Geoscience Reference
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1
0.8
0.6
0.4
0.2
h
0
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
t
Fig. 4 A piecewise linear function f(t) with a slope f (1) = 1/h at the non-horizontal part. As it is easily
shown (see text), for this function, the ' 1 (total variation)-norm
1 is constant and independent of
f ð 1 Þ
2
2 ¼ 1 = h goes to infinity as h goes to zero (i.e., for a very steep gradient). As a
result, the ' 2 -norm solutions do not allow steep gradients, while the ' 1 -norm does
f ð 1 Þ
h while the ' 2 -norm
singularities in a quite different way than the ' 2 -norm of S(f). It is important to demonstrate
this point as it plays a key role in the proposed downscaling scheme.
Let us consider a piecewise linear function:
8
<
:
0 t\ 2
0 ;
ð
1 h
Þ
t
h 1 h
1
2
Þ t 2
f ð t Þ¼
;
ð
1 h
ð
1 þ h
Þ
;
ð 6 Þ
2h
1
2
1 ;
ð
1 þ h
Þ \t 1
as shown in Fig. 4 . It can be shown that the smoothing norms associated with the ' 1 and ' 2 -
norms of f (1) (t) satisfy:
1 ¼ Z 1
0
dt ¼ Z
h
1
h dt ¼ 1
f ð 1 Þ
f ð 1 Þ ð t Þ
ð 7 Þ
0
while
2 ¼ Z
dt ¼ Z h
0
1
h 2 dt ¼ 1
1
2
2
f ð 1 Þ
f ð 1 Þ ð t Þ
h :
ð 8 Þ
1 is independent of the slope
of the middle part of f(t) while the smoothing ' 2 -norm is inversely proportional to h and, as
such, it severely penalizes steep gradients (when h is small). In other words, the ' 2 -norm of
f (1) will not allow any steep gradients and will produce a very smooth solution. Clearly, this
is not desirable in solving an inverse problem associated with the reconstruction of small-
scale details in precipitation fields, such as in the hurricane storm shown in Fig. 2 .
0
It is observed that the TV smoothing norm S TV ð f Þ¼ f ð 1 Þ
2.2 Discrete Representation
Writing Eq. ( 1 ) in a discrete form, the problem of downscaling amounts to estimating a
high-resolution (HR) state, denoted in an m-element vector as x 2
m , from its low-
R
n , where m n. It is assumed that this LR counterpart
resolution (LR) counterpart y 2
R
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