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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