On the response of polarimetric synthetic aperture radar signatures at 24-cm wavelength to sea ice thickness in Arctic leads

We investigate observationally and theoretically the response of polarimetric backscattering at 24-cm wavelength to the thickness of Arctic sea ice in leads and first-year ice features. We employ backscattering data acquired by the Jet Propulsion Laboratory airborne synthetic aperture radar (SAR) during March 1988 in the Beaufort Sea, together with nearly simultaneous passive microwave imagery acquired by the U.S. Navy Ka band radiometric mapping system. We find that 24-cm copolar ratios and copolar phases vary strongly with apparent ice thickness. We observe copolar phase shifts between −10° and −50° (relative to multiyear ice phases) for new ice features in the imagery, as well as positive copolar phases in a first-year ice feature. Copolar ratios also vary with apparent thickness, from values larger than those expected theoretically for seawater to values slightly lower than those expected for thick ice. We derive a signature model based on scattering from a rough air/sea ice interface with realistic vertical profiles of brine volume and relative permittivity beneath. Model predictions for copolar ratios and phases show ice thickness-dependent variations consistent with those observed. We present simulation results showing that plausible ice thickness variations between pixels in a multilook average diminish, but do not eliminate, the signature response to thickness. This suggests that direct thickness estimation of sea ice in leads may be possible using polarimetric SAR at wavelengths of 24 cm or longer.

[1]  R G Onstott,et al.  Theoretical and Experimental Study of Radar Backscatter from Sea Ice , 1984 .

[2]  M. Drinkwater,et al.  Modelling changes in the dielectric and scattering properties of young snow-covered sea ice at GHz frequencies , 1988 .

[3]  Environmental Measurements in the Beaufort Sea, Spring 1991 , 1989 .

[4]  S. Rice Reflection of electromagnetic waves from slightly rough surfaces , 1951 .

[5]  E. Rignot,et al.  Characterization of spatial statistics of distributed targets in SAR data , 1993, International Journal of Remote Sensing.

[6]  W. F. Weeks,et al.  Numerical simulations of the profile properties of undeformed first‐year sea ice during the growth season , 1988 .

[7]  E. Carmack,et al.  On the halocline of the Arctic Ocean , 1981 .

[8]  L. Tsang,et al.  Sea-ice characterization measurements needed for testing of microwave remote sensing models , 1989 .

[9]  Alex Stogryn,et al.  An Analysis of the Tensor Dielectnc Constant of Sea Ice at Microwave Frequencies , 1987, IEEE Transactions on Geoscience and Remote Sensing.

[10]  Duane T. Eppler,et al.  Texture analysis of radiometric signatures of new sea ice forming in Arctic leads , 1991, IEEE Trans. Geosci. Remote. Sens..

[11]  Vassilios Makios,et al.  The complex‐dielectric constant of sea ice at frequencies in the range 0.1–40 GHz , 1978 .

[12]  Ron Lindsay,et al.  Arctic Sea Ice Surface Temperature from AVHRR , 1994 .

[13]  G. S. Agarwal,et al.  Interaction of electromagnetic waves at rough dielectric surfaces , 1977 .

[14]  J. Luby,et al.  Environmental measurements in the Beaufort Sea, Spring 1988. Technical report , 1989 .

[15]  J. Bredow,et al.  Comparison Of Measurements And Theory For Backscatter From Bare And Snow-covered Saline Ice , 1990 .

[16]  John S. Wettlaufer,et al.  Heat flux at the ice‐ocean interface , 1991 .

[17]  Gary A. Maykut,et al.  The Surface Heat and Mass Balance , 1986 .

[18]  Akira Ishimaru,et al.  Wave propagation and scattering in random media , 1997 .

[19]  E. Carmack,et al.  Thermohaline circulation in the Arctic Mediterranean Seas , 1985 .

[20]  A Mathematical Model for Signal Analysis of FM Radar , 1990 .

[21]  John G. Proakis,et al.  Digital Communications , 1983 .

[22]  K. M. Mitzner Effect of Small Irregularities on Electromagnetic Scattering from an Interface of Arbitrary Shape , 1964 .

[23]  D. Eppler,et al.  Classification of sea ice types with single‐band (33.6 GHz) airborne passive microwave imagery , 1986 .

[24]  Donald B. Percival,et al.  Probability density functions for multilook polarimetric signatures , 1994, IEEE Trans. Geosci. Remote. Sens..

[25]  L. Dennis Farmer,et al.  Passive microwave signatures of fractures and ridges in sea ice at 33.6 GHz (vertical polarization) as observed in aircraft images , 1993 .

[26]  James E. Conel,et al.  Microwave emission from geological materials: Observations of interference effects , 1972 .

[27]  K. Carver Radiometric recognition of coherence , 1977 .

[28]  L. Ulander,et al.  C-band radar backscatter of Baltic sea ice: theoretical predictions compared with calibrated SAR measurements , 1992 .

[29]  J. Kong,et al.  Theory of microwave remote sensing , 1985 .

[30]  Akira Ishimaru,et al.  Comparison of perturbation theories for rough‐surface scattering , 1988 .

[31]  Eric Rignot,et al.  Multifrequency Polarimetric Synthetic Aperture Radar Observations of Sea Ice , 1991 .

[32]  John C. Curlander,et al.  Synthetic Aperture Radar: Systems and Signal Processing , 1991 .

[33]  Anthony Freeman The effects of noise on polarimetric SAR data , 1993, Proceedings of IGARSS '93 - IEEE International Geoscience and Remote Sensing Symposium.