Geoscience Reference
In-Depth Information
The (projected) background influence is complementary to the observation
influence. For example, if the self-sensitivity with respect to the
th observation
is S ii , the sensitivity with respect the background projected at the same variable,
location and time will be simply
i
1 S ii . It also follows that the complementary
trace, tr
, is not the df for noise but for background, instead.
That is the weight given to prior information, to be compared to the observational
weight tr( S ). These are the main differences with respect to standard LS regression.
Note that the different observations can have different units, so that the units of the
cross-sensitivities are the corresponding unit ratios. Self-sensitivities, however, are
pure numbers (no units) as in standard regression. Finally, as long as R is diagonal,
( 4.6 ) is assured (see Sect. 4.3.2 ), but for more general non-diagonal R -matrices it is
easy to find counter-examples to that property.
Inserting ( 4.12 )into( 4.14 ), we obtain
.
I S
/ D m tr
.
S
/
S D R 1 H
B 1 C H T R 1 H
/ 1 H T
.
(4.16)
/ 1 is equal to the analysis error covariance matrix A , we can
also write S D R 1 HAH T .
B 1 C H T R 1 H
As
.
4.3.2
R Diagonal
In this section it is shown that as long as R is diagonal ( 4.6 ) is satisfied. Equation
( 4.16 ) can be written as
S D R 1 H
B BH T .
HBH T C R
/ 1 HB
H T
Œ
(4.17)
D R 1 HBH T R 1 HBH T .
HBH T C R
/ 1 HBH T
HBH T ,( 4.17 ) becomes
Let's introduce the matrix V
D
S D R 1 V R 1 V
/ 1 V
.
V C R
D R 1 V
/ 1 V
Œ
I .
V C R
D R 1 V
/ 1 .
/ 1 V
Œ.
/ .
V C R
V C R
V C R
D R 1 V
/ 1 R
.
V C R
D R 1 Œ.
/ 1 R
/ 1
/.
.
V C R
V C R
V C R
R
(4.18)
D R 1 Œ
/ 1
.
I R
V C R
R
/ 1 R
D I .
V C R
/ 1 V
D .
V C R
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