Superscripts 1 and 2 in Equation 10.4 indicate the two image acquisitions at the two extremes of the
temporal baseline. The Hermitian coherency matrices of each acquisition are represented as [T
11
]
and [T
22
], and, the non- Hermitian complex polarimetric– interferometric matrix is represented as
[
Ω
12
]
[2]. The complex coherences were obtained from Equations 10.5– 10.8 [27].
µω
111
=
†
K
p
, (10.5)
µω
222
=
†
K
p
, (10.6)
γγγ
φ
ωω
==
()
e
i
12
, (10.7)
γ
µµ
µµµµ
ωω
ωω
ωω
ωω
12
12
1122
1122
111122
22
()
==
†
††
†
††
Ω
TT
, (10.8)
where,
ω
1
and ω
2
are the unitary projection ...
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