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Image restoration using HOS and the Radon transform

Abstract

The authors propose the use of higher-order statistics (HOS) to study the problem of image restoration. They consider images degraded by linear or zero phase blurring point spread functions (PSF) and additive Gaussian noise. The complexity associated with the combination of two-dimensional signal processing and higher-order statistics is reduced by means of the Radon transform. The projection at each angle is an one-dimensional signal that can be processed by any existing 1-D higher-order statistics-based method. They apply two methods that have proven to attain good one-dimensional signal reconstruction, especially in the presence of noise. After the ideal projections have been estimated, the inverse Radon transform gives the restored image. Simulation results are provided.

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Image restoration using HOS and the Radon transform

Author: Sayrol Clols, Elisa,Nikias, C L,Gasull Llampallas, Antoni
Publisher: IEEE IEEE PRESS
Year: 1993
DOI: 10.1109/HOST.1993.264593
Source: https://upcommons.upc.edu/bitstream/2117/101471/1/00264593.pdf
IMAGE
RESTORATION
USING
HOS
AND
THE
RADON
TRANSFORM
Elisa
Say ol*,
Ch ysos omos
L.
Nikias*,
and
Toni
Gad**
Signal
and
Image P ocessing Ins i u e
Uni e si y o Sou he n Cali o nia
Los
Angeles
CA
90089-2564
el:
(213) 7404654,
ax:
(213) 7404651
email:
[email p o ec ed]
*Depa men o Signal
~beo y
and
~ommunica im.
Uni e si a Polibica
de
Ca alunya
08080
Ba celona,
Spain
*
i
El3400
Apdo.
3O002
ABSTRACT^
We p opose he use
o
highe -o de s a is ics
(HOS)
o
s udy he p oblem
o
image es o a ion. We conside
images deg aded by linea
o
ze o phase blu ing poin
sp ead i ne ions (PSF) and addi i e Gaussian noise.
The
complexi y associa ed wi h he combina ion
o
wo-
dimensional signal p ocessing and highe -o de
s a is ics is educed by means
o
he
Radon
T ans o m
The
p ojec ion a each angle is an one-dimensional
signal ha can
be
p ocessed by any exis ing 1-D highe -
o de s a is ics-based me hod. We apply wo me hods
ha ha e p o en o a ain good one-dimensional signal
econs uc ion, especially in he p esence
o
noise.
A e he ideal p ojec ions ha e been es ima ed, he
In e se Radon T ans o m gi es he es o ed image.
Simula ion esul s a e p o ided.
1
INTRODUCTION
Highe -O de s a is ics ha e been success ully applied
be o e
U,
he p oblem o
2-D
signal econs uc ion. In
[l]
he phase o he bispec um is used o econs uc
images
deg aded by
a
ji e y channel wi h addi i e one
in e e ence. In
[2]
he bispec um is used
o
es ima e a
andomly ansla ing and o a ing objec om
a
sequence
o noisy images. Ano he applica ion is desc ibed in
[3]
whe e in a ian Highe -O de Spec a ea u es
o
p ojec ions
a e
used
o objec classi ica ion.
The Bispec um
B lwl,w2)
o a one-dimensional,
de e minis ic. disc e e- ime signal
in),
is
de ined
as
he
Fou ie T ans o m o i s iple co ela ion unc ion and
is
gi en by
[41 151
whe e
F(w)
is
he Fou ie T ans o m
o
in).
The
phase
o he Bispec um is he e o e
his
wo k
was
suppo ed
by
he
O ice
o
Na al Resea ch unde con ac
N0oO14-92-J-1034
and he Spanish Minis y
o
Educa ion and Science.
dBpwpw2)
=
NWl)
+
W2)
-
Nq+w2)Q)
whe e
#(w)=.CF(w).
The Bispec a, and HOS in
gene al, a e insensi i e
o
addi i e Gaussian
noise
and
p ese e he Fou ie phase o he signal up
o
a
linea
phase ac o .
Ou
goal is
o
exploi such p ope ies o
he "a ion o
2-D
blu ed
and
noisy images.
We ha e de eloped echniques ha conside
wo
HOS-based me hods ha ha e p o en
o
a ain
good
1-D
signal econs uc ion. The m one is he Bispec um
I e a i e Recons uc ion Algo i hm
@IRA)
desc ibed
in
[6]
ha was u ilized o signal econs uc ion om he
phase o he bispec um. Al hough i was applied o
es o a ion o images, he p ocessing
was
made
on
a
line
by line
basis.
When
he
image
is
a ec ed by
a
ocus blu
he dis o ing il e is
2-D
and he econs uc ion o
lines
does no lead o good
esul s.
This me hod canno be
ex ended o he wo dimensional
case
since
i
is
based
on
he ceps al coe icien s ha
can
no
be
de ined in
2-D.
Addi ionally,
BIRA
does no pe o m well
when
he
Z-
ans o m o he signal has ze os
on
he uni ci cle,
unless
an
exponen ial window
o
he o m
an
mo es
he
ze os ou wa ds o inwa ds. An adequa e pa ame e
U
is
usually di icul o ind. Fo una ely,
as
we will
see,
we
can o e come bo h p oblems by econs uc ing om
p ojec ions. The second app oach
we
s udy is
he
Weigh
Slice
me hod
(WS)
[7]
ha eco e s he signal o in em
e en in he case o ze os
on
he uni ci cle. Howe e ,
al hough possible, i s ex ension
o
2-D
will
inc ease
eno mously i s analy ical complexi y. We p esen
an
algo i hm using he WS me hod o e he p ojec ions
o
he image.
In Sec ion
2
we desc ibe he imaging sys em ha
we
assume. We e iew he p ojec ion heo em ha allows
he es o a ion o images om hei p ojec ions. In
Sec ion
3
we de elop wo di e en me hods o he
es o a ion ei he om he
phase
o he Bispec um
o
om he phase
o
he Fou ie T ans o m.
In
Sec ion
4
some examples
a e
gi en. Finally, Sec ion
5
is de o ed
o conclusions and ema ks.
0-7803-1238493 $3.00
0
1993
IEEE
76
..
.
.
I_-.
2
PRELIMINARY DEFINITIONS
To add ess he p oblem o eco e ing images om
deg aded e sions o i ,
we
assume a linea imaging
sys em wi h space in a ian poin sp ead unc ion and
addi i e Gaussian noise. Thus. o he con inuos model
(3)
whe e g(x,y) is he obse ed image, h(x,y) he poin
sp ead unc ion, (sy) he o iginal image and n(x,y) he
addi i e Gaussian noise.
The 2-D signal eco e y p oblem can be uniquely
decomposed in o many l-D signal econs uc ion
p oblems. The Radon ans o m o a 2-D unc ion, lx,y),
deno ed pe(s), is de ined
as
i s line in eg al along a line
inclined a
an
angle
8
om he y-axis and a a dis ance
s
om he o igin.
A
undamen al ela ionship, he
P ojec ion Theo em, ela es he l-D Fou ie ans o m o
he p ojec ion
pds),
wi h he cen al slice, a angle
e,
o
he 2-D Fou ie ans o m o he objec l y)
gp&)
=
hp&)
* ps(S)+Fl,S+G@ )
=
H(e, F(6@
(4)
whe e
gpds).
hpe(s),
pds)
a e he p ojec ions o g(x,y),
h(x,y), (x,y) a angle
8,
and
G(e, ),
H(e. ),
F(8, )
a e
he Fou ie ans o ms in pola coo dina es o g(x,y),
h(x,y), and lx,y), espec i ely.
We conside ha he Op ical T ans e Func ion
(OF),
he Fou ie ans o m o he PSF, has linea o ze o
phase.
As
we
see
om
(4).
when he phase o he
OTF
is
ze o, he phase o
he
l-D Fou ie ans o m o each
p ojec ion G(O, ), co esponds o he phase o he
Fou ie ans o m o he p ojec ion o he o iginal image,
In
mos applica ions, blu deg ada ions due o a numbe
o
sou ces
a e
conside ed o ha e linea o ze o phase. Fo
example in
[8]
models o eal ou -o - ocus images a e
in es iga ed. I is shown ha he phase is ei he ze o o
linea . Fu he mo e, a unique disc e e ep esen a ion
esul s in a PSF suppo ha co e s he minimum
numbe o pixels and whe e he
OTF
has ze o phase.
I is well known ha he disc e iza ion o he in e se
o mula o he Radon T ans o m is no easily de ined.
Finding accu a e and as algo i hms is a cu en opic o
esea ch. On he o he hand, i he PSF suppo is no an
in ege numbe , in e ms o numbe o pixels, some
dis o ion occu s. Despi e hese p oblems, es o a ion
om p ojec ions is s ill easible.
F(e.5).
3
RESTORATION FROM THE PHASE OF
THE PROJECTIONS
I was shown in
[9]
ha a sequence o leng h
N
can
be
uniquely speci ied i he phase unc ion
is
known
a
(&I)
dis inc equencies in he in e al
O<w<z,
excep o a
cons an ac o . Likewise in
[6],
i is shown ha a
sequence is uniquely speci ied
i€
he phase o he
bispecuum is known a
N{N-l)n
dis inc equencies in
he egion
O<WI+W~<
z,
W~<WI,
wl 0,
excep o
a
cons an ac o and a linea shi . This
is
ue unde he
assump ions ha he Z- ans o m o he signal has no
ze os in ecip ocal pai s.
The e o e, i he p ojec ion o he blu ing il e
has
leng h
da
and he blu ed p ojec ion
has
leng h
Lb
he e
is
a
unique signal o leng h
Lbe
=
Le
-
(de
-1)
wi h he
same phase unc ion (o phase bispec um) han he
blu ed p ojec ion. This signal
is
no hing bu he
p ojec ion o he o iginal image.
We nex desc ibe wo HOS-based me hods ha
can
be
used o he econs uc ion o he p ojec ions. Fo mo e
de ails on he algo i hms
see
161
and
171
3.1 Recons uc ion
wi h
BIRA
As
we men ioned be o e, BIRA econs uc s
a
signal
om he phase o i s
bispecuum.
I employs he
ceps al
coe icien s ha o a signal pe(n) a e
de ined
as
L,
whe e aipa
bipe
a e
he ze os inside and ou side
he
uni
ci cle espec i ely, and
Cipe
a e he poles inside he uni
ci cle o he Z- ans o m o pe(n). The las e m is no
included o ini e sequences
(L2
=O).
The ceps al
coe icien s a e ela ed o
he
phase o he bispec um
as
and
o
he powe ceps um
as
whe e
Aipe
is a cons an . I s ela ion
o
he signal is
pe(n)
=
F1/eF/C P~m)l),
n=O,..,N-1
(9)
77
Wh
C
m)
=
P
e(
-l/mA
e(")
D0
op
m=O
l/mB
8-m)
md)
P
is he ceps um o he signal.
The algo i hm
s a s
om he ue sequence o he phase
o he bispec um o a leas
N(N-1)/2
samples and
an
ini ial guess o he powe ceps um. I con e ges
o
a
unique solu ion o he ceps al coe icien s and
consequen ly o he signal, excep o
a
cons an ac o
and a space shi .
An
addi ional p ocedu e is added
o
conml he space shi . The scale ac o is calcula ed
aking in o accoun ha he p ojec ion is a posi i e
unc ion and ha
all
he p ojec ions ha e he same a ea,
he olume o
he
image.
As
we
see
in
(5)
and
(6)
in
he case ha he e a e ze os
on
he
uni ci cle, he ceps al coe icien s a e in ini e
sequences. I s unca ion leads o inco ec solu ions.
Two di e en al e na i es a e p oposed when p ojec ions
wi h ze os on he uni ci cle
a e
de ec ed.
A)
When he numbe o such p ojec ions
is
low
:
In his case we es o e he image om he es o he
p ojec ions since he omission o ew p ojec ions does
no al e he es o a ion signi ican ly.
B)
When he numbe o such p ojec ions is high
:
We
y
o
iden i y he coe icien s o he blu ing il e
using he ollowing p ocedu e:
B1)
Recons uc he p ojec ions ha ha e nei he ze os
on he uni ci cle no ecip ocal pai s.
B2)
F om (4) we
see
ha i we know gpB(s) and pe(s)
we
can
ob ain
hpHs)
by decon olu ion. The sequence
is
he p ojec ion o he blu ing il e a
an
angle Band i s
coe icien s a e weigh ed sums o
he
coe icien s o he
blu ing il e . We build a sys em o equa ions o he
ollowing o m
xa=y,
(11)
whe e
X
is
he
ma ix
o he weigh s
o
he coe icien s a
he
speci ied angles,
a
is he coe icien ec o and
y
is
he ec o o he es ima ed blu ing il e p ojec ed a he
speci ied angles.
As
an
example suppose we ha e only
he p ojec ion a angle
B
=
0"and a squa e 3x3 PSF wi h
coe icien s named om
a
o
i.
Then, he sys em o
equa ions will be
111000000
000111000
000000111
[
.I
a
b
C
d
c
8
h
i
.I
a+b+c
d+c+
In gene al, we can sol e he
sys em
o
equa ions
b
ind
he Coe icien ec o i
he
ank
o he ma ix is
equal
o g ea e han
Nc.
Using a
LS
app oxima ion he
solu ion will be
21
=
(XHX)-'
XH
y
(12)
B3)
Once we know he blu ing il e coe icien s we
can
ei he decon ol e he 2-D noise- ee image o he Id
noise ee p ojec ions.
3.2
Recons uc ion wi h he
WS
me hod
We
can
uniquely econs uc he p ojec ions om he
phase only o he Fou ie ans o m e en in
he
case
ze os lie on he
uni
ci cle [9]. Howe e , in
he
p esence
o noise he phase
is
deg aded. The e o e, we decompose
he econs uc ion o a blu ed noisy p ojec ion
in
wo
s eps. In he i s s ep, a me hod based on
HOS
educes
Gaussian noise p ese ing he phase unc ion. We choose
he WS me hod because i wo ks when hen?
a e
oo s
on
he uni ci cle and i
has
be e pe o mance han o he
me hods. In he second s ep we deblu he signal om i s
Ph.
S ep
1)
I is known ha o a causal and exponen ially
s able sys em wi h inpu assumed o
be
independen ,
iden ically dis ibu ed and non Gaussian, wi h skewness
p.
he ou pu bispec um
BX(wl,w2)
exis s and
is
gi en
by [31, [dl
BX(wpw$
=
B
H(w1)
WW~)
H*(wl +w2)
(13)
As
we
see,
inding he coe icien s o he il e
H(w)
is
equi alen
o
es ima e he sequence
F(w)
in (1).
The Weigh Slice WS) algo i hm
has
been p e iously
used o ob ain he pa ame e s o a non-minimum
FIR
sys em. The pa ame e s can
be
exp essed
as
a
linea
combina ion o cumulan slices. I was shown ha
i
he e exis s a se o weigh s ha gi es
a
causal slice,
hen he
FIR
sys em can be iden i ied. The sys em o
equa ions
is
exp essed
as
SW
=
bo (14)
whe e
S
is
he ma ix o cumulan s
s
1
C,is
he es ima ed
n h
o de cumulan o he ou pu
signal,
w
is
he
weigh ec o
w
=
(
w2, w3cj), w4(j,k),
...
)
(16)
and
bo
is
he coe icien ec o
bo
=
(0
...
0
I
...
b(q-I) b(9)).
(17)
The unknowns a e he ec o
w,
and he las q elemen s
The ma ix equa ion is sol ed in
wo
s eps
:
1) Compu a ion o he minimum no m weigh s ha gi e
a
causal
W-slice
o
bo.
su
wm
=
(0,
..
,
0,I)
wm
=
SU#
1
whe e
Su
is he
ma ix
o med om he uppe
q+l
ows
o
S,
and
Su#
deno es he pseudo in e se o
Sua
2)
Compu a ion o he coe icien s
as
bo=Swm=SSu#l
S ep
2)
The ec o
bo
is he sequence o he noise-
educed blu ed p ojec ion. Once
bo
has been calcula ed,
we
deblu he signal using a simila algo i hm han he
one desc ibed in
[9].
I is equi alen o BIRA, i
s a s
wi h he
Vue
sequence o he phase o he Fou ie
T ans o m and an ini ial guess o i s magni ude.
4
EXAMPLES
In he nex examples, he Radon T ans o m
is
calcula ed
om an in e pola ion
o
he Ca esian sampling g id o
he
2-D
FFT
o he image o a pola g id. The In e se
Radon
T ans o m
is
implemen ed in a e e se way.
Fig. la shows a 24x24 image. The econs uc ed image
a e
applying Radon T ans o m ollowed by he In e se
Radon ans o m is shown on Fig. Id. The dimensions o
he
2-D
FIT
and
2-D
IFFT
a e
64x64
o
a oid dis o ion
in he
high
equencies. Fig. lb p esen s a blu ed
e sion o his image when a
3x3
Gaussian il e wi h
pa ame e
a
=
0.4
is used. Fig.
le
shows he es o ed
image om he Fou ie phase o he p ojec ions. In Fig.
IC
he
image is blumd wi h he same il e and Gaussian
noise o
SNR=25
dbs is added. The es o ed image
is
shown in Fig.
I
whe e he Ws me hod
is
applied using
one slice only, he hi d o de cumulan
is
es ima ed
hm
50
ealiza ions. Ano he example
is
shown
in Fig.
2a
and
Fig.
24
whe e he o iginal image
is
64x64
and he
2-D
FFTs
a e
256x128.
Fig.
2b
is
a
blu ed e sion
o
his
image wi h a 5x5 Gaussian il e and
a
=
0.4.
Fig.
2c
is
he es o ed image om he Fou ie phase. F om his
image
we
see
ha
high equencies
ha e
been eco e ed.
Howe e , we obse e some dis o ion. This is due
o
ela i e shi ing among p ojec ions. Fig.
3
shows
a
ypical p ojec ion, i s blu ed e sion, he econs uc ed
signal and he di e ence be ween
he
o iginal and he
es o ed signal.
5
CONCLUSIONS AND REMARKS
In his pape ,
we
ha e
shown
ha
i is possible
o
es o e
a blu ed and noisy image om
HOS
o
i s
p ojec ions.
Two di e en app oaches we e gi en
o
econs uc
he
1-
D
signals om ei he he phase o he Fou ie T ans o m
o he phase o he bispec um. Al hough he complexi y
using
HOS
o e
2-D
signals is educed, he
compu a ional load is s ill
high.
Some o he applica ions
o
HOS
o e he p ojec ions
a e
unde in es iga ion.
REFERENCES
[l]
S.A.
Diana , M. R. Raghu ee . “Fas Algo i hms
o phase and magni ude econs uc ion om
bispec a”,
Op ical Enginee ing, May 1990.
[2]
B.M.Sadle , “Shi and Ro a ion In a ian Objec
Recons uc ion using Bispec um”,
Wo kshop
on
HOS
analysis, Vail, Colo ado, I989,pag
106
[3]
V. Chand an,
S.
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P oc.
ICASSP ‘92,
S.
F.,pp -213-216.
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C.
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M.
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J.M.
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P oc.
o
IEEE,
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A.
Pe opulu,
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L.
Nikias, “Signal Recons uc ion
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pug
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J.A.
Fonollosa,
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o
IEEE
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M.I.
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G.
Pa lo ic,
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P oc. ICASSP
‘92, Albuque que.NM,
pp
248.5-2488.
[9]
M.
H. Hayes,
J.
S.
Lim and A.
V.
Oppenheim.
“Signal Recons uc ion om
he
phase o
magni ude”,
IEEE
on
ASSSP,
Vol
28,
No.
6,
Dec
1980.
79
Fig.
la
....................................
..
Fig. lb Fig.
lc
ig. Id Fig.
le
Fig. I
Fig.
2a
Fig. 2b Fig.
2c
e)
RcmmWcIed
om
b
wFl
0
......
...
-50
.
02l4060~
Fig. 2d
80
Fig.3