Some Notes On Differential Operators

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SOME NOTES ON DIFFERENTIAL OPERATORSAIntroductionIn Part 1 of our course, we introduced the symbol D to denote a function which mapped functions into their derivatives. In other words,the domain of D was the set of all differentiable functions and theimage of D was the set of derivatives of these differentiable functions. We then, as usual, introduced the notation D(f) f'.*Recalling that if f is any function and c is any number, we define thefunction cf by [cfI (x) means cf (x); and that if f and g are any twofunctions which have the same domain, we define the new function[f gl by [f gl (XI f (x) g (x); we notice that D is a linearmapping. That is, if f and g are both differentiable functions defined on the same domain and if a and b are any (real) numbers thenNotice that (1) is the special case of our notation L(f) or morefamiliarly;L(y) where L(y) y'.The key point is that if we restrict the domain of D to the set of allanalytic functions**(where by analytic we mean that the function isinfinitely differentiable which in turn means that the function possesses derivatives of every order) we can, in a natural way, invent astructure on D that is very analogous to the arithmetic structure ofpolynomials.Aside from this structure giving us some very convenient notationand aside from its being interesting in its own right (in fact, theset of analytic functions is a very nice example of a more generalvector space which we shall talk about more in Block 3 ) , it is veryhelpful to us in handling linear differential equations and systems oflinear differential equations. These ideas will be discussed in thefollowing sections.*It i s c o n v e n t i o n a l t o w r i t e f r a t h e r t h a n , s a y , f ( x ) b e c a u s e t h ev a r i a b l e used t o d e n o t e t h e "input" i s i r r e l e v a n t .For example, i f fi s t h e r u l e w h i c h d o u b l e s a n u m b e r i t makes n o d i f f e r e n c e w h e t h e r wewrite f(x) 2x or f ( t ) 2t or f( ) 2 etc.T h i s i s why we o f t e n maker e m a r k s l i k e " D e f i n e f b y f ( t ) 2 t f o r a l l r e a l n u m b e r s , t . " Thep o i n t i s t h a t i t i s f w h i c h we a r e s t u d y i n g .**In many p r a c t i c a l c a s e s , o n e i s i n t e r e s t e d i n a s p e c i f i c d o m a i n , s a yI n t h e s e c a s e s , we o n l y r e q u i r e t h a t t h e d o m a i nthe interval [a,b].o f D i n c l u d e f u n c t i o n s w h i c h a r e a n a l y t i c on [ a , b ] .

Some Notes on S t r u c t u r eI n o r d i n a r y m u l t i p l i c a t i o n , w e a c c e p t w i t h l i t t l e i f any d i f f i c u l t yt h e n o t a t i o n t h a t an d e n o t e s t h e p r o d u c t of n f a c t o r s o fa.Thisn o t i o n i s extended t o any mathematical s t r u c t u r e i n t h a t w e o f t e n u s et h e exponent n o t a t i o n t o i n d i c a t e t h a t a c e r t a i n o p e r a t i o n i s b e i n gc a r r i e d o u t s u c c e s s i v e l y a c e r t a i n number of times.*One p l a c e t h a t t h i s n o t a t i o n i s used e x t e n s i v e l y i n mathematicala n a l y s i s i s when w e r e f e r t o composition of f u n c t i o n s .For example,suppose t h a t f i s a f u n c t i o n t h a t maps a s e t S i n t o i t s e l f . Then, f o r.a g i v e n SES, i t makes s e n s e t o t a l k a b o u t , s a y , f ( f ( f ( s ) ) )That i s ,s t a r t i n g w i t h s , w e compute f ( s ) . Then, s i n c e f ( s ) i s a g a i n i n S , w emay compute t h e e f f e c t of f on f ( s ) ; i . e .f ( f ( s ) ), etc.Pictorially,[Notice t h a t i t i s c r u c i a l t h a t t h e image o f f b e c o n t a i n e d i n S s i n c ei f f (sl) and t4tts,t h e n f (f (sl)) i s n o t d e f i n e d because f (f ( s l ) ) f ( t )domain of f .Again, p i c t o r i a l l y ,tts,dom f S f ( t )i s not defined*An i n t e r e s t i n g n o t e o n n o t a t i o n i s t h a t when we u s e r a t h e r t h a nx t o denote t h e o p e r a t i o n , i t i s conventional t o w r i t e na r a t h e r thannFor example, w i t h r e s p e c t t o o r d i n a r y a d d i t i o n , t o i n d i c a t e t h a ta a , we w r i t e n a y n o t a nwe w a n t a a .n termsI n o t h e r w o r d s , f o r any r e a l number a and a n y p o s i t i v e i n t e g e r n - na. d e n o t e s t h e sum a a.n times

In terms of specific illustration, let S be the set of integers and6S f(6) T 3.for each s&S. Then, E andNow,define f by f(s) f (f(6)) means f (3) and this is undefined if we insist that f :S S since3 & S.1f(3) 3- - - -In any event, as long as f:S S, we may talk meaningfully aboutof where foof means [foof1 (s) f(ff(s) .))fo.n timesn timesn times(.n timesAs an illustration, let S denote the set of all integers and define fon S by f(s) 2s 3 for each SES. Since 2s 3 is an integer if sis an integer, we have that f:S S. Now, for each SES, we havehence,hence, 8s 21, etc.For example,*Again, keep in mind the irrelevancy of the symbol used to denote the"input." f(s) 2s 3 means f([ I) 2 [ ] 3 s o that when[ I 2s 3, f([ I) 2[2s 31 3.

Rather than write, say, (f f (f (f(s)))), it is conventional to abbreviatethis by fn(s), where fn means foof-.n timesImportant NoteThis new notation is somewhat unfortunate since it now gives us twoentirely different meanings for the same symbol. Namely, we havepreviously used, say, f2 (x) to denote [f (x)l 2 and now we are saying2Clearly, If (x)I and f (f(x)) arethat f (x) could also mean f (f(XI)entirely different concepts. For example, if f(x) 2x 3, then[f(x)12 (2x 312 4x2 12x 9 while f(f(x)) f(2x 3) 2(2x 3) 4x 6. This same problem occurred as a special case whenwe first introduced f-l to denote the inverse of f in the sense thatfof-I f-1of identity function, i .e. [fof-11 (x) x for all x. In1this context, we saw that if f (x) 2x 3, then [f (x)] - 1 2x 3x - 3while f-I (x) 2.-Hopefully, whether fn(x) means [f (x)ln or whether it meansf1 )will be clear from context, but for the remainder off (f .C.4.-n timesthis chapter. fn ( x ) shall mean f (f. f (XI ) .) .n timesWith this discussion as background, we are now in a position todefine D2, D3. D4, etc. Namely, suppose f is in the domain of D.Then by definition of the domain of D, f possesses derivatives ofevery order. Since D(f) f', we see that f' also belongs to the domain of D (i.e. if f has derivatives of all orders, f' must also possess derivatives of all orders since the nth derivative of f' is the(n l)th derivative of f etc.Hence,Proceeding inductively, D" is defined by "( 1 f (n' ,

for each f E dom D. We may also define cD for any constant c.Namely, cD is defined by[cDl (f cD (f)We may now invoke the linear properties of D to define what we mean bya polynomial in D. In particular, if ao 1 al'and an are constantswe define anO" an-lDn-1 a1D .a to mean nn-1(f)anD (f) an-lD .,. a1D(f) aof The connection between this definition and our previous study of linear differential equations with constant coefficients should seemrather obvious. Specifically, if we replace f by y in ( 2 ) , we obtainNow certainly we would not have gone through all this discussion justto show that we can express linear differential equations in a newnotation which involves polynomials in D! What is really importantis that in terms of the new polynomial notation, there is a fantasticresemblance between polynomial properties and derivative properties.Rather than launch into an avalanche of formal proofs, let us beginwith a few concrete examples.Example #1Consider the expression* T h i s i s why we r e q u i r e t h a t f b e a n a l y t i c .e x i s t f o r each n .O t h e r w i s e f ( n ) need n o t

Using our new notation, (4) would be expressed as( D 4D-3)y.*If we were to look at D 40 - 3 as a "normal" polynomial in D, wewould be tempted to "factor" it by writingThe only problem is what do we mean bywhich we get by using (6) in (5).In terms of multiplication meaning composition of functions, a naturalinterpretation of (71 would be ( 2y) -- 3( y) d(*dx dx-**y)3 ( 2 - y).As a check that (4) and (8) are equivalent, notice that (8) may bewritten as* F o r b r e v i t y , i t i s c o n v e n t i o n a l t o w r i t e ( D 4D2[D 4 D - 31 ( y ) .**Notice2(D-that i f y is analytic, so also is2-y a s a s i m p l e f u n c t i o n ( s a y , u) a n d a p p l y D3 ) ( 2-y ) (D-3 ) u Du-3u (y.- 3)y r a t h e r thanT h u s , w e may v i e w- 3 t o u.- y) - 3-That i s ,y).

which is ( 4 ). 4D 3)y into (DIn other words, "factoring" ( D us specifically how the 2nd-order equation-may be viewed as the first order linear equation in3) (D( --1) showsy); namely,Example # 2Consider (D - 1) (D - 3)y which we obtain by permuting the "factors" of(D - 3) (D - 1)y. We obtainso thatand our multiplication is commutative.Example #3The property of commutativity requires that the coefficients of the"powers" of D be constants. For example,

(xD 1) (D - x)y (xD 1) (Dx - xy) xD(2-xy) (2- xy)On the other hand,Comparing (9) and (lo), we see that (xD 1) (D - X) # (D - x) (xD 11,and, moreover, neither (xD 1) (D - x) nor (D - x) (xD 1) is equalto the "usual" product X D (1 - x2 )D - x.In summary, this new arithmetic loses its nice structural appeal if wedo not restrict its usage to constant coefficients, and this stronglyaffects our ability to handle nicely linear equations with nonconstant coefficients.

In summary, then, if we introduce the notation of differential operators whereby we rewritewhere .a,., an-1 are constants asthenpossesses the same structure as does the "usual" polynomial arithmetic.In particular, if P1 (Dl , P2 (D), and P3 (Dl denote three polynomials inD with constant coefficients, it is true (but we omit any formalproofs ) that(i) P1 (DlP2 (Dl P2 (DlP1 (DlandThus, we may manipulate polynomials in D in the "usual" way, as illustrated in the following examples.Example # 4(Il2 2D 2) (D-1) D3 2D2 2D - D - 2D - 2I D Hence, we may view D -2.

and this in turn is(D2 2D 2)(D-1)y- (D2 2D (D2 2D 2)(2 - y)- D (dx-y(dx2- y)"2)(Dyy) 20( -- 2( which is second-order and linear iny) 2 ( % y). 2(2d - y).(2By commutativity, we may also rewrite (11) aswhich is first order and linear in (y" 2y' 2y).The main point is that by (12) and (13) we have thatis equivalent to either of the lower order equationswhere u y t-y, or-y)y)

where v y" 2y' 2y.Hopefully, this analysis supplies some insight as to how we solve linear differential equations, structurally, by reducing them to equivalent lower order equations.Example #5Suppose we want to solve the equationBy our "new" algebraHence, equation (14) is equivalent toy"' - 2y"-Letting yr3 erx-y' 2y 0.erx in (IS), we obtain2r2erx-rerx 2erx orx# 0, (16) implies thatand since eSince r3 - 2r2 - r 2 (reral solution of (15) is-1) (r 1) (r-2 ) , we see that the gen-The main observation here is that the "roots" of (14) are also 1, -1,and 2. More generally, using the D-notation, if the nth order homogeneous linear equation with constant coefficients can be representedin the "factored" form

(D-al)(D-a2).(D-an)y, where ai # aj if i # jthen the general solution of the equation is simplyExample # 6Sometimes the a's in (18) are not all distinct.tion concerns solving, sayAn interesting ques-Of course, we have learned to solve (19) by other methods.example, (19) is equivalent toForfor which the substitution y erx yieldsr3-3r2 3r-1 0, or (r-113 0whereupon.is the general solution of (19)To handle (19) by the method of differential operators, we have thestructural property thatWe may prove (20) by induction, observing that for nobtain*Mechanically,D by D m . ( 2 0 ) t e l l s u s t h a t we may " f a c t o r o u t " e1, 2, etc., wemxand r e p l a c e

-ern(% my) emx ( D m ) y emd (9 dxmydx mem9 (dxmy)mx [ ( D 2mD m2)yl e emx ( D m) 2y ,etc.and t h e i n d u c t i v e d e t a i l s a r e l e f t t o t h e i n t e r e s t e d r e a d e r .3R e t u r n i n g t o Example #6, s i n c e D (e-Xy) e-X (D(20) w i t h n 3 and m -11,w e have t h a t (D-t h a t is,S i n c e D3 (e-Xy) e-X(D-31) y , i t f o l l o w s t h a t-31) y [ i . e .this is31) y 0 i m p l i e s t h a t

whereupon we may integrate (21) successively to obtainIt is not our purpose here to teach the differential operator methodin detail. Our main aim for now is to help you get acclimated to thisnew language so that later, in Section D, we can show a very nice nontrivial application of this discussion to the fairly sophisticatedconcept of systems of linear differential equations. For this purpose,Section C may be omitted without any loss of continuity, but the moreinvolved reader may prefer to study Section C if only to gain a littlefurther insight to how the arithmetic of differential operators isfurther developed.Inverse Differential OperatorsGivenwe already know thatNamely, (1) nay be written aswhereupon an integrating factor of ( 3 ) is e-ax.we obtainsides of ( 3 ) by e'ax,Multiplying both

Hence,from which ( 2 ) f o l l o w s .On t h e o t h e r hand, suppose w e wanted t o s o l v e (1) " a l g e b r a i c a l l y "t r e a t i n g (D - a ) a s a " f a c t o r , " r a t h e r t h a n a s an o p e r a t o r , i n t h eexpression (D-a)y.We would " d i v i d e " b o t h s i d e s of(1) by D-a toobtainWhat w e have r e a l l y done i n o b t a i n i n g ( 4 ) from (1) i s t o have "com--(1) w i t h t h e i n v e r s e of t h e o p e r a t o r (Da ) . In11i s definedwhere (D - a )e f f e c t , we a r e w r i t i n g ( D - a )asposed" b o t h s i d e s of-by t h e r e l a t i o nThe p o i n t i s t h a t w e may now compare (4) [which w e would l i k e t o meant h e v a l u e of yl w i t h e q u a t i o n ( 2 )[which w e know i s t h e v a l u e of y (upt o an a r b i t r a r y c o n s t a n t 1 1 and conclude t h a t i f ( 4 ) i s going t o y i e l dIt h e s o l u t i o n of (1), t h e n we have no c h o i c e b u t t o d e f i n ef (XI ,or,(D-a)-' (XIbyD-a f ( x ) eaxJe-axf( x )dx.Example #1To e v a l u a t eyieldsx 4 , w e u s e ( 5 ) w i t h a 3 and f ( x ) x4.This

c an a r b i t r a r y , b u t f i x e d , c o n s t a n t ." I n v e r t i n g " ( 6 ) , w e a r e saying t h a tTo show t h a t ( 7 ) i s c o r r e c t , we could e v a l u a t eb u t t h i s i s n o t necessary f o r our purposes.r u l e and t h e f a c t t h a t dxiXe-3tt4dtNamely, by t h e productg ( t ) d t g (x) , we conclude t h a tX x4 Computing t h e l e f t s i d e ofexplicitly,3e3.le -3t. t 4d t .(7) and using ( 8 ) , w e have t h a t

which checks w i t h t h e r i g h t s i d e of(71,.Example # 2L e t us u s e i n v e r s e o p e r a t o r s t o s o l v eW e haveHence,I f we now u s e ( 5 ) w i t h a 6 and f ( x ) e5X, (10) becomes -e5X ce 6xA s a check of9dx -5e5X.( l l ) ,y -e5x ce6x i m p l i e s 6ce6X;whence,which a g r e e s w i t h ( 9 ).I n more advanced c o u r s e s , one p u r s u e s t h e i d e a of i n v e r s e d i f f e r e n t i a lo p e r a t o r s i n more c o m p u t a t i o n a l d e t a i l , b u t f o r o u r purpose of t r y i n gt o show how t h e d i f f e r e n t i a l o p e r a t o r n o t a t i o n i s used, t h e d i s c u s s i o ni n t h i s s e c t i o n should be s u f f i c i e n t .

In the next and final section, however, we shall present an application of differential operators in which we really reap the rewards ofthe structural similarity between differential-operator polynomialsand "ordinary" polynomials.Systems of EquationsIn the study of numerical algebra, the student begins by practicing onsingle equations with a single unknown. As he gains experience, hethen is exposed to the idea that in many real situations, there isoften more than a single variable with which he has to contend.An analogous situation prevails in the study of differential equations. We first learn to handle equations where we are dealing with asingle function of, say, t. We learn to solve such equations as2 *d dt dt29y sin t,etc. Now a natural extension of this problem occurs when we begin torealize that we may have an equation which involves two or more functions of t.Consider, for example, the equationwhere x and y are assumed to be functions of t.What do we mean by a solution of (I)? Obviously, we mean that we wantexplicit functions x (t) and y (t) which satisfy (1).Finding such solutions is, in a way, child's play. Namely, we maypick x or y arbitrarily and then solve (1) for the other. By way ofillustration, suppose we letin (1).In this case, (1) simplifies into

e-3t is an integrating factor of (31, so that (3) may be rewritten aswhereupon it follows thatx c e3tAs.a check, we may use (2) and 14) to show thatso thatisone family ofsolutions of (1).We may generalize our treatment of (1) by allowing y yo(t) to be any(integrable) function of t, whereupon (1) would becomeOnce yo(t) is specified, equation ( 5 ) is a linear first order differential equation in x, which may be solved by rewriting (5) as

whereuponObviously, t h e c h o r e of e x p r e s s i n g t h e i n t e g r a l on t h e r i g h t s i d e of( 6 ) depends s t r o n g l y on t h e c h o i c e of y o ( t ) , b u t what s h o u l d b e c l e a ri s t h a t (6) shows u s how t o d e t e r m i n e x a s a 1-parameter f a m i l y oncey y o ( t ) i s g i v e n s o t h a t w e o b t a i n a " g e n e r a l " s o l u t i o n of (1) f o reach c h o i c e of yo ( t ).Before c o n t i n u i n g f u r t h e r , n o t i c e how t h i s d i s c u s s i o n r e l a t e s t o o r d i nary algebra.When w e a s k f o rthes o l u t i o n of x y 7 , w e may p i c ky a r b i t r a r i l y and t h e n d e t e r m i n e x i n t e r m s of y . What happened h e r eThe samewas t h a t w e had an e x t r a d e g r e e of freedom t o " p l a y w i t h . "t h i n g happens i n o u r d i s c u s s i o n of e q u a t i o n (1). W e have two funct i o n s , b u t o n l y one e q u a t i o n . Thus, w e e x p e c t t o have a d e g r e e offreedom a t o u r d i s p o s a l .I n o t h e r words, g i v e n two f u n c t i o n s of t , w e e x p e c t t h a t w e need twod i f f e r e n t i a l e q u a t i o n s i n o r d e r t o d e t e r m i n e t h e two f u n c t i o n s .Suppose, t h e n , i n a d d i t i o n t o e q u a t i o n ( I ) , w e a r e t o l d t h a t o u r funct i o n s x ( t ) and y ( t ) must a l s o s a t i s f yThat i s , w e wish t o s o l v e t h e system of e q u a t i o n sS i n c e t h e theme of t h i s c h a p t e r is d i f f e r e n t i a l o p e r a t o r s , l e t u s re-w r i t e t h e g i v e n system i n t h i s form.Namely,

Since differential operators obey the same arithmetic as do polynomials, we suspect that we may be able to solve (8) by treating thecoefficients of x and y as polynomials and then eliminating variablesjust as we do in the algebraic case.For example, to eliminate y in (8), we "multiply" the first equationby (D - 3), the second equation by 6, and then add the two equations.Thus ,We now invoke the definition of the differential operator as well asits algebraic properties to rewrite (9) as

Equation (10) r e p r e s e n t s 9 s i n g l e e q u a t i o n w i t h "one unknowntt whichc a n b e s o l v e d e a s i l y by t h e method o f undetermined c o e f f i c i e n t s .Namely, t h e s o l u t i o n of t h e reduced e q u a t i o n i s x clsin 3 thC C O S 3 t and w e t h e n t r y f o r a p a r t i c u l a r s o l u t i o n ofx e P(10) i s t x c 1s i n 3 t (10) i n t h e formC t E , and w e o b t a i n t h a t t h e g e n e r a l s o l u t i o n ofc 2c o s 3 t et-5t2 2p 227 'S i m i l a r l y , w e can e l i m i n a t e x from ( 8 ) by m u l t i p l y i n g t h e f i r s t equat i o n by - D , t h e second by (D - 3) and

helpful to us in handling linear differential equations and systems of linear differential equations. These ideas will be discussed in the following sections. *It is conventional to write f rather than, say, f(x) because the variable used to denote the "input" is irrelevant. For example, if f

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