Monitoring snow layers of the Antarctic ice-sheet using reflected signals: GNSS and the Sun as sources of opportunity E.Cardellach1, F. Fabra1, A. Rius1 S. Pettinato2, Giovanni Macelloni2 S. D'Addio3 1 Institut de Ciències de l'Espai (ICE/IEEC-CSIC), Spain 2 “Nello Carrara” Institute of Applied Physics (IFAC-CNR) 3 ESTEC/ESA Outline Background and introduction Experimental campaigns: GNSS-R: GPS-SIDS L-band radiometry: DOMEX GNSS-R: “Strange” features in the data Possible explanations and final hypothesis Model to validate hypothesis Results Sun Fringes: Availabe data sets Adaptation of the model (GNSS-R to radiometry) Preliminary results Summary & Conclusions Background & Introduction • Information on internal layer structures of the dry-snow zones is required to better estimate snow accumulation rates. In turn, the snow accumulation in ice sheet (Greenland and Antarctica) is a key factor for estimating Earth’s ice mass balance. • In the ice-sheets snow layering could also provide useful information for a better understanding of the past climate history • EO data, acquired by microwave sensors, together electromagnetic models, are useful for estimating snow accumulation because volume scattering is the dominant mechanism. Therefore the snow layering is one of the unknowns that limit the retrieval capability • Because of the high-penetration, it is possible to use low frequency microwave signal to infer information on ice sheet layering? Sources of Opportunity L band GNSS + R Radiometer + Sun ICE SHEET • How Deep L-Band Signals Penetrate into the Dry-Snow? • Can they be used to sense snow sub-structure? • Which physical infromation/parmeters can be extracted? Experimental Campaigns © CSA Within the framework (related to SMOS experimental campaigns at DOME-C Antarctica period. of ESA projects and GNSS-R) were conducted in 2009 -2010 •The site is view on a sub-daily frequency by polar-orbiting satellites, at a variety of incidence and azimuth angles. Dome C • Homogeneity of snow surface at the 100 km scale. • Small surface roughness relative to other ice sheets. • Low snow accumulation rate (around 3.7cm/yr). Concordia Station (Dome C): 75.125 S, 123.25 E - 3270 a.s.l • Clear sky, and extremely dry and stable atmosphere. • Well known topography and environmental condition Experimental Campaigns Both campaigns were conducted at the American Tower, observing a pristine snow area 45 m GPS-SIDS CAMPAIGN (2009): → GPS antenna (LHCP+RHCP) mounted on top of the American Tower, ~45 m altitude → Antenna pointing towards the horizon, NW direction → GPS –Receiver: GOLD-RTR, dedicated GNSS-R hardware receiver, L1, 10 parallel complex (I/Q) waveforms every millisecond, 64 lags each, ~15 m inter-lag spacing DOMEX CAMPAIGN L-band radiometer installed for SMOS calibration (2009-2011) Frequency : 1413 MHz Bandwidth: 27 MHz Sensitivity = 0.2 K (Ti =2 sec) Polarization: H and V HPBW: 20° 15 m L – band Antenna IR - Radiometer Complementary Snow measurements Summer Snow deposition: Grains shape and Size Classification(precipitati on, hoar,wind, etc.) Winter Snow layers: Temperature Hardness Density Grains shape and Size Dielectric Constant GNSS-R: data features LAG 22 GNSS-features: For specular surfaces • Specular reflections tend to generate waveforms with the shape of the signal modulation's auto-correlation function, with no further deformations (in opposition to diffuse scattering). LAG 37 • The signal modulation used in this experiment, has an autocorrelation • function shaped as a triangle. • The received waveforms do not show the expected triangle shape, but a series of distorted triangles, with added tails and secondary peaks. Same oscillation over four days no noise! GNSS-R: data features In order to interpret the data a new observable was defined : THE LAG-HOLOGRAM → A reference wave field (“direct” ray, no reflection) is used to reveal the spectra from the total received field, at each lag independently: Direct Ray Snow Surface -10 m -70 m Specular direction = 45° GNSS-R: data features → Lag-holograms show high temporal repeatability: 17-Dec. 19-Dec. 18-Dec. 20-Dec. GNSS-R: external multipath? Are the results due to multipath interferences ? → Planar horizontal reflecting surfaces: GNSS-R: external multipath? - Frequency of the first (less negative) stripe in the lag-holograms (dots) and theoretical frequency of the air-snow surface reflection interference (solid grey line): REFLECTORS ABOVE SNOW SURFACE Snow Surface REFLECTORS BELOW SNOW SURFACE Main contribution comes from reflector placed below snow surface but external reflector (i.e. building) are to far from the tower GNSS-R: external multipath? HYPOTHESIS: frequency fringes found in the data correspond to interferences between direct signals and reflections off the snow surface and sub-surface snow layers. GNSS-R: model Different components of the signal coming from the different layers Total signal Snow model Ice sheet is modeled as a multilayer media . Model inputs: -ground data collected at Concordia station 0-10 m • Temperature • Layer depth • Later density -theoretical models/measurements 10 – 700 m (density saturates at 250 m) For density and layering more realizations were performed (monte carlo approach). GNSS-R: model results Waveform LagHologram GNSS-R: model results Waveform Simulated Data Real Data Comparison with Real Data Example of comparison between real and simulated data Simulated Data Real Data Inc. angle = 45 ° GNSS-R: results → A set of layers presented reflectivity stripes consistently in most of the lagholograms: Depth (m) 10 70 130 240 → Reflections down to ~300 meter depth → Vertical resolution: 5-10 meter → Full inversion procedures (lagholograms to density profiles) were not yet successful DOMEX-2 data Observing Radiometer data (at fixed incidence angle) fringes appear in the data when sun is in front of the radiometer (specular reflection) Sun in the specular direction ! Because of layering the sun effect is observed as «fringes» in the signal. Since we observe at q = 42° (≈ Brewster angle) the effect is evident at H polarization Sun Fringes: data Interference fringes found when Sun's reflection azimuth/elevation within the radiometer's antenna pattern : → ~September-March summer season Very high temporal repeatability, slowly changing with Sun's coordinates Sun Fringes: model The model developed for dry-snow GNSS-R is adapted to radiometric emissivity with Sun internal reflections: - Cross-polar circular polarization → power of linear polarized reflections HH, VV - lag-structure → peak power solely - Radiometer's antenna pattern included Sun Fringes: data&model Comparison between data and model for strong Sun signals (Feb 16, and Oct 16, 2010): SUMMER PERIOD - DOTS: DATA, SOLID LINE: MODEL Horizontal Polarization February October Vertical Polarization February October Sun Fringes: data&model Comparison between data and model for vanishing Sun signals (March 16, and Sep 16, 2010): WINTER PERIOD - DOTS: DATA, SOLID LINE: MODEL Horizontal Polarization March Sept. Vertical Polarization March Sept. Sun Fringes: data&model → Data could be also represented in a different way : JAN-MAR Intensity is represented in an arbritary scale: Green = high sun reflection Purple = low sun reflection SEP-NOV If we assume homogeneous vertical profiles of snow density, horizontal parallel layers (elevation dependence solely) azimuthal symmetry is expected in the signal. → Sun's data polar plot slightly disagree → TILTED LAYERS? Sun Fringes: extract info → Very coarse adaptation of the model to tackle non-homogeneous density profiles, introducing layers' slopes along the azimuthal direction (and antenna pattern disabled to facilitate pattern recognition): COARSE TILTED MODEL → Need to refine slopes' model: RAY TRACER approach (work on going) Conclusions → GNSS and L-band Sun signals penetrate into Antarctic dry-snow, down to ~300 meter, and reflect off internal layers; → These reflections interfere between them, generating sets of fringes, detectable in the frequency domain; → The lag-holograms have been created to visualize the fringes, affecting different delay-lags of the GNSS-R waveforms. Their temporal repeatability is significantly high; → Reflections have been identified, consistently, from a set of depths; → The vertical resolution of the technique is 5-10 meter depth; → The Sun reflection fringes captured by a L-band radiometer are also qualitatively explained using the same hypothesis/model; → Discrepancy found in the global behavior, it seems to indicate that the vertical profiles are not homogeneous, possible internal tilted slopes. Checked with a coarse model. A ray-tracer model is being implemented to further validate this hypothesis. Thank you for your attention !
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