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148 VI. BOUNDARY-VALUE PROBLEMS

where b = t. Note that t = 0 is a regular singular point of (VI.1.8) and the indicial equation is 4s2 + 2s + A = 0 whose roots are s = - 2 f 4 - A. These roots are real if and only if A < 4 This verifies the claim. 0

Note that J

+00

dx

1 + x2

0

2*

The following theorem shows some structure of solutions in the case when

+00

ig(x)ldx < +oo.

0

Theorem VI-1-8. Let g(x) be a real-valued and continuous function on the inter-

f+C0

valA. If 1 jg(x)ldx < +oo, then there exist unbounded solutions of differential

0

equation (VI. 1. 1) on Ia.

Proof.

The assumption of this theorem and (VI.1.1) imply that

lim dq(x)

= -Y exists

 

:-+oo dx

 

for any bounded solution n(x) of (VI.1.1). If 7 0, then i(x) is unbounded. Hence,

lim odd) = 0. Therefore, calculating the Wronskian of two bounded solutions

z

of (VI.1.1), we find that those bounded solutions are linearly dependent on each other. This implies that there must be unbounded solutions. 0

Remark VI-1-9. Theorems VI-1-1 and VI-1-2 are also explained in ]CL, §1 of

Chapter 8, pp. 208-211] and [Hart, Chapter XI, pp. 322-403]. For details concern- ing other results in this section, see also [Cop2, Chapter 1, pp. 4-33] and [Be12,

Chapter 6, pp. 107-142].

VI-2. Sturm-Liouville problems

A Sturm-Liouville problem is a boundary-value problem

dd-x (p(x) Ly) + u(x)y = f (.T),

(BP)

y(a) cos a

-Ip(a)y'(a)sin or = 0,

 

y(b) cos Q - P(b)y(b) sin )3 = 0,

under the assumptions:

(i)the quantities a, b, a, and $ are real numbers such that a < b,

(ii)two functions u(x) and f (x) are real-valued and continuous on the interval

Z(a,b) = {x: a < x < b},

(iii)the function p(x) is real-valued and continuously differentiable, and p(x) > 0

on 1(a, b).

In this section, we explain some basic results concerning problem (BP).

2. STRUM-LIOUVILLE PROBLEMS

149

Let 4(x) and O(z) be two solutions of the homogeneous linear differential equation

(VI-2.1)

(p(x)A) + u()y = 0

 

-dx

 

such that

 

 

(VI.2.2)

m(a) = sins, p(a)d'(a) = cosa,

,p(b) = sin f3, p(b)t'(b) = cosfi,

respectively. Then, these two solutions satisfy the boundary conditions

(VI.2.3)

¢(a) cos a - p(a)4,'(a) sin a = 0,

i (b) cos /3 - p(b)0'(b) sin /3 = 0.

The two solutions 4(x) and /;(x) are linearly independent if and only if

(VI.2.4)

4(b) cos Q - p(b)©'(b) sin /3 # 0 or

'(a) cos a - p(a)rb'(a) sin a # 0.

The first basic result of this section is the following theorem, which concerns the existence and uniqueness of solution of (BP).

Theorem VI-2-1. If the two solutions 4(x) and ip(x) of (VI.2.1) are linearly independent, then problem (BP) has one and only one solutwn on the interval

I(a, b).

Proof

Using the method of variation of parameters (cf. Remark IV-7-2), write the general solution y(x) of the differential equation of (BP) and its derivative y'(x)

respectively in the following form:

(VI.2.5)

6

'j'(_)f (_)

 

VW = CIOW + C20 W + 4(x) J P(f)WW

4 +

Y' (X) = Clo'(x) + C21k'(x) + 0'(x) I

 

4

s

P(A)W

 

i,&(x)1= o(f)f

a

(x) J

A,

JJJu P(A)W V)

 

where cl and c2 are arbitrary constants and W (x) denotes the Wronskian of

Now, using (VI.2.3) and (VI.2.4), it can be shown that solution

(VI.2.5) satisfies the boundary conditions of (BP) if and only if cl = 0 and c2 =

0. 0

Observation VI-2-2. It can be shown easily that p(x)W(x) is independent of x.

Observation VI-2-3. Under the assumption that the two solutions 40(x) and tfi(x) of (VI.2.1) are linearly independent, the unique solution of (BP) is given by

rb

 

y(x) = d(x)

 

 

10(x) I (- ))- W(f )

(VI.2.6)

Jx P(A)W (O

 

 

 

i

 

Y 'W = O(x)

rb owfwdC + V,'(x) r= 4(W W 4.

 

1r

W

Ja P(OW (O

150 VI. BOUNDARY-VALUE PROBLEMS

Setting

 

 

4(x)1()

if

x

< C <b,

(VI.2.7)

G(x, ) =

p(OW (c)

 

 

 

O WOW

 

a

< t < x,

 

 

if

 

 

p(f)W(c)

 

 

 

we can write (VI.2.6) in the form

 

 

 

 

b

 

 

J

b aG

 

y(x) = J G(x, )f

 

8x (x, Of (Ode.

 

 

 

y '(x) =

 

The function G(x,l;) is called Green's function of problem (BP). The following theorem gives the characterization of Green's function.

Theorem VI-2-4. The function G(x, C) given by (VI. 2.7) satisfies the following conditions:

(i) G(x, l:) is continuous with respect to (x, e) on the region D = {(x,) a < x < b, a< £<b},

(ii) 8 (x, l:) is continuous with respect to (x, C) on the region D -

a <

C < b},

 

 

(iii) at ({, l;), we have

 

 

8 (tr + 0. 0 -

for a < < b,

 

( - 0, 0 = p(0

 

(iv)as a function of x, G(x, l:) satisfies homogeneous linear differential equation

(VI. 2. 1) if x 0 4,

(v)as a function of x, G(x, 4) satisfies the boundary conditions of (BP), i. e.,

G(b,Z:)cosf3-p(b)8G(b,{)sinf3=0

for a:5 < b.

Furthermore, the function G(x, f) is uniquely determined by these five conditions.

Proof.

It is evident that the function G(x, l;) satisfies these five conditions. Suppose H(x,t) satisfies the five conditions. Conditions (iv) and (v) imply that

Cl(l;)4(x) for

{ C2(t;)V(x)

for

a < x < l;,

{ < x < b

for (x,l;') E D, where Ci(1;) and C2(C) must be determined by conditions (i), (ii),

and (iii). This means that C,({) and

must be determined by

0 and

-PW

2. STRUM-LIOUVILLE PROBLEMS

151

OW

4(f)

Since {(x,e) : a < x < }

This yields Cl(a;) = p(OW(O and C2({) =

p(OW(O

-

-

x<t<b}and {(x,t): 1;<x< b}{(x,£): a<t<x}for

(x, ) E V, we obtain H(x,1;) = G(x, l;). 0

The second basic result co//ncerns self-adjointness of problem (BP). Define a dif-

ferential operator L[y] _

(p(x)

I + u(z)y and a vector space V(a, b) over the

real number field 1R by

\

/

V(a, b) _ { f r C2(a, b) : f (a) cos a - p(a) f'(a)sin a = 0, f(b)cos5 - p(b)f'(b) sin,3 = 01,

where C2(a, b) denotes the set of all real-valued functions which are twice contin- uously differentiable on the interval I(a, b) = {x : a < x < b). Define also an inner product (f, g) for two real-valued continuous functions f and g on I(a, b) by

(f,9) = f

Since

a

 

 

 

(())

4

(f, 4191) =

J6f() [

+

 

= p(b)f (b)9 (b) - p(a)f (a)9'(a) + fb

dl;

 

 

a

 

for f E V(a, b) and g E V(a, b), we obtain

(f,L[g) - (L(f1,9)

={p(b)f(b)9'(b) - p(b)g(b)f'(b)} - {p(a)f(a)9 (a) - p(a)9(a)f'(a)}.

Also, since

(

f (a) cos a - p(a)f'(a) sin a = 0,

f (b) cos Q - p(b) f'(b) sin O= 0,

t

9(a) cos a - p(a)9'(a) sin a = 0,

g(b) cos, - p(6)9'(b) sin /3 = 0

for f E V(a. b) and g E V(a, b), we obtain

 

p(a)f(a)9'(a) - p(a)g(a)f(a) = 0,

p(b)f(b)9'(b) - p(b)g(b)f(b) = 0.

Thus, we proved the following theorem.

Theorem VI-2-5 (self-adjointness). The operator L has the following property:

(f, 0191) = (L(f], 9)

for

f E V (a, b) and g E V(a, b).

152

VI. BOUNDARY-VALUE PROBLEMS

Observation VI-2-6. In Theorem VI.2.1, it was assumed that the two solutions ¢(x) and '(x) are linearly independent. Consider the case when this assumption is not satisfied. So, assume that ¢(x) and ?P(x) are linearly dependent. This means that

0(a) cos a - p(a)0'(a) sin a = 0

and

¢(b) cos ji - p(b)5'(b) sin fi = 0.

In other words,

 

 

 

(VI.2.8)

lr[o) = 0

and

0 E V(a, b).

The boundary-value problem (BP) can be written in the form

(VI.2.9)

G[yl = f

and

y E V(a, b).

Using (VI.2.8) and (VI.2.9), we obtain

 

(f, 0) = (C [y], 0) = (y, x[01) = 0,

if there exists a solution y of problem (VI.2.9). The converse is also true, as shown in the following theorem.

Theorem VI-2-7. Assume that O(x) satisfies condition (VI.2.8). Then, if a real- valued continuous function f (x) on T (a, b) satisfies the condition

(VI.2.10)

(f. 0) = 01

problem (BP) has solutions depending on an arbitrary constant.

Proof.

Using the method of variation of parameters, write the general solution y(x) of the differential equation of (BP) and its derivative y(x) respectively in the following form:

(VI.2.11)

 

b

+ (x)J __

11

y(x) = cjW(x) + c2p(X) + 0(x)j

 

P(A)W f )

o P(A)W (E)

?% (z) =

J p _ {

+ F' (r)

1-v _),

 

r P(f)ww

u

P(t)

where u(x) is a solution of the linear homogeneous differential equation (VI.2.1) such that 0 and p are linearly independent, two quantities ca and c2 are arbitrary constants, and W(x) denotes the Wronskian of {0(x),p(x)}. Note that p(x)W(z) is independent of x and that

(VI.2.12)

p(a)cosa-p(a)u'(a)sina,-40, p(b)cosQ-p(b)p'(b)sinfl,40.

From (VI.2.10) and (VI.2.11), we derive

 

 

 

 

y(a) = ctm(a) + c2p(a) + 0(a) J

b

 

 

 

 

 

 

c P(4)W(E)

 

y'(a) = ca0'(a) + c2 (a) + 0'(a)

r°

A,

 

a

-N)

 

 

 

 

y(b) = ciO(b) + c2p(b),

y'(b) = c,O'(b) + c2p'(b)

The condition that y E V(a,b) and (VI.2.12) imply that ca is arbitrary and c2 =

0. 0

3. EIGENVALUE PROBLEMS

153

Remark VI-2-8. The materials of this section are also found in (CL, Chapters 7 and 11] and [Har2, Chapter XI].

VI-3. Eigenvalue problems

In this section, we consider the eigenvalue problem

(P(x) dx ) + u(x)y = Ay,

(EP)

y(a)coso - p(a)y'(a)sina = 0,

 

 

y(b) cos /3 - p(b)y'(b) sin /3 = 0,

under the assumptions:

(i) the quantities a, b, a, and 0 are real numbers such that a < b,

(ii) u(x) is a real-valued and continuous function on the interval Z(a, b) = {x :

a<x<b},

(iii) the function p(x) is real-valued and continuously differentiable, and p(x) > 0 on I(a, b).

The quantity A is the eigenvalue parameter.

Let 6(x,,\) and ti(x, A) be two solutions of the homogeneous linear differential equation

(VI.3.1)

 

(px) + u(x)y = Ay

such that

 

 

 

(VI.3.2)

{

¢(a, A) = sin a,

p(a)4'(a, A) = cos a,

,O(b, A) = sin /3,

p(b)t,V(b, A) = cos f3,

 

 

respectively. Then,

-O(a, A) cos a - p(a)6'(a, A) sin a = 0,

(VI.3.3)

tp(b, A) cos /3 - p(b) 0'(b, A) sin /3 = 0.

These two solutions 6(x, A) and tp(x, A) are analytic in A everywhere in C. Also, they are linearly independent if and only if

(VI.3.4)

f

0(b, A) cos (3 - p(b)¢'(b, A) sin /3

i4 0

or

t'(a,A)cosa - p(a)ty'(a,A)sina # 0.

 

 

 

 

Therefore, we obtain the following result.

Theorem VI-3-1. In order that A be an eigenvalue of (EP), it is necessary and sufficient OW ,\ satisfies the equation

(VI.3.5)

¢(b, A) cos i3 - p(b)cp'(b, A) sin 0 = 0

or, equivalently,

+'(a, A) cos a - p(a)0'(a, A) sin a = 0.

154

VI. BOUNDARY-VALUE PROBLEMS

Observation VI-3-2. All roots of (VI.3.5) are simple, since, if A is a root of

(VI.3.5), we can prove

80(b, A)

cos j3 - P(b)

8¢'(b, A)sun f # 0

8A

 

8A

in the following way. Let A be a root of (VI.3.5). Then, notice that z = 84(x, A)

8A

is a solution of the differential equation

CP(x)L1 + u(x)z = Az + ¢(x,A).

This implies that

(VI.3.6)

r_

 

 

Z(X) = c16(x, A) + c2p(x) - O(x, A)

A) dC + p(x) f =

' , A)2 de,

J

Ja P(O1't'(O

 

1 n

z'(x) = clOx, A) + C21L (x) - 4'(x, A) f pW¢(f, A)dC +

p '(x) j

= w(), A)2

 

PwW (f)

P(O-N) dd,

where p(x) is a solution of homogeneous linear differential equation (VI.3.1) such that 4(x, A) and p(x) are linearly independent, two quantities ct and c2 are constants, and W(x) denotes the Wronskian of {¢(x,A),p(x)}. Note that p(x)W(x) is independent of x and that

(VI.3.7) p(a) cos a - p(a)p'(a) sin a 0, p(b) cos,3 - p(b)1 (b) sin Q # 0.

Formulas (VI.3.6) imply that

(VI.3.8)

z(a) = clo(a,A) + c2p(a), z'(a) = ci4'(a,A) + c2,u (a),

z(b) = cj¢(b, A) + c2p(b) - 4(b, A)

 

fb

 

p(b)

Jn

 

Pwww

z'(b) = c1 ¢'(b, A) + c2p'(b) - 0'(b.,\) j

w

+ p'(b)rP(u)W

 

o P(4)W (0

Since (VI.3.3) is true for all values of A, it follows that z(a) cos a - p(a)z(a) sin a

0. Hence, from (VI.3.7) and (VI.3.8), we conclude that c2 = 0. Therefore,

z(b) cos

cos$

- P(b)

(b) sin 0) ° 0(Td

# 0.

0

 

- P(b) z'(b) sin,3 = (,u(b)

Ia a P(A)W w

 

 

 

 

 

 

 

Remark VI-3-3. If A = 0 is not an eigenvalue of (EP), we can define Green's function G(x,t) of problem (BP of §V-2 so that (EP) is changed equivalently to

the integral equation y(x) = A

G(x,

To prove that all eigenvalues of (EP) are real, it is convenient to extend Theorem VI-2-5 (self-adjointness) to complex-valued functions f and g. Define a differential

3. EIGENVALUE PROBLEMS

155

operator C[y] = ((x)) + u(x)y and a vector space U(a, b) over the complex

number field C by

U(a,b) _ If E C2 (a, b; C) : f (a) cos a - p(a) f'(a)sin a = 0,

f (b) cos a - p(b) f'(b) sin,3 = 0},

where C2(a, b; C) denotes the set of all complex-valued functions which are twice continuously differentiable on the interval I(a, b) = {x : a < x < b}. Also, define an inner product (f, g) for two complex-valued continuous functions f and g on 2(a, b) by

b

(f, 9) = Jn f (09(041

where g(1;) denotes the complex conjugate of g(f ). Since

b

 

(f,'CWi) = 1f

\p(e) <J + u(C)9(C)] dC

a

 

= P(b)f(b)9'(b) - p(a)f(a)9'(a) + e [-Pwfv)9'(o + uh)fw9(-j <'

J

for f E U(a, b) and g E U(a, b), we obtain

(f, C(91) - (C[f ], 9)

= {p(b)f(b)9'(b) - p(b)9(b)f'(b)} - {p(a)f(a)g(a) - p(a)9(a)f'(a)}.

Also, since

f (a) cos a - p(a) f'(a) sin a = 0,

f (b) cos Q - p(b)f'(b) sin /3 = 0,

. 9(a) cos a - p(a)9'(a)sin a = 0,

9(b) cosQ - p(b)91(b) sin p = 0

for f E U(a,b) and g E U(a,b), we obtain

 

p(a)f(a)9'(a) - p(a)9(a)f'(a) = 0,

p(b)f(b)9'(b) - p(b)9(b)f'(b) = 0.

Thus, we extended Theorem VI-2-5 as follows.

Theorem VI-3-4 (self-adjointness). The operator C has the following property:

(f, C[9]) = (C[f], 9)

for

f E U(a, b) and g E U(a, b).

Theorem VI-3-4 implies the following conclusion.

156

VI. BOUNDARY-VALUE PROBLEMS

Theorem VI-3-5. All eigenvalues of (EP) are meal.

Proof.

Let A be an eigenvalue of (EP) and let y(x) be an eigenfunction corresponding to A. We may assume that (y, y) = 1. Then,

(y,Cjy]) = (y, Ay) = X(y,y) = X,

(hjyl,y) = (Ay,y) = A(yy) = A,

and Theorem VI-3-4 imply that J = A. 0

In order to explain distribution of eigenvalues on the real line IR, look at the basic comparison theorem (Theorem VI-1-1) more closely. Let us rewrite the differential equation

(VI.3.9)

(P(X) dy) + g(x)y = 0

in the form

p(x) = (1 - p(x)g(x))rsin(O)cos(9)

and

(VI.3.10) p(x)dO = I + (p(x)g(x) - 1) sin2(a)

by setting

y = r sin(O), p(x) Li = r cos(B).

The right-hand side of (VI.3.10) is independent of r. Therefore, (VI.3.10) is a first- order nonlinear differential equation on 0. Our main concern is the behavior of solutions of (VI.3.10).

Remark VI-3-6. Set w = ! ((x) L) . Then, differential equation (VI.3.9) be-

comes p(x) dx + w2 + p(x)g(x) = 0. This equation is further changed to (VI.3.10)

by the transformation w = cot(8).

Remark VI-3-7. If the function g(x) is continuous on the interval 2(a, b), then every solution 0(x) of (VI.3.10) exists on T(a,b).

Now, we prove the following basic lemma.

Lemma VI-3-8. Assume that

(1) four functions gl(x), g2(x), pi (x), and p2(x) are continuous on the interval

2(a, b),

(2) 92(x) ? gi(x) and pi(x) ? P2(x) > 0 on T(a,b),

(3) 01(x) (j = 1,2) are solutions of the differential equations

Pi (x) !

= 1 + [pi (x)gg (x) - 1J sin2(01)

(j = 1, 2),

 

 

 

3. EIGENVALUE PROBLEMS

157

respectively.

 

 

 

 

 

Then,

 

 

 

 

 

02(x) > 61(x)

on I(a,b)

 

if 02(a) > 01(a).

Proof.

 

 

 

 

 

Set

 

 

 

 

 

 

 

9(x) - 1

stn2(02) - sin2(0)

(1x,61,62()1p()

 

 

l

 

 

/ l

 

02

01

 

 

 

 

1

WS2(02)

h(x,02) _ (92(x) - 91(x))Sin2(62) +

 

P2(x)

1

 

 

 

 

P1 (x)

Then, the function w(x) = 02(x) - 01(x) satisfies the differential equation

dw - A(x,01(x),02(x)) w =

h(x,02(x)) > 0.

dx

 

 

 

 

-

Therefore,

 

 

 

 

 

w(x)eXP L-Ja

r

I

 

 

 

w(a) +

 

 

 

ds > 0

x h(s,02(s))eXP [- f

 

 

Ja

 

 

 

 

on T(a, b). 0

Remark VI-3-9. The proof given above also showed that if pi (x) > p2(x) > 0 on

Z(a, b), then we obtain

(a) 02(x) > 61(x) on I(a,b) if 02(a) > 01(a),

02(x) > 01(x) for a < x < b if 02(a) > 01(a) and g2(x) > g1(x) on a < x < b, ( y) in the case when g2(x) > g1(x) on a < x < b, if 01(a) = 0 and 61(b) = 7r and

if 0<02(a)<rr,then 02(b)>a.

Also, y=rsin(0)>0 if and only if 0<0<r(mod 2rr)and p(x) = 1 > 0 at

0 = 0 (mod jr). Theorem VI-1-1 follows from (y).

Setting 9(x,,\) = u(x) - A, apply Lemma VI-3-8 to problem (EP).

Lemma VI-3-10. Let 0(x, A) be the unique solution to the initial-value problem

Ax)

= 1 + (P(x)(u(x) - A) - 1)sin2(0),

0(a,A) = a

on the interval Z(a, b), where u(x) is continuous on Z(a, b), p(x) is continuous and positive on I(a, b), A is a real parameter, and at is a fixed real number such that 0 < a < rr. Then, for every c E 2(a, b) such that c > a,

(i) 0(c, A) is a continuous and strictly decreasing function of A for -oo < A <

+00,

(ii)lira 0(c, A) = +oo,

a

lim 0(c, A) = 0.

(iii)

A

+00

Proof.

 

We prove this lemma in three steps.