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Linear, Degenerate BSPDEs In the case that 2.6 holds, we use the following estimate: 5.21 fit.. [] w Comparison Theorems In this section, we are going to present some comparison theore

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130 Chapter 5 Linear, Degenerate BSPDEs

In the case that (2.6) holds, we use the following estimate:

(5.21)

fit ((O~-Z BT)D(OZu), BT D(O~u) ) dx

for small enough e > 0 to get

(5.22)

/ R ~ {((A - BBT)D(O~u), D(a~u) )

+ 2 ~ C, z ((O~-ZBT)D(Oeu),BTD(O~u))

o < ~ < a

> ~o/~

_ -~ ((A - BBT)D(O~u), D(O~u) ) dx - Clul~

Then, we still have (5.14) and finally have (5.20) which is the same as (4.1)

In the case (2.7) holds, we use the following estimate:

(5.23)

it ( ( O~-Z BT)D(OZu), BT D(O~u) ) dx

= fitJ(O"- Br)D(O u), c9~-a[BrD(Oau)]

- (O~-5BT)D(O~u)) dx

= - fit { ((02(=-~)BT)D(O/3u)' BTD(O~u) )

+ ((O(~-~)BT)D(O~u), BTD(OZu) ) + I(O~-aBT)D(OZu)I 2 } dx

for c > 0 small enough to obtain (5.22) and finally to obtain (5.20) Note that in the case (2.6) or (2.7) holds, we have (2.10) Then, (4.2) follows from (4.1) easily Finally, if in addition, (1.9) also holds, then, (4.3) follows from (4.2) This completes the proof of Lemma 4.1 []

w Comparison Theorems

In this section, we are going to present some comparison theorems on the solutions of different BSPDEs For convenience, we consider BSPDEs of

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w Comparison theorems 131 form (1.5) Let us denote (compare (3.1))

i s ltr[ADeu] - (a, D u ) - c u

A/[q A_ tr [BT Dq] - ( b, q ),

(6 1)

s ~ l t r [AD2~] - ( ~, DE) -Uu,

- - A ' -T

Mq=tr[B D ~ ] - ( b , ~ )

We assume that (H),~ holds for {A, B, a, b, c] and {A, B, ~, b, U] Consider the following BSPDEs:

I du = - { s + Mq + f }dt + < q'dW(t) )' (t,x) e [O,T] x ]1% n, (6.2)

f d-~= -{-s + M ~ +-]}dt + (~,dW(t) ), (t,x) E [0,T] x M% n,

(6.3) [ult=T = #"

Note that (6.2) and (3.2) are a little differenl since the operators s and J~4 are defined a little differently However, by the discussion at the end

of w we know that Theorems 2.1, 2.2 and 2.3 hold for (6.1) Throughout this section, we assume that the parabolicity condition (1.6), the symmetry condition (2.2) and (H),~ (for some m _> 1) hold for (6.2) and (6.3) Then

by Theorem 2.3, for any pairs (f, g) and (f, ~) satisfying (2.14), there exist unique adapted weak solutions (u, q) and (~, ~) to (6.2) and (6.3), respec- tively We hope to establish some comparisons between u and ~ in various

cases

Our comparison results are all based on the following lemma

L e m m a 6.1 Let (1.6), (2.2) and (H)m with m > 1 hold Let (u,q)

be the unique adapted weak solution of (6.2) corresponding to some (f, g) satisfying (2.14) for some A ~_ O Then there exists a constant # 6 ~, such that

E e lu(t, x)- 12, x

(6.4)

T

Proof We first assume that (f,g) satisfies (2.14) with A = 0 L e t : IR -+ [0, oc) be defined as follows:

(6.5) qo(r) = (6r 3 + 8 r 4 + 3r5) 2, 1 < r < 0,

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132

We can directly check that ~ is C 2 and

~(0) = / ( 0 ) = / ' ( 0 ) = O, (6.6)

~o(-1) = 1, ~o'(-1) = - Z , qo"(-1) = 2

Next, for any e > 0, we let ~o~(r) = e2~o(r) Then, it holds

lim ~'e (r) = - 2 r -

l i m ~ ( r ) = Ir i2, ~-~o

r

(6.7) J ' ( r ) l < C, Ve > o, r c IR;

lim ~ " ( r ) = ~ 2, r < O,

s-+O [ O, r > O

Denote

1

T h e n by (1.3), we have

Chapter 5 Linear, Degenerate BSPDEs

a = b - V - B

uniformly,

E i R ~e(g(x))dx- E s ~e(u(t,x))dx

= E {V'e(u) [ - ~ V.(ADu) - V-(Bq) - (a, Du )

t

- e u - ( g , q ) - f ] + ~o;'(u)lql=}dxds

= E s { ( ADu, Du) +2 ( BrDu, q) +iq,2 ]

- ~o'e (u)[ (a, Du ) +cu + ('b, q) + f ] }dxds : E iQ, {~ ~~ ( ( A - BBT)Du'Du)+]BTDu +q-~ul2]

1 u

+ 7 ~ ( ~ ) [ - I ~ 1 ~ ~ + 2 ( B ~ D ~ , ~ ) +2 ( ~ , q ) ]

- ( "d, Dg~e (u)) -~'~ (u)[cu + ( b, q } + f ] } dxds

_ < 7~o (~)l'gl2u= + (Bb, D ~oy(r)rdr)

+ [~"(~)~ -/~(u)} (~, q) +(v a)~(u)

- ~o'E(u)[cu + f]}dxds

(6.10)

(6.9) { ltr[AD2u]+(a, D u ) = ~V.[ADu]+('d, Du),

tr[BTDq] + (b,q) = V.(Bq) + (b,q}

Applying the It6's formula to ~o~ (u), we obtain (let Qt = [t, T] x IR n)

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w Comparison theorems 133

We note that

(6.11)

and

fo ~ 99~ (r)rdr = ~ (u)u - (p~ (u),

(6.12) l i m [ ~ ( u ) u - ~ ( u ) ] = 2uI(._<o) + 2 u - = 0

e - + 0 Thus, let e + O in (6.10), we obtain

(6.13)

E /R I g ( x ) - i ~ d x - E /R lu(t,x)-12dxds

> E/Q~ { - I(u<<_o)lbl2n ' - V ( B b ) [ - 2 u - u - lu-I 2]

+ (v.a)lu-I 2 + 2 u - [ ~ + f]}dxds

where

A (6.14) I t = s u p [ - V ~ + V ( B b ) + Ib[' + 2 c + 1 ] < c o

t~X,~O Then by Gronwall's inequality, we obtain (6.4) for the case )~ = 0 The general case can be proved by using transformation (2.11) and working on

Our main comparison result is the following

T h e o r e m 6.2 Let (1.6), (2.2) and (H),~ hold for (6.2) and (6.3) Let

(f,g) and (f,~) satisfy (2.14) with some ~ >_ O Let (u,q) and (~,~) be

adapted strong solutions of (6.2) and (6.3), respectively

# > 0 ,

(6.15)

E / R ~ e -~ (~)[[u(t, x) - g(t, x)]-12dx

< e"(~-*)E/~o e-~ ('>l[g(~) - Y(~)]-I :d~

+ ( M - M)~(s, x) + f(s, x) - ] ( s , x)]-[2dxds,

v t e [0, T],

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134

In the case that

Chapter 5 Linear, Degenerate BSPDEs

g(x) - F(x) > 0, Vz ~ ~t", a.s

(6.16) (s - Z)~(t, x) + ( M - M ) ~ ( t , x) + f ( t , x) - f ( t , x) >_ O,

V(t, z) ~ [0, T] x IR n, a.s

it holds

(6.17) u(t, x) >_ ~(t, x), V(t, x) E [0, T] x ~ n , a.s

This is the case, in particular, if s = s M = ,44 and

(6.18) ~ g(x) >_ -~(x),_ a.e x E ]R n, a.s

L f ( t , x) _ f ( t , x), a.e (t, ~) ~ [o, T] • ~ , a.s

Proof It is clear that

{ d ( u - ~ ) - - { Z : ( u - ~) + M ( q - ~)

(6.19) + (s - -~)~ + (2vf - M ) ~ + f - ] } d t

+ ( q - ~, d W ( t ) ),

Then, (6.15) follows from (6.4) In the case (6.16) holds, (6.15) becomes (6.20) EfR e-~(*>i[u(t,x) ~(t,z)]-12dz<_O, Vt E [0, T] This yields (6.17) The last conclusion is clear

C o r o l l a r y 6.3 Let the condition of Lemma 6.1 hold Let

I g(x) >_ 0, a.e x E Rn, a.s

(6.21)

f ( t , x) > O, a.e (t, x) E [0, T] x ~'~, a.s

and let (u, q) be an adapted strong solution of (6.2) Then

(6.22) u(t, x) > 0, a.e (t, x) E [0, T] x l& '~, a.s

[]

Proof We t a k e Z = s M = A4, f _ = 0 a n d y - 0 Then (~,~) = (0,0) is the unique adapted classical solution of (6.3) and (6.18) holds

Let us make an observation on Theorem 6.2 Suppose (~,~) is an adapted strong solution of (6.3) Then (6.16) gives a condition on A, B,

a, b, c, f and g, such that the solution (u, q) of the equation (6.2) satisfies (6.17) This has a very interesting interpretation (see Chapter 8) We now look at the cases that condition (6.16) holds

L e m m a 6.4 Let A, B, -d, b and -~ be independent of x Let -] and -~ be convex in x Let (~,~) be a strong solution of (3.1) Then, ~ is convex in

x almost surely

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w Comparison theorems 135

Proof First, we assume t h a t f and g are smooth enough in x Then, the corresponding solution (~,-9) is smooth enough in x Now, for any

9 ~ n , we define

v(t,x) = ( D2~(t, xfihT1);

p(t,x) = ( p l ( t , x ) , " " ,pd(t,x)), V(t,x) 9 [O,T] x IR ~, a.s

p k ( t , x ) = ( D 2 ~ k(t,xfi?,~), l < k < d ,

Then, it holds

dv = [ s - -Mp - ((D2-f)rI,~)]dt + (p, dW(t) ),

(6.23) v]t: T = ((D2~)~/' ~/)

By Corollary 6.3 and the convexity of f and g (in x), we obtain

( D2~(t, x)r/, r/> = v(t, x) >_ O,

(6.24) V(t, x) e [0, T] x Rn, y 9 ~tn, a.s

This implies the convexity of ~(t, x) in x almost surely In the case t h a t and ~ are not necessarily smooth enough, we may make approximation

[]

P r o p o s i t i o n 6.5 Let A, B, -5, b and -~ be independent of x Let f and

be convex in x and nonnegative Let (~,~) be a strong solution of (6.3)

Let A4 = A/[ and let

A(t,x) = A(t) + Ao(t,x),

(6.25) c(t,x) = -5(t) + co(t,x), (t,x) 9 [0, T] x IR ~, a.s

f ( t , x ) = f ( t , x ) + fo(t,x),

with

Ao(t,x)>_O, co(t,x)>_0, V(t,x) e [ O , T ] • n, a.s (6.26) fo(t,x) > O, go(x) >_ O,

Then (6.16) is satisfied and thus (6.17) holds

Thus,

(E - s x) = ~tr [AoD2~] + c0~ > 0

Next, we have the following

P r o p o s i t i o n 6.6 Let all the functions A, B, -5, b, -~, -] and -9 be determin- istic Let ~ be the solution of the following equation:

~t = - Z u - 7, (t, x) 9 [0, T] x IR n, (6.27)

(, ~l~=T = -9

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136 Chapter 5 Linear, Degenerate BSPDEs

Further, we assume that g(t, x) is convex in x Next, let (6.25) hold Then (6.16) is satisfied and (6.17) holds

Proof In the present case, (g, 0) is an adapted strong solution of (6.3)

T h e n similar to the proof of Proposition 6.5 and note ~ = 0, we can obtain

Note that in Proposition 6.6, B and b are arbitrary

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C h a p t e r 6

M e t h o d o f C o n t i n u a t i o n

In this chapter, we consider the solvability of the following FBSDE which

is the same as (3.16) of Chapter 1 (We rewrite here for convenience):

dX(t) = b(t, X(t), Y(t), Z(t))dt + a(t, X(t), Y(t), Z(t))dW(t),

(0.1) dY(t) = h(t, X(t), Y(t), Z(t))dt + Z(t)dW(t),

x ( o ) = x, Y ( T ) = g ( X ( T ) )

Here, functions b, a, h and g are allowed to be random, i.e., they can depend

on w E ~ For the notational simplicity, we have suppressed w and we will

do so below

We have seen t h a t for the case when all the coefficients are determin- istic, one can use the Four Step Scheme to approach the problem (see Chapter 4), which involving the study of parabolic systems; in the case of random coefficients, in applying the Four Step Scheme, we need to study the solvability of BSPDEs (see Chapter 5) In this chapter, we are going

to introduce a completely different method to approach the solvability of (0.1) Such a method is called the method o/ continuation

w T h e B r i d g e

Recall t h a t S '~ is the set of all (n • n) symmetric matrices In what follows, whenever A is a square matrix, (with A being a scalar), by A + A, we mean

A + M For any A E S n, by A >_ 5, we mean t h a t A - 5 is positive semidefinite The meaning of A _< - 5 is similar For simplicity of notation,

we will denote M = ~'~ x ][:~m X ~:~m• a generic point in M is denoted

by 0 = ( x , y , z ) with x C ]R '~, y E IR m and z E ]R "~• The norm in M is defined by

(1.1) 101 ~ {Ix12 + lYl 2 + Izl~} 1/=, VO = ( x , y , z ) 9 M ,

where Izl 2 ~ tr (zzT) Similarly, we will use 0 = (X, ]I, Z), and so on Now, let T > 0 be fixed and let

H[0, T] =L~:(0, T; WI'~ M ; ~ • ]R ~• • ~ m ) )

(1.2)

• L~(a; W I , ~ ( ~ ; ~ ) )

Any generic element in H[0, T] is denoted by F =- (b, a, h, g) Thus, F - (b, a, h, g) 9 H[0, T] if and only if

b E L~(O,T; W I ' ~ ( M ; I R n ) ) ,

a E L2_r(O,T;WI'~176215

h E L2(0, T; WL~176

g e n~%(~; Wl'~

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138 Chapter 6 Method of Continuation where the space L~(0, T; WI,~(M; ~'~)), etc are defined as in Chapter 1,

w Further, we let

(1.3) ~/[0, T] = n~(0, T; ]R ~) x n3:(0 , T; R )

2 m

x n~:(0, T; ~ m ) x n~- r (s ~ )

An element in ~[0, T] is denoted by 7 - (bo, ao, ho, go) with

bo 9 L~(0, T; R~),

ao 9 L~(0, T; ~nxd),

ho 9 L~(0, T; ~m),

go 9 L ~ r (~t; ~m)

We note that the range of the elements in H[0, T] and ~[0, T] are all in

~ n x ~ n x d x ~ m x ~ m Hence, for any F = (b,a,h,g) E H[0, T] and

7 = (bo, ao, ho,go) E ~/[0, T], we can naturally define

(1.4) F + ~ / = ( b + b o , ~ + a o , h + h o , g + g o ) E H[0, T]

Now, for any F - (b, a, h, g) C H[0, T], 7 - (b0, Cro, ho, go) E 7/[0, T] and x E ~ n , we associate them with the following F B S D E on [0, T]:

dX(t) = {b(t, O(t)) + bo(t)}dt + {a(t, O(t)) + ao(t)}dW(t),

(1.5)r,~,~ dY(t) = {h(t, O(t)) + ho(t)}dt + Z(t)dW(t),

x(0) = z , Y ( T ) = g ( X ( T ) ) + go,

with O(t) -= (X(t), Y(t), Z(t)) In what follows, sometimes, we will simply identify the FBSDEs (1.5)r,~,~ with (F, 7, x) or even with F (since 7 and x are not essential in some sense) Let us recall the following definition

D e f i n i t i o n 1.1 A process 0(-) - (X(.),Y(.),Z(.)) E M[0, T] is called

an adapted solution of (1.5)r,~,~, if the following holds for any t C [0, T], almost surely

~0 t X(t) = x + {b(t, O(s)) + bo(s)}ds

Y(t) = g(X(T)) + go - I t {h(t, O(s)) + ho(s)}ds

T

.It

When (1.5)r,~,~ admits a unique adapted solution, we say that (1.5)r,~,~ is

(uniquely) solvable

We see that (1.6)r,~,~ is the integral form of (1.5)r,~,~ In what follows,

we will not distinguish (1.5)r,~,~ and (1.6)r,~,~

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w The bridge 139

D e f i n i t i o n 1.2 Let T > 0 A F E HI0, T] is said to be solvable if for any x C ~ n and 7 E ~[0, T], equation (1.5)r,%~ admits a unique adapted solution O(.) E ~4[0,T] The set of all F E H[0,T] that is solvable is denoted by S[0, T] Any F E g [ 0 , T] \ S[0, T] is said to be nonsolvable

Now, let us introduce the following notions, which will play the central role in this chapter

D e f i n i t i o n 1.3 Let T > 0 and F - (b,a, h,g) e H[O,T] A C 1 function (:

= : [0, T] + S n+m, with A : [0, T] -~ S n, B: [0, T] -+ ~rn•

c

and C : [0, T] + S "~, is called a bridge extending from F, (defined on [0, T]),

if there exist some constants K, 5 > 0, such that

{ c(T) _< A(t) o, vt Io, T],

and either (1.8)-(1.9) or (1.8)'-(1.9)' hold:

(1.9)

X w

y ' h(t,O) h(t,8)] )

<_-5Ix-hi 2, VO, O e M , a.e t e [O,T], a.s

(1.8)' (O(T) g(x)-g(5) ' g(x)-g(5) ) > 0 , V x , h e l R n

y ' h(t,e) - h(t,~) )

+ ( ~(t) ( a(t'O) -a(t'z 2 -0) ) a(t,O)z-_a(t,-~) ) )

< - 5 { l y - ~ l 2 + I z - ~ 1 2 } , v e , ~ e M, a e t e [0, T], a.s

If (1.7)-(1.9) (resp (1.7) and (1.8)'-(1.9)') hold, we call 9 a type (I) (resp

type (II)) bridge emending from F (defined on [0, T]) The set of all type

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