4
SIMULATION OF A PANCHROMATIC SAND BY SPECTRAL LINEAR COMBINATION OF MULTISPECTRAL BANDS Nelson D.A.Mascareiihas; Gerald Jean F.Baoon; Leila IMaria 6. Fonseca Instituto N(aciona1 de Pesquisas Espaciais - INPE - SCT Caixa Postal !515 - 12201 - Sao Jose dos Campos, SP, B r a s i l The simulation of one or more bands of a mu1 tispectral sensor by combination of other bands represents an attractive possibility. In this work an analysis of the simulation of the spatially degraded SPOT panchromatic band by linear combination of the multispectral bands has been perforved uzivg least squares methods. The results ivc1ildC: 1 ) i? theoretical study of the signal to noise ratio of the simulated band as compal-ed with the multispectral bands, and 2) experimental work showing a numerically and visually reasonable estimate of the panchromatic band. Image Simulation; Least Squares Method; SPOT Satellite. 1. INTRODUCTION The simulation of satellite imagery is a useful tool as an image processing technique. One could mention at least two applications in the remote sensing area. a) The large sizes of remote sensing images impose a severe burden on the communications link between the satellite and the ground. Therefore, the simulation of an image by ground processing could offer the potential of a decrease on the data rate. b) In sensor feasibility studies it is common practice to develop simulation procedures before the actual sensor is built, so that many technical aspects can be predicted i n advance. The main idea of this paper is to present a simulation technique f o r a sensor band based on linear combination of other bands. This is possible if there is a substantial spectral overlap beheen the simulated band and the bands that are linearly combined. As an example of this procedure, we present a study of the sinula,ion of a degraded, 20 12 resolution SPOT panchromatic band (P), by linear combination of the two multispectral bands (XS1 and XS2) that spectrally overlap the panchromatic band. The use of the third multispectral band (XS3) was discarded because of the negligible spectral overlap between P and XS3. 2. THEORETICAL BACKGROUND Let f(X) be the spectral characteristic of the scene, gi(X), i=1,2 be the spectral characteristics of the two multispectral bands and gp(X) the spectral characteristic of the panchromatic band. The observed value at each pixel of the multispectral b'ands can be approximately given by : bi = 1 f(A) gi (A)~A i = 1,2 (1 1 Likewise, for the panchromatic band We want to estimate p by 6, where 6 would be given by a fictitious band that is a linear combination of the two multispectral bands, ie: (3) If the coefficients and<, can be determined, the estimate of p at each pixel would be given by p = 5, bl + E2 b2 (6) By comparing eqs. (2) and (5) it is clear that we have to approximate xhe spectral curve g (A) by the linear combination a,gl(X) + E2g2(!). A resonable criterion to adopt is based on the least squares procedure, that is, we want to mi ni mi ze (7) f J [gp(h) - ([xlg,(X) + a , g 2 ( X ) ) I 2 dX by the appropriate choice of =land @z. In order to do this we idiscretize the curves g,(x), gl(A) 32 1 CH2971-0/91/0000-0321$01.00 0 1991 IEEE

[IEEE [IGARSS'91 Remote Sensing: Global Monitoring for Earth Management - Espoo, Finland (June 3-6,1991)] [Proceedings] IGARSS'91 Remote Sensing: Global Monitoring for Earth Management

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Page 1: [IEEE [IGARSS'91 Remote Sensing: Global Monitoring for Earth Management - Espoo, Finland (June 3-6,1991)] [Proceedings] IGARSS'91 Remote Sensing: Global Monitoring for Earth Management

SIMULATION OF A PANCHROMATIC SAND BY SPECTRAL LINEAR COMBINATION OF MULTISPECTRAL BANDS

Nelson D.A.Mascareiihas; Gerald Jean F.Baoon; L e i l a IMaria 6. Fonseca

I n s t i t u t o N(aciona1 de Pesquisas Espaciais - INPE - SCT Caixa Postal !515 - 12201 - Sao Jose dos Campos, SP, B r a s i l

The s i m u l a t i o n o f one o r more bands o f a mu1 t i s p e c t r a l sensor by c o m b i n a t i o n o f o t h e r bands r e p r e s e n t s an a t t r a c t i v e p o s s i b i l i t y . I n t h i s work an a n a l y s i s o f t h e s i m u l a t i o n o f t h e s p a t i a l l y degraded SPOT panchromat ic band by l i n e a r c o m b i n a t i o n o f t h e m u l t i s p e c t r a l bands has been p e r f o r v e d u z i v g l e a s t squares methods. The r e s u l t s ivc1ildC: 1 ) i? t h e o r e t i c a l s t u d y o f t h e s i g n a l t o n o i s e r a t i o o f t h e s i m u l a t e d band as compal-ed w i t h t h e m u l t i s p e c t r a l bands, and 2) e x p e r i m e n t a l work showing a n u m e r i c a l l y and v i s u a l l y reasonab le e s t i m a t e o f t h e panchromat ic band.

Image S i m u l a t i o n ; L e a s t Squares Method; SPOT S a t e l l i t e .

1. INTRODUCTION

The s i m u l a t i o n o f s a t e l l i t e imagery i s a u s e f u l t o o l as an image p r o c e s s i n g t e c h n i q u e . One c o u l d ment ion a t l e a s t two a p p l i c a t i o n s i n t h e remote sens ing area. a) The l a r g e s i z e s o f remote sens ing images impose a severe burden on t h e communicat ions l i n k between t h e s a t e l l i t e and t h e ground. There fore , t h e s i m u l a t i o n o f an image by ground p r o c e s s i n g c o u l d o f f e r t h e p o t e n t i a l o f a decrease on t h e d a t a r a t e . b ) I n sensor f e a s i b i l i t y s t u d i e s i t i s common p r a c t i c e t o deve lop s i m u l a t i o n procedures b e f o r e t h e a c t u a l sensor i s b u i l t , so t h a t many t e c h n i c a l aspects can be p r e d i c t e d i n advance.

The main i d e a o f t h i s paper i s t o p r e s e n t a s i m u l a t i o n t e c h n i q u e f o r a sensor band based on l i n e a r combina t ion o f o t h e r bands. T h i s i s p o s s i b l e i f t h e r e i s a s u b s t a n t i a l s p e c t r a l o v e r l a p b e h e e n t h e s i m u l a t e d band and t h e bands t h a t a r e l i n e a r l y combined. As an example o f t h i s procedure, we p r e s e n t a s tudy o f t h e s inu la , ion o f a degraded, 20 12 r e s o l u t i o n SPOT

panchromat ic band (P) , by l i n e a r combina t ion o f t h e two m u l t i s p e c t r a l bands (XS1 and XS2) t h a t s p e c t r a l l y o v e r l a p t h e panchromat ic band. The use o f t h e t h i r d m u l t i s p e c t r a l band ( X S 3 ) was d i s c a r d e d because o f t h e n e g l i g i b l e s p e c t r a l o v e r l a p between P and XS3.

2. THEORETICAL BACKGROUND

L e t f ( X ) be t h e s p e c t r a l c h a r a c t e r i s t i c o f t h e scene, gi(X), i=1 ,2 be t h e s p e c t r a l c h a r a c t e r i s t i c s o f t h e two m u l t i s p e c t r a l bands and gp(X) t h e s p e c t r a l c h a r a c t e r i s t i c o f t h e panchromat ic band.

The observed v a l u e a t each p i x e l o f t h e m u l t i s p e c t r a l b'ands can be a p p r o x i m a t e l y g i v e n by :

bi = 1 f ( A ) gi ( A ) ~ A i = 1,2 (1 1

L i k e w i s e , f o r t h e panchromat ic band

We want t o e s t i m a t e p by 6, where 6 would be g i v e n by a f i c t i t i o u s band t h a t i s a l i n e a r c o m b i n a t i o n o f t h e two m u l t i s p e c t r a l bands, i e :

( 3 )

I f t h e c o e f f i c i e n t s and<, can be determined, t h e e s t i m a t e o f p a t each p i x e l would be g i v e n by p = 5, b l + E2 b2 ( 6 )

By comparing eqs. ( 2 ) and ( 5 ) i t i s c l e a r t h a t we have t o approximate xhe s p e c t r a l c u r v e g (A) by t h e l i n e a r c o m b i n a t i o n a,gl(X) + E2g2(!). A r e s o n a b l e c r i t e r i o n t o adopt i s based on t h e l e a s t squares procedure, t h a t i s , we want t o m i n i m i ze

( 7 ) f J [ g p ( h ) - ( [ x l g , ( X ) + a , g 2 ( X ) ) I 2 dX

by t h e a p p r o p r i a t e c h o i c e o f = land @ z . I n o r d e r t o do t h i s we i d i s c r e t i z e t h e c u r v e s g,(x), gl(A)

32 1 CH2971-0/91/0000-0321$01.00 0 1991 IEEE

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and g 2 ( X ) over n points and a l i n e a r regression model i s obtained g ( A , ) = a lg l (x , ) + a,g2(Al) + r l

g (A,) = a l g l ( A , ) + a 2 g 2 ( x Z ) -t r 2 P

p .

The sca la rs r . , i = 1 , 2 ... n take i n t o account the e r ror in the approximation. By defining

I-rn J n x 1

We obtain the l inear model gp= 5 a t 1 (10)

I t i s well known t h a t under the hyphotesis t h a t the rank of the matrix G i s given by the number of columns ( 2 in t h i s c a s e ) , t h e l e a s t squares solut ion of t h i s overdetermined system i s given

(11 1 T -1

- ? = ($5) 5 4p = G+ Yp

where G+ i s the Moore-Penrose pseudoinverse o f 5 (Lewi s-and Ode1 1, 1971 ) . For reasons t h a t wi l l become c l e a r in the next sect ion, one may w a n t t o impose an additional cons t ra in t on the values of U, and a2 , namely t h a t a1 t a, = 1 . I n matrix form, t h i s can be expressed as

- _ A U = t , where A = ( I 1 ) and t = 1 ( 1 2 )

This l i n e a r equal i ty constrained l e a s t squares problem has the solut ion given by (Lewis and Odell, 1971):

T - l T T T -1 - - & : = - + ( G _ - G ) A (5 (G;) A (t-5:) (13)

where - CL i s given by equation ( 1 1 ) .

3. SIGNAL TO NOISE RATIO CALCULATION

Let us assume t h a t the l i n e a r cons t ra in t given by eq. ( 1 2 ) i s imposed. I n p rac t ice , It was ver i f ied t h a t the components a1 and a, are pos i t ive so no inequal i ty cons t ra in ts have t o be imposed.

I n order t o ca lcu la te the signal t o noise r a t i o of the simulated band and compare with the signal t o noise r a t i o of the bands b l a n d b,, l e t us assume t h a t each of these bands i s degraded by addi t ive noise, i e

b , = s1 + n b, = s 2 f n 2 (14)

Assume f o r s implici ty (without any loss of genera l i ty ) the following conditions: E(s , ) = E ( s 2 ) = E ( n l ) = E ( n , ) = 0 (15)

E(n: = E (n; ) = 0; (16)

E(S: =E ( S ; = 0' ( 1 7 )

Furthermore, l e t us a l so assume uncorrelated noise processes on the two bands, i e

E ( n , n , ) = 0 (18)

For each mult ispectral band

S

0;' SNRb = -2-

5 2 n (19)

For the simulated band given by - . . p = a,s, t i 2 s 2 + i 1 n l + G2n2 (20)

w S P

U2 we have S N R i j = __

"P ( 2 1 )

We need an additional assumption which i s f requent ly ver i f ied in prac t ice , namely, high cor re la t ion between mult ispectral bands, i e

E 1 (22) psls2

Then, i t can gas i ly be shown t h a t

But 1 - 2 & 1 3 2 < 1 s ince &,and G 2 > 0. Therefore S N R p > SNRb (24)

This r e s u l t shows t h a t an improved signal t o noise r a t i o i s obtained in t h e simulated band . Let us remark t h a t t h e key assumptions leading t o t h i s der ivat ion are: 1 ) l i n e a r constrained est imators ( & + & = 1 ) and 2) high cor re la t ion between the combined bands b l and b,. I t should be observed t h a t in the experimental r e s u l t s we obtained a cor re la t ion coef f icent of .89 between b , and b,.

4. SIMULATION USING SPOT IMAGES

The use of only XS1 and XS2 SPOT mult ispectral bands t o simulate a s p a t i a l l y degraded SPOT panchromatic band i s j u s t i f i e d by the f a c t t h a t XS3 has l i t t l e overlap with the P-band ( s e e Figure 1 ) .

Figure 1 - Typical Spectral S e n s i t i v i t y of HVR Instruments (source: CNES; SPOT-Image, 1986.

The spectral curves of XS1, XS2 and P were d iscre t ized with 10 points ( i e , n=10), leading t o the following numerical r e s u l t s f o r the unconstrained solut ion

322

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- r 0.3426 1

~ r 0.4937 -1

= L 0.397 J

a = L 0.5046 _I

and the constrained solut ion

- r 0.3426 1

~ r 0.4937 -1

= L 0.397 J

a = L 0.5046 _I

and the constrained solut ion

Figure 2 shows the d iscre t ized XS1 and XS2 curves. Figure 3 displays the d iscre t ized P curve, the unconstrained estimated P curve and the l inear constrained estimated P curve.

r-.

Figure 2 - Discretized XS1 and XS2 curves

Figure 3 - Discretized P , ? and p curves

5. EXPERIMENTAL RESULTS 5.1. Spa t ia l Simulation o f 2Om - Resolution SPOT

Panchromatic Band

Since bands XS1 and XS2 have a sampling r a t e of 20m, we degraded the 10m P band, according t o the following two s teps .

a ) Step 1 : Spat ia l F i l t e r i n g of the 10m Resolution Panchromatic Band

The P-band was s p a t i a l l y degraded by applying twice the low pass l i n e a r f i l t e r with f i n i t e impulse response given by

3000 I 1 6 9 337 169

This impulse response was obtained following the procedure suggested by (Banon, 1990) and considering the at tenuat ion f a c t o r Y of the modulation t r a n s f e r function at half the sampling r a t e ( t h a t i s , a t Nyquist frequency) given in Table 1 .

______-__

row 0.16 .~

Table 1 - Attenuation Factor \

The value f o r P-band a r e those of (CNES; SPOT Image, 1986); the values f o r XSP-band are not those of the previous reference b u t have been reevaluated so t h a t the visual impression of the simulated panchromatic band be s imilar t o the mult ispectral bands from t h e point of view of spa t ia l resolut ion.

b ) Step 2: Resampling of the F i l te red 10m Resolution Panchromatic Band

The f i l t e r e d 10m resolut ion panchromatic band of s tep 1 was resampled a t 0.5 spa t ia l r a t e , i e , keeping only the f i r s t pixel of each pa i r of consecutive pixels and keeping only the f i r s t l i n e of each pa i r of consecutive l ines . Figure 4 shows the r e s u l t of t h e spa t ia l simulation of the 20m resolut ion panchromatic band.

I t should be noted t h a t the f i l t e r i n g and resampling procedures could a l so be done using mul t i ra te d i g i t a l signal processing techniques, according t o (Fonseca; Mascarenhas, 1988).

5.2. Spectral Simulation of 2Om - Resolution

5.2.1. Unconstrained Simulation

The spec t ra l ly simulated image has lower mean and lower variance than t h e s p a t i a l l y simulated band. The reason f o r t h i s l i e s in the f a c t t h a t t h e spectral curves do not incorporate o f f s e t and gain fac tors t h a t a re used in ground processing.

5.2.2. Constrained Simul a t ion

I t was observed t h a t the histogram of the spec t ra l ly simulated image under a l inear cons t ra in t i s c loser t o the histogram of the s p a t i a l l y simulated image than the previous case; however, mean and variance of spec t ra l ly simulated image a r e s t i l l lower (although c l o s e r ) than the s p a t i a l l y simulated image.

5.2.3. Gain and Offset Adjustment

The adopted procedure i s t o introduce the gain and o f f s e t adjustments so t h a t the mean value and the standard deviation of the estimated band ( e i t h e r through the unconstrained or the constrained est imat ion) a re equal t o the s p a t i a l l y simulated 20m resolut ion band, i e , in t h e unconstrained case: E ' = such t h a t E ( n ' ) = E ( P O )

where po i s the s p a t i a l l y simulated panchromatic band. Analogous expressions a re va l id f o r the constrained estimators. I n order t o avoid increasing r o u n d off e r r o r s oa, and a& where combined by applying t h e transformation d i r e c t l y on bl and b Z . I t was ver i f ied t h a t the histogram of the gain and o f f s e t compensated estimator without cons t ra in t approximates be t te r the histogram of the s p a t i a l l y degraded panchromatic band than the constrained estimator.

5.2.4. Mean Square Error Between Jmages

The m.s.e. between the s p a t i a l l y simulated band (P, and the spec t ra l ly simulated bands without cons t ra in t ( P 2 s ) , w i t h cons t ra in t (P;c ) , w i t h o u t cons t ra in t with gain a n d o f f s e t compensation ( P Z s G ) and w i t h cons t ra in t with gain of o f f s e t

Panchromatic Band

bl + G, b, ) t 6

a ( p ' ) = ( p ' )

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compensat ion (P, 1 were computed, a c c o r d i n g t o t h e e x p r e s s i o n CG

112 2 5 6 2 5 6

LEWIS, T.O.; ODELL, P.L. E s t i m a t i o n i n L i n e a r Models, P r e n t i c e H a l l , Englewood C l i f f s , N.J., 1971.

These r e s u l t s a r e d i s p l a y e d on T a b l e 2.

P= 1 10.75 I 4.87 I 2.65 I 2.68 I T a b l e 2 - Mean Square E r r o r Between

S p a t i a l l y and S p e c t r a l l y S i m u l a t e d Bands

One can observe t h a t : a ) P, approx imates P, b e t t e r t h a n PzS; b ) t h e r e s s l t s f o r P, and P, a r e approxrmate ly t h e same. It s h h q d be obGGrved t h a t t h e comparison between t h e s p e c t r a l l y s i m u l a t e d band and t h e s p a t i a l l y degraded band r e q u i r e d a smal 1 t r a n s 1 a t i o n a l r e g i s t r a t i o n procedure t h a t was per fo rmed manua l ly . It i s expected t h a t even s m a l l e r mean square e r r o r s c o u l d be o b t a i n e d i f no r e g i s t r a t i o n were necessary.

5.2.5. Visual results

F i g u r e 4 d i s p l a y s 256 x 256 images o f P, P, and Pz . F i g u r e 5 d i s p l a y s P,, Pzs , P,CG a n a t h e a b s o l u t e v a l u e o f t h e d i f f e r e n 5 e image (Pn - P z s G ) , t h r o u g h a l i n e a r c o n s t r a s t s t r e t c h t h a t i n c r e a s e d t h e maximum v a l u e o f t h e a b s o l u t e v a l u e o f t h e d i f f e r e n c e image f r o m a p p r o x i m a t e l y 16 t o 85 f o r v i s u a l purposes. F i g u r e 6 d i s p l a y s t h e SPOT m u l t i s p e c t r a l bands XSl(bl) and XSZ(b2).

It i s observed t h a t Pz, has l o w e r c o n s t r a s t t h a n P2 due t o unknown g a i n and o f f s e t f a c t o r s . Pqc approx imates P, b e t t e r t h a n P z ~ , which i s i n accordance w i t h T a b l e 2. Fur thermore , PZSG and PZCG a r e v e r y c l o s e t o P2 i n v i s u a l te rms.

6. CONCLUSIONS

Through l e a s t squares c r i t e r i a t h e p o s s i b i l i t y o f s i m u l a t i n g one band b y l i n e a r c o m b i n a t i o n o f bands t h a t s p e c t r a l l y o v e r l a p t h e d e s i r e d band has been demonstrated. N u m e r i c a l l y and v i s u a l l y a c c e p t a b l e r e s u l t s were ob ta ined.

BIBLIOGRAPHICAL REFERENCES

BANON, G.J.F. Simulaczo de Imagens de B a i x a ResolucZo (Low R e s o l u t i o n Image S i m u l a t i o n ) , SBA: C o n t r o l e e Automaczo, v o l . 2, n.2, M a r c h / A p r i l 1990, pp. 180-192 ( I n Por tuguese) .

CNES; SPOT I M A G E Guide des U t i l - i s a t e u r s des Ejonn6es SPOT, Vol . 1 Manuel de Reference, l e r e E d i t i o n , Toulouse, 1986.

FONSECA, L.M.G.; MASCARENHAS; N.D.A.; Methods f o r Combined I n t e r p o l a t i o n - R e s t o r a t i o n Through a FIR F i l t e r Design Technique, 1 6 t h I n t e r n a t i o n a l Congress o f t h e I n t e r n a t i o n a l S o c i e t y f o r Photogrammetry and Remote Sensing, Kyoto, Japan, J u l y 1988 i n I n t e r n a t i o n a l A r c h i v e s o f Photogrammetry and Remote Sensing, 27, p a r t B3, Commission 111, pp. 196-205.

“SG ’ “ C G F i g u r e 5 - Images o f P, ,

S G ‘ IP, - P,

F i g u r e 6 - Images o f XS1 and XS2

and

324