Geoscience Reference
In-Depth Information
16.2.1
Analysis Error Covariance for the Routine Observations
with the ET Technique
To be consistent with the ET technique of ensemble generation, we need to utilize
a guess of the analysis error covariance matrix
P
g
associated with the routine
observational network. Let the columns of the nxK matrices
X
o
and
X
v
list the raw
ensemble perturbations at the observation and verification times, respectively, of the
ensemble forecast initialized at the initialization time.
The forecast perturbations
X
o
can be transformed into a set of perturbations
X
r
that are consistent with
P
g
using
X
r
D
X
o
T
(16.1)
where
ƒ
1=2
B
T
T
D
B
—
(16.2)
and where
B
D
Œ
b
1
;
b
2
;:::;
b
K
is a
K
K
orthogonal matrix containing the
eigenvectors of the symmetric matrix
X
oT
P
a
1
g
.Inotherwords,
X
0
=N
X
oT
P
a
1
g
X
o
ƒ
K
K
B
T
:
D
B
(16.3)
N
where
ƒ
D
diag
.
11
;
22
;:::;
KK
/
is a
K
K
diagonal matrix listing the eigen-
values of
X
oT
P
a
1
g
. Since the sum of the forecast perturbations is equal to
zero, one of these eigenvalues will be equal to zero. Consequently, provided each
ensemble contains K1 linearly independent perturbations,
X
0
=N
ƒ
can be written in the
form,
ƒ
.K
1/
.K
1/
0
0
ƒ
K
K
D
(16.4)
0
where
ƒ
.K
1/
.K
1/
is a (K1)(K1) diagonal matrix whose diagonal elements
are all greater than zero. The —
ƒ
used in (
16.4
) is obtained from
ƒ
by setting its zero
eigenvalue equal to 1, in other words,
ƒ
.K
1/
.K
1/
0
0
—
ƒ
K
K
D
(16.5)
1
Note that while —
does not exist. This adjustment of
the eigenvalue matrix is permissible because it does not affect the sample covariance
matrix of initial perturbations implied by (
16.3
). To see this, first note that pre and
post multiplying (
16.5
) by the eigenvector
b
K
corresponding to the zero eigenvalue
K
D
0
ƒ
has an inverse, the inverse of
ƒ
shows that
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