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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