent years (Reference Dunse, Schuler, Hagen, Eiken, Brandt and HøgdaDunse and others, 2009). In contrast, the total reflection power does not seem to show any clear relation to glacier facies or snow depth. Instead it is highly influenced by the power of the LSS reflection, internal backscatter within the winter snowpack, and the power of the surface/near-surface return.
Fig. 4. Airborne ASIRAS-tracked LSS abruptness (normalized color) overlaid on multi-looked satellite SAR image (normalized gray-scale). The long-term firn area corresponds to the high backscatter (white) in the SAR image. This area is characterized in the ASIRAS data by a lower LSS abruptness.
Discussion
Snow depth
The ASIRAS and snow thickness data agree to within 0.008 m, despite the fact that the measurements were done with different spatial offsets, on different days and with significantly different footprint size.
Notably, there are three areas illustrated in Figure 3 where the airborne radar processing fails to accurately retrieve winter snow depth. These three profiles (A–A′, B–B′ and C–C′ in Fig. 3) are shown in their entirety in Figure 5. The regions in question are 60–70 km along profile A–A′, 15– 20 km along profile B–B′ and 0–5 km along profile C–C′. In the first instance, the airborne retracker appears to successfully track the same layer, but the ground-based radar clearly recorded a different surface as the LSS. In the next two profiles, the snow is getting relatively thin. Since we identify peaks that are at least 0.75 m apart to track the LSS, as the snowpack thins we encounter the limitations of the method.
Fig. 5. Upper panels: The full length of the airborne altimeter profiles A–A′, B–B′ and C–C′ in Figure 3. Radar data have been masked (and eliminated from our analysis) where aircraft roll exceeded ±1.5°. These areas are evident as ‘dropouts’ in the radargram. Lower panels: Retracked LSS surface from the airborne radar in black, and corresponding LSS depth inferred from ground-based measurements (Reference Dunse, Schuler, Hagen, Eiken, Brandt and HøgdaDunse and others, 2009) in blue.
At a few locations within the long-term firn area, over distances shorter than 50 m, the LSS reflection is weak and the retracker tracks deeper reflectors. This is manifested in the LSS depth record as discontinuities in depth. In most cases, these sudden changes in depth can easily be filtered, but this would be a potential problem if larger areas with these types of waveforms were encountered.
Evident in Figure 5 is an internal reflecting layer within the winter snowpack, distinct from the surface and LSS return. This reflector may represent one or more events (e.g. storms) which caused a discontinuity in snow density, giving rise to a contrast in permittivity. In areas with snow depths shallower than ~1 m, strong internal reflection horizons within the winter snow are closely spaced with the reflection from the LSS, hampering unambiguous retracking of the LSS. We have not found a way to overcome this problem since we have limited ground-based data close to the margins to support testing of other methods (the presence of crevasses restricts safe access at several locations). Further work is therefore needed to evaluate the performance of ASIRAS at low-accumulation sites. These results therefore show that the methods outlined here cannot be applied to an area without direct ground-based verification. This emphasizes the need for independent ground-truth measurements in these types of regions.
The airborne data were collected over 3 days, while the ground-based data were recorded over a 2 week period during which redeposition of snow by wind drift and new snowfall was observed. This effect appears to be minimal, as we do not find a consistent pattern in snow depth differences along profiles recovered on different days. Over the eastern flank of Austfonna the field team observed significant and varied surface roughness, with sastrugi heights up to 40– 50 cm. In the airborne data we do not see any clear effect from this.
Facies
Reference LangleyLangley and others (2007, Reference Langley2008) and Reference Dunse, Schuler, Hagen, Eiken, Brandt and HøgdaDunse and others (2009) successfully determined glacier facies from ground-based radar surveys. Therefore it seemed worth seeing whether it would also be possible to determine facies from airborne radar. Because electromagnetic energy is reflected from surfaces with strong dielectric contrasts, and because density differences provide the strongest dielectric contrasts in the near-surface glacier regime, the stronger density contrast of snow on glacial ice should give a stronger response than the weaker contrast of snow over long-term firn. For this reason we investigated both the power of the LSS reflecting horizon and its abruptness. The high power of the LSS reflection between 60 and 80 km along the line B–B′ in Figure 5 is an example of what we might expect to see in the SI or ablation facies, and it is indeed the transition between this and the long-term firn area that we see in this region (Fig. 4). Though the power shows the kind of behavior we would expect in this instance, it is not consistent across the ice cap. For this reason we turn to a measure of the abruptness of the LSS peak.
In the SI and ablation facies of the ice cap, the LSS peak should be very abrupt, as most of the energy is reflected at the interface between winter snow and glacial ice. Further, dielectric contrasts below the snow ice contact do not yield reflections of comparable power. Thus it follows that abruptness of the LSS peak may serve as an indicator of facies. In determining facies from the abruptness of the LSS peak, we note in Figure 4 that there is a general correspondence between lower abruptness of the LSS peak and higher SAR backscatter, implying that the lower LSS abruptness can be used as an indicator for the firn area. However, in seeking a quantitative relationship between LSS abruptness and SAR backscatter, we do not find a compelling enough correlation to warrant classification of facies solely from ASIRAS radar waveforms.
Extension to spaceborne radar altimeters
The success with which ASIRAS penetrates winter snow and firn in the percolation zone (this work; Reference HelmHelm and others 2007) and in the dry-snow zone (Reference Hawley, Morris, Cullen, Nixdorf, Shepherd and WinghamHawley and others 2006) makes it attractive to extend similar analyses to spaceborne radar altimeters, such as that flown aboard ESA’s CryoSat-2. Such an application faces distinct challenges. The first of these challenges is that of range resolution: the resolution of CryoSat-2′s radar is ~47cm in air (Wingham and others 2005), and, though the range resolution in snow will be slightly finer, the entire thickess of the winter snow in our survey area would be represented by five to ten range bins, making many of the techniques we use for identifying the LSS impossible. In addition, the footprint size of a spaceborne radar altimeter is significantly larger, and contributions to the echo from off-nadir returns (surface clutter) are likely to be combined with subsurface returns, obscuring the LSS.
Conclusions
We have used airborne ASIRAS altimeter waveforms to map winter snow accumulation in the accumulation and upper ablation zone of Austfonna. The accumulation area is typically exposed to extensive summertime melt and is thus composed of a wet snow zone and a SI zone. We used a local peak-finding algorithm to retrack the LSS. This contrasts with the method of Reference HelmHelm and others (2007), which used a threshold retracker to follow the LSS horizon in a profile from Greenland’s percolation zone. In our case, a similar threshold retracking failed due to large spatial variations of the received power returns from the LSS over Austfonna.
The depth of LSS, as tracked in the ASIRAS data, agrees within ~0.008 m with ground-based measurements of snow thickness, the latter based on manual snow depth probing and GPR (Reference Dunse, Schuler, Hagen, Eiken, Brandt and HøgdaDunse and others, 2009). Snow depth retrieved by ASIRAS differs slightly from snow depth retrieved by GPR at lower-elevation and lower-accumulation sites. This emphasizes the need for independent ground-truth measurements to verify the airborne data in these regions. It also demonstrates the need for further investigations at low winter snow accumulation sites close to the equilibrium line and within the ablation zone. In spite of this need, ASIRAS can be a useful tool for measuring winter balance on glaciers and small ice caps such as Austfonna.
The LSS power (after normalization to the total received power) and its abruptness are both lower over the long-term firn area compared to the other encountered glacier facies. These differences can potentially be used to delineate the long-term firn area from the superimposed ice and ablation zone. Though we note a general correspondence between lower LSS abruptness and higher SAR backscatter, consistent with our predictions, the relationship between the two is clearly more complex and we do not find a distinct classification of glacier facies based on ASIRAS radar waveforms at Austfonna.
Acknowledgements
This work was supported by the European Space Agency (ESA) and the Norwegian Space Center as part of the CryoSat program and by the Norwegian Research Council through the International Polar Year (IPY) project GLACIODYN. This work was also funded in part by the German Ministry of Economics and Technology (grant 50EE1008). Envisat ASAR data were provided by ESA under IPY AO contract No. 4122. We thank the aircrews who flew the ASIRAS data flights for their work. We are especially grateful to Trond Eiken for carrying out the ground-based GPR and GPS work. The manuscript benefited greatly from the comments of Ginny Catania and Jo Jacka, Scientific Editors, and two anonymous reviewers.
