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Sensing Surface and Underneath Features

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Book cover Understanding Earth Observation

Part of the book series: Remote Sensing and Digital Image Processing ((RDIP,volume 23))

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Abstract

It is now clear that both passive and active remote observing systems gain information on the Earth’s environment by essentially capturing the power carried by the electromagnetic waves that interacted with the terrestrial materials in the sense outlined in Sect. 10.1.3 It should be added that the phase of the waves, measurable by coherent radar observations, provides supplemental pieces of knowledge. The information brought by the directly measured wave quantities (power and/or phase) resides in the imprinting that the observed target exerts on the interacting electromagnetic field.

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Notes

  1. 1.

    Systems exploiting low-frequency or quasi-static fields are not considered.

  2. 2.

    Indeed, as already noted, it is not even uncommon to find the term “reflection” denoting scattering.

  3. 3.

    Extremely dry scenarios are disregarded.

  4. 4.

    Given the finite dimension of the coherent source, the term diffracted could be more appropriate.

  5. 5.

    The more restrictive Fraunhofer criterium [22, Chap. 11] can be also adopted.

  6. 6.

    The reflection coefficients can be alternatively expressed in terms of refractive index.

  7. 7.

    The degree of roughness can be consequence of natural processes, as well as of agricultural practices [28].

  8. 8.

    Clearly apart from targets the surface of which has peculiar orientations, or which include corner reflectors.

  9. 9.

    As said, the second term in (7.65) is further reduced by the effect of the permittivity-dependent attenuation in the surface layer.

  10. 10.

    Lidar returns behave analogously.

  11. 11.

    It is again pointed out that the multi-platform systems such as TanDEM, although named bistatic, actually do not perform this kind of measurements, which should be carried out over an angular range sufficiently wide to observe the complete features of bistatic “scattering”, including specular reflection.

  12. 12.

    Clearly apart from the effect of the frequency-dependent permittivity on \(\mathcal{R}\).

  13. 13.

    As usual, the antenna is assumed collapsed in its phase center.

  14. 14.

    Clearly according to the frequency of the interacting wave.

  15. 15.

    The present simplified approach does not account for polarization.

  16. 16.

    In ground-based observations, the contribution comes from the environment above the observed layer.

  17. 17.

    The upward scattered wave is assumed to emerge almost entirely: this implies that the inner field has negligible stationary component and that total reflection (Sect. 6.4) does not occur.

  18. 18.

    For sufficiently low extinction.

  19. 19.

    Strong fluctuations of scattering intensity about high values are observed because of speckle (Sect. 7.2).

  20. 20.

    The relatively smooth surface of oil-covered water in the slick area considered in Sect. 14.2.2.3 is a typical target yielding reduced backscattered power.

  21. 21.

    Except that when the mean surface is perpendicular to the direction of observation, or when its shape corresponds to the dihedral or trihedral configurations considered in Sect. 6.6

  22. 22.

    Clearly, down to the penetration depth (say, a few micrometers) of the optical radiation.

  23. 23.

    Application details are given in Sect. 14.2.1.1

  24. 24.

    Especially at grazing angles.

  25. 25.

    This concept should be kept distinct from that of permanent scatterer outlined in Sect. 12.3.3.3

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Solimini, D. (2016). Sensing Surface and Underneath Features. In: Understanding Earth Observation. Remote Sensing and Digital Image Processing, vol 23. Springer, Cham. https://doi.org/10.1007/978-3-319-25633-7_13

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