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TSINGHUA SCIENCE AND TECHNOLOGYISSN 1007-0214 21/21 pp404-407Volume 10, Number 3, June 2005
Rotationally Symmetric Translating Solutions to Curvature Flows in Image Processing*
LIU Qinghua ( )**, CHEN Xiuqing ( )
Department of Mathematical Sciences, Tsinghua University, Beijing 100084, China
Abstract: This paper proves the existence of rotationally symmetric solutions to a curvature flow in image
processing. The flow includes the level sets flow and the mean curvature flow projected onto the normal.
Sharp estimates are obtained for these solutions..
Key words: level sets flow; mean curvature flow; singular ordinary differential equation; priori estimate;rotationally symmetry
Introduction
According to the geometrical framework for image
processing, intensity images can be considered as
surfaces in the spatial-feature space. The image is
thereby a two-dimensional surface in three-
dimensional space (see Refs. [1-3] for a detailed
description of this idea). If we use the graph
of a function to denote
the surface (i.e., the image), various mathematical
flows can be used to model the restoration processing
of the image. In this paper, we study the best-known
flow among these, namely,
={( , ( )) : }X x V x x ( )V x
2
1div
| | +| |
V V
t V V 2 (1)
where 0 is a constant, and is a
function depending on and Here,
and div are the gradient operator and the diver-
gence operator with respect to
( , )V V x tnx R [0, ).t
x (see Ref. [4] for
further details).
In the view of pure mathematics, the flow given by
Eq. (1) is very interesting because it includes two fa-
mous flows:
For 1 , Eq. (1) is the mean curvature flow pro-
jected onto the normal[5,6]
. For 0, Eq. (1) is the
mean curvature flow of the level sets
{ : ( )n
t }M x V x tR (Refs. [7, 8]).
The existence of an entire smooth convex solution
to Eq. (1) for general remains an open issue, al-
though there are some results on smooth solutions
(but not necessarily convex) for the case of 1
(Refs. [5, 6]) and on continuous viscous solutions for
the case of 0 (Refs. [7, 8]). All of these solu-
tions obtained are not necessarily convex. Recently,
to analyze the geometric structure of convex translat-
ing solutions to Eq. (1), Jian[9]
used the maximum
principle and moving plane methods and showed that
such an entire solution may be rotationally symmetric.
In this paper, we will restrict our interest to the
existence of entire rotationally symmetric translating
convex solutions to Eq. (1). This requires us to find a
strictly convex function such that2[0, )r C
( , ) (| |)V x t t r x nRReceived: 2004-01-17; revised: 2004-03-08
Supported by the National Key Basic Research and Devedepment
(973) Program of China (No. G19990751) and the Trans-Century
Training Program Foundation for the Talents of China
To whom correspondence should be addressed.
E-mail: [email protected]; Tel: 86-10-62784334
that solves Eq. (1) in .
We would like to point out that the variational
method in image processing is very active (see
Ref. [10] for the details).
LIU Qinghua ( ) et al Rotationally Symmetric Translating Solutions to 405
1 Main Theorem
Theorem 1 If and 2n 0 , then there exists
a strictly convex function such that
solves Eq. (1) in . Further-
more, r is a solution to the initial value problem of the
following singular ordinary differential equation
(ODE):
2[0, )r C
( , ) (| |)V x t t r x nR
2
( ) 1( ) 1, (0, )
( ( ))
r" t nr' t t
r' t t (2)
and
(3) ( ) 0 for (0, ), (0) (0) 0r" t t r r'
Finally, the function ( ) (| |)u x r x satisfies
| | | |( ) ,
1
nx xu x x
n nR (4)
and2 2
| | | |( ) ,
2 2( 1)
nx xu x x
n nR (5)
2 A Prior Estimate
In this section, assume and sat-
isfies Formulas (2) and (3). We will prove Formulas
(4) and (5).
2n 2[0, )r C
Lemma 1 If 0, 2,n and [0, satis-
fies Formulas (2) and (3), then satisfies
2r C( ) (| |)u x r x
| | | |( ) ,
1
nx xu x x
n nR (6)
and2 2
| | | |( ) ,
2 2( 1)
nx xu x x
n nR (7)
Proof It follows from Formulas (2) and (3) that
1( ) 1, (0, )
nr' t t
t (8)
and
11, (0, )
nr" r' t
t (9)
Obviously, Formula (8) implies2
( ) and ( ) , [0, )1 2( 1)
t tr' t r t t
n n (10)
Let2
( ) ( ) .2
tw t r t
n
Then w satisfies
10, for (0, )
nw'' + w' t
t
'
(11)
and
(0) 0 (0)w w (12)
Consequently, we conclude that
(13) ( ) 0, (0, )w' t t
Otherwise, we could find and0
0t 0 such
that0
( ) 0w' t but for ( ) 0w' t0 0
( , ].t t t
Integrating Formula (11), we would then have
0
00
10 ( ) ( )d
t
t
nw' t w' t t
t0,
a contradiction!
It follows from Formulas (12) and (13) that 2
( ) and ( ), [0, )2
t tr' t r t t
n n (14)
which, together with Formula (10), verfies Formulas
(6) and (7).
3 Existence
In this section, we prove the existence result of
Theorem 1.
Lemma 2 If 0 and , then there exists a
function
2n2[0, )r C which satisfies Formulas (2)
and (3).
Proof Because of the singularity of Eq. (2) at the
origin, we have to consider the approximation
problem,
2
( ) ( ) 1( ) 1, (0, )
( ( ))
r" t nr' t t
r' t t (15)
2
(0) and (0)2
r r'n n
(16)
For each (0,1) , by ODE theory, there exists a
unique smooth solution to Eqs. (15) and (16) in the
maximal interval [0, T) for some We de-
note it by
.T.r Obviously,
2 2
30
( )(0) lim ( )
( )
" "
t
nr r t
n (17)
This leads us to claim that
(18) ( ) 0, [0, )"r t t T
In fact, if there is a such that1
(0, )t T1
( ) 0,"r t
then we may assume:
Tsinghua Science and Technology, June 2005, 10(3): 404 407406
00 0( ) 0, ( ) 0, ( , + )
" "r t r t t t t (19)
for some and 0
0t 0 such that0
.t T
Owing to Eqs. (16) and (17), we may then further
assume
0 0( ) 0, [ , + )
'r t t t t (20)
Thus,
0 0 00 ( ) ( ), ( , +
' 'r t r t t t t ).
This result, together with Formulas (15), (19), and
(20), implies, however,
0
0 02
0 0 0
( ) ( ) 1 11 ( ) (
( ( ))
"' '
'
r t n nr t r t
r t t t)
2
( ) ( )1( )
( ( ))
"'
'
r tnr t
t r t
0 0
1( ) 1, ( , + ),
'nr t t t t
t
a contradiction! Therefore,
(21) ( ) 0, [0, )"r t t T
which, together with Eqs. (16), implies
( ) , (0, )'r t t T
n(22)
Similarly, if there is a such that
we obtain by Eq. (17). Further-
more, Eqs. (15) and (21) imply the function
2[0, )t T
2( ) 0,
"r t2
0t
2
( ) ( )1( ) : ( ) 1
( ( ))
"'
'
r tny t r t
t r t
attains a maximum at t2. Therefore,
2 2 2
2 2
2
( 1)[ ( )( ) ( )]( ) : 0,
( )
" 'n r t t r ty' t
t
i.e., =0, in contradiction with Formula (22). In
this way, we have proved Formula (18).
2( )
'r t
By Formula (18), we conclude that .T
Otherwise, we see that T is finite and
lim ( ) lim ( )'
t T t Tr t r t
(18).
.
by the maximality of T and Formula (22). Taking the
limit as t goes T in Eq. (15), we obtain a
contradiction with Formula
to
To obtain a smooth solution to Formulas (2) and
(3), we require a priori estimate for problem Eqs. (15)
and (16). This will be carried out by repeating the
arguments of the proof of Lemma 1
First of all, it follows from Formulas (15)-(18) that
1( ) 1, (0, )
'nr t t
t (23)
and
11, (0, )
" 'nr r t
t (24)
Thus, Formulas (23) and (16) yield2 2
( )( ) and ( ) , [0, )
1 2( 1) 2
' t tr t r t t
n n n
(25)
We also note that the function ( ) : ( )w t r t2
( )
2
t
nsatisfies
10, for [0, )
" 'nw w t
t
and
(0) 0 (0).'w w
Consequently,
( ) 0, [0, ).'w t t
(See the proof of Eq. (13).) This gives: 2
( )( ) and ( ), [0, ),
2
't tr t r t t
n n
which, in combination with Formula (25), yields
( ) and1
't tr t
n n2
( )
2
t
n
2 2( )
( ) , [0, )2( 1) 2
tr t t
n n (26)
This result, together with Eqs. (5) and (18), implies
210 ( ) ( ) 1 ( ( ) )
" 'nr t r r
t'
2
11 1
1
n t
n n
2 2
2
( 1)( 1) ( ), [0, )
( 1)
n tt
n n (27)
Now consider two cases: 0 and 0. First,
we assume 0. Using the estimates, Formulas
(26) and (27), we can choose a subsequence
and a function (for
any
0k (k )1,
[0, )r C
(0,1)) such that
(28) 1,
in [0, ) ask
r r kC
Moreover, since r satisfies Formulas (15)-(18), we
see that 2[0, )r C satisfies:
LIU Qinghua ( ) et al Rotationally Symmetric Translating Solutions to 407
2
( ) 1( ) 1, (0, )
1 ( ( ))
r" t nr' t t
r' t t
'
(29) References
(30)(0) 0 (0)r r
[1] El-Fallah A I, Ford G E. On the mean curvature diffusion
in nonlinear image filtering. Pattern Recognition Letters,
1998, 19: 433-437.
and
(31)( ) 0, [0, )r" t t[2] Sochen N, Kimmel R, Malladi R. A geometrical frame-
work for low level vision. IEEE Transaction on Image
Processing, Special Issue on PDE Based Image Process-
ing, 1998, 7(3): 310-318.
To finish the proof of Lemma 2, we only need to
prove
(32)( ) 0, [0, )r" t t
In fact,
1(0) : lim (0) lim 1 (0)
k
" '
k kk
nr" r r
k
[3] Yezzi A. Modified curvature motion for image smoothing
and enhancement. IEEE Transaction on Image Processing,
Special Issue on PDE Based Image Processing, 1998,
7(3): 345-352.
[4] Aubert G, Kornprobst P. Mathematical Problems in
Image Processing Partial Differential Equations and
Calculus of Variations. New York: Springer-Verlag, 2002. 2
( ( (0)) ) .k
'k r
n[5] Huisken G. Non-parametric mean curvature evolution
with boundary conditions. J. Differ. Equations, 1989, 77:
365-379.
If there is a such that , then
Formulas (29) and (31) imply the function
3(0, )t
3( ) 0r" t
[6] Ecker K, Huisken G. Mean curvature evolution of entire
graphs. Ann. of Math., 1989, 130: 453-471. 2
1( ) : ( ) 1
( )
n rZ t r' t
t r
"
'
attains a maximum at the point t3. Thus,
3 3 3
3 2
3
( 1)( ( ) ( ))( ) 0,
n r" t t r' tZ' t
t
[7] Evans L C, Spruck J. Motion of level sets by mean curva-
tures. J. Diff. Geom., 1991, 33: 635-681.
[8] Chen Y G, Giga Y, Goto S. Uniqueness and existence of
viscosity solutions of generalized mean curvature flow
equations. J. Diff. Geom., 1991, 33: 749-786. which would yield in contradiction with
Eq. (26). Hence, Formula (32) has been proved.
3( ) 0,r' t
[9] Guan B, Jian H. The Monge-Ampere equation with
infinite boundary value. Pacific J. Math., 2004, 216(1):
77-94.Second, assume 0. Then we solve Eq. (2) to
get a function
2
( ) .2( 1)
tr t
n Obviously, this func-
tion satisfies the requirement of Lemma 2. In this way
we have proved the lemma.
Proof of Theorem 1 Theorem 1 is only the
combination of Lemma 1 and Lemma 2.
[10] Chan T F, Shen J, Vese L. Variational PDE methods in
image processing. Notices of the AMS, 2004, 50(1): 14-26.