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| | Relation between measurements in circular and linear polarization bases. |
 | | The relations have formed the basis for interpreting circular polarization measurements in a number of studies (e.g., McCormick and Hendry, 1975, 1979; Hendry and Antar, 1984; Bringi and Hendry, 1990; Metcalf, 1995, 1997); Krehbiel et al., 1996) but are conceptually and analytically difficult to understand. |
 | | corresponds to the total signal power (polarized plus unpolarized), both the tangent and the projection points are on the surface of the outer, total power sphere, while the polarization state itself is on the inner, Poincaré sphere (see Figure 4). |
 | | Circular polarization measurements can be well represented in covariance or Poincaré sphere space (Torlaschi and Holt, 1993, 1998; Krehbiel and Scott, 1999). |
| www.lightning.nmt.edu /nmt_lms/jtech/node15.html (740 words) |
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