Research article

Study of weak solutions of variational inequality systems with degenerate parabolic operators and quasilinear terms arising Americian option pricing problems

  • Received: 28 June 2022 Revised: 18 August 2022 Accepted: 19 August 2022 Published: 06 September 2022
  • MSC : 35K99, 97M30

  • In this paper, we study variational inequality systems with quasilinear degenerate parabolic operators in a bounded domain. As a series of penalty problems, the existence of the solutions in the weak sense is proved by a limit process. The uniqueness of the solution is also proved.

    Citation: Jia Li, Changchun Bi. Study of weak solutions of variational inequality systems with degenerate parabolic operators and quasilinear terms arising Americian option pricing problems[J]. AIMS Mathematics, 2022, 7(11): 19758-19769. doi: 10.3934/math.20221083

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  • In this paper, we study variational inequality systems with quasilinear degenerate parabolic operators in a bounded domain. As a series of penalty problems, the existence of the solutions in the weak sense is proved by a limit process. The uniqueness of the solution is also proved.



    Let ΩRN(N2) be a bounded simple connected domain, 0<T< and QT=Ω×[0,T]. We study the following parabolic systems

    {min{Liuifi(x,t,u1,u2),uiui,0}=0,(x,t)QT,ui(0,x)=ui0(x),xΩ,ui(t,x)=0,(x,t)Ω×(0,T), (1.1)

    with quasilinear degenerate parabolic operators, where

    Liui=uitdiv(|ui|pi2ui),i=1,2.

    The initial boundary value problem of variational inequalities arise in many application in pricing American options and their derivatives. Through the risk neutral strategy, the intrinsic value of many American options can ultimately be attributed to the solution of a variational inequality in the Black-Scholes models. The author refers to [1,2,3] and the references their in.

    The nonexistence, existence and uniqueness theory for weak solutions of parabolic systems were studied by many existing works, see e.g., [4,5,6]. In particular, Hassnaoui and Idrissi [6] studied the existence and uniqueness of weak solutions for a nonlinear parabolic system with non-degenerate case of (1.1). Escher, Laurencot and Matioc in [7] proved the global existence of nonnegative weak solutions to a degenerate parabolic system without quasilinear terms in (1.1). Furthermore, the authors showed that these weak solutions converge at an exponential rate.

    In recent years, there has been tremendous interest in developing existence and uniqueness theory for weak solutions of parabolic variational inequality (see, for example, [3,8,9,10,11,12,13,14] and the references therein). In 2014, the authors in [9] discussed the problem

    {min{utLuF(u,x,t),u(x,t)u0(x)}=0inQT,u(x,0)=u0(x)inΩ,u(x,t)=0onΩ, (1.2)

    with second order degenerate elliptic operator

    Lu=udiv(a(u)|u|p(x,t)2u)γ|u|p(x,t).

    Under the assumptions about u0 and F, they proved the existence and uniqueness of the weak solution. When a(u)=1, and p(x,t)=2, the authors in [10,11] discussed the existence and numerical algorithm of solution. In [12], a new property of variable exponent Lebesgue and Sobolev spaces was examined. Using these properties, the authors proved the existence of the solution of some parabolic variational inequality.

    To the best of our knowledge, the existence and uniqueness for multi-variable problem of parabolic variational inequalities (called variational inequality systems) were less studied. We cannot easily put the method in [10,11] to the multi-variable case since the systems are coupled with quasilinear terms.

    The aim of this paper is to study the existence and uniqueness of solution for parabolic systems with quasilinear degenerate inequalities in a bounded domain. We mainly use comparison theorem and penalty method to construct a sequence of approximation solutions with the help of monotone iteration technique. Then we obtain the existence of solutions to the system (1.1) by a standard limiting process.

    The paper is organized as follows. In Section 2, we present our main theorems. Section 3 gives some estimates about penalty problems to prove our main results. Section 4 analyses the existence and uniqueness of solutions to variational inequality system (1.1).

    In spirit of [3] and [9], we introduce the following maximal monotone graph

    G(x)={0,x>0,1,x=0. (2.1)

    The purpose of the paper is to obtain the existence and uniqueness of weak solutions of (1.1), and the weak solution is defined as follows.

    Definition 2.1. Function {(u1,ξ1),(u2,ξ2)} is called a generalized solution of the systems (1.1) if uiL(QT)L(0,T,W1,pi0(Ω)), tuiL2(ΩT), ξiL(0,T;L(Ω)), i=1,2, and satisfies (a) ui(x,t)ui0(x), (b) ui(x,0)=ui0(x), (c) ξiG(uiui0), (d) for every test-function φiC10(ˉQT)

    QT(uitφi+|ui|pi2uiφi)dxdtQTui0φi(x,0)dx=QTfi(x,t,u1,u2)φidxdt+t0Ωξiφidxdt. (2.2)

    Here C10(ˉΩT) is the space of all continuous and differentiable functions satisfying

    φi(x,T)=0for(x,t)Ω×(0,T),i=1,2.

    Condition (d) of Definition 2.1 implies that

    t0Ω(uitφi+|ui|pi2uiφi)dxdt+QTui(x,t)φi(x,t)dxΩTui0φi(x,0)dx=t0Ωfi(x,t,u1,u2)φidxdt+t0Ωξiφidxdt. (2.3)

    We introduce the constrains to the nonlinear functions fi,i=1,2 involved in this paper as follows.

    Definition 2.2. A function f=f(u1,u2) is quasimonotone nondecreasing (resp., nonincreasing) if for fixed u1 (or u2), f is nondecreasing (resp., nonincreasing) in u2 (or u1).

    To study the problem (1.1), we make the following assumptions:

    (H1) fi(x,t,u1,u2) is quasimonotonically nondecreasing for u1, u2, i=1,2.

    (H2) fi(x,t,u1,u2)C(Ω×[0,T]×R2), and there exists a nonnegative function g(s)C1(R) such that

    |fi(x,t,u1,u2)|min{g(u1),g(u2)}.

    Our main results are present as follows:

    Theorem 2.1. Let (H1) and (H2) be satisfied, and ui0L(ΩT)W1,pi0(Ω), i=1,2. Then problem (1.1) has a solution u=(u1,u2) in the sense of Definition 2.2.

    Theorem 2.2. Assume that f=(f1,f2) is Lipschitz continuous in (u1,u2), then the solution of problem (1.1) is unique.

    To prove the theorem, we consider the following penalty problem

    {Liεuiε=fi(x,t,u1ε,u2ε)βε(uiεui0),(x,t)QT,uiε(x,0)=ui0ε(x)=ui0+ε,xΩ,uiε(x,t)=ε,(x,t)QT, (3.1)

    where

    Liεuiε=uiεtdiv((|uiε|2+ε)pi22uiε).

    Here, βε() is the penalty function satisfying

    ε(0,1),βε()C2(R),βε(x)0,βε(0)=1,βε(x)0,βε(x)0,limε0+βε(x)={0,x>0,1,x=0. (3.2)

    It is worth noting that when ui>ui,0, Liuifi(x,t,u1,u2)=0, and when ui=ui,0, one gets Liuifi(x,t,u1,u2) in (1.1). In (3.1), βε(uiεui0) plays a similar role. When uiε>ui0+ε,

    Liεuiεfi(x,t,u1ε,u2ε)=βε(uiεui0)=0,

    and when ui0uiεui0+ε, we have

    Liεuiεfi(x,t,u1ε,u2ε)=βε(uiεui0)0.

    With a similar method as in [8], we can prove that regularized problem has a unique weak solution

    uiL(QT)L(0,T,W1,pi0(Ω)),tuiL2(QT),i=1,2,

    satisfying the following integral identities

    Ωtuiφidx+Ω|ui|pi2uiφidx+Ωβε(uiεui0)φidx=QTfi(x,t,u1,u2)φidx (3.3)

    with φiC1(ˉΩT) and t(0,T).

    We start with two preliminary results that will be used several times henceforth.

    Lemma 3.1. [[15], Lemma2.1.] Let M(s)=|s|p(x,t)2s, then ξ,ηRN

    (M(ξ)M(η))(ξη){2p|ξη|p,2p<,(p1)|ξη|2(|ξ|p+|η|p)p2p,1p<2.

    Lemma 3.2. (Comparison principle) Assume ui and vi are in Lpi(0,T;W1,pi(Ω)). If LiεuiLiεvi in QT and ui(x,t)vi(x,t) on QT, then ui(x,t)vi(x,t) in QT, i=1,2.

    Proof. We argue by contradiction. Suppose ui(x,t) and vi(x,t) satisfy LiεuiLiεvi in QT, and there is a δ>0 such that for some 0<τT, wi=uivi>δ on the set

    Ωδ=Ω{x:wi(x,t)>δ}

    and |Ωδ|>0, i=1,2. Let

    Fε(ξ)={2ε122ξ12,ifξ>ε,0,ifξε,

    whereδ>ε>0. Since Fε(wi)0, we multiply LiεuiLiεvi by Fε(wi) and integrate in Qτ to have

    QτtwiFε(wi)dxdt+Qτ[(|uiε|2+ε)pi22uiε(|viε|2+ε)pi22viε]Fε(wi)dxdt0

    or equivalently

    J1+J20, (3.4)

    where Qτ,ε={(x,t)QT|w>ε},

    J1=Qτ,εtwiFε(wi)dxdt,
    J2=12Qτ,εw32i[(|uiε|2+ε)pi22uiε(|viε|2+ε)pi22viε]widxdt.

    Now let t0=inf{t(0,τ]:w>ε}, then we estimate J1 as follows

    J1=Qτ,θtwiFε(wi)dxdt=Ω(t00twiFε(wi)dt+t00twiFε(wi)dt)dxΩwiεFε(s)dsdxΩδwiεFε(s)dsdx. (3.5)

    Using δ>ε>0 and the function Fε() to (3.5), we have

    J1Ωθ(wiε)Fε(s)dx(wiε)Fε(ε)|Ωδ|. (3.6)

    By the virtue of the first inequality of Lemma 3.1, we use wi=uivi>δ to arrive at

    J22(pi+1)Qτ,θw32i|wi|pidxdt0. (3.7)

    Since viLpi(0,T;W1,pi(Ω)), and we plug the above estimates (3.6) and (3.7) into (3.4) and drop the nonnegative terms, we arrive at

    (δε)ε12|Ωδ|<˜C.

    Note that limε0(δε)ε12|Ωδ|=+, we obtain a contradiction. This means that |Ωδ|=0 and wi0 a.e. in Qτ, i=1,2.

    Lemma 3.3. Let be weak solutions of (3.1). Then

    ui0εuiε|ui0|+ε,i=1,2, (3.8)
    uiε1uiε2forε1ε2,i=1,2, (3.9)

    where |u0|=supxΩ|u0(x)|, for details, see [16,17].

    Proof. First, we prove uiεui0ε by contradiction. Assume uiεui0ε in Q0T, i=1,2, Q0TQT. Noting uiεui0ε on QT, we may assume that uiε=ui0ε on Q0T. With (3.1) and letting t=0, it is easy to see that

    Lui0,ε=βε(ui0,εui0,ε)=1,i=1,2, (3.10)
    Luiε=βε(uiεui0,ε)1,i=1,2. (3.11)

    From Lemma 3.2, we have that

    uiε(x,t)ui0,ε(x)forany(x,t)QT,i=1,2. (3.12)

    Therefore, we obtain a contradiction.

    Second, we pay attention to uiε(t,x)|ui0|+ε. Applying the definition of βε() gives

    L(|ui0|+ε)=0, Luiε=βε(uiεui0,ε)0, i=1,2. (3.13)

    Using Lemma 3.2, (3.13) leads to

    uiε(t,x)|ui0|+εonΩ×(0,T),
    uiε(t,x)|ui0|+εinΩ,i=1,2. (3.14)

    Thus, combining (3.13) and (3.14) and repeating Lemma 3.2, we have

    uiε(t,x)|ui0|+εinQT,i=1,2. (3.15)

    Third, we aim to prove (3.9). From (3.1), it is easy to see that

    Luiε1=βε1(uiε1ui0,ε1),i=1,2. (3.16)
    Luiε2=βε2(uiε2ui0,ε2),i=1,2. (3.17)

    It follows by ε1ε2 and the definition of βε() that

    Lui0,ε2+βε1(uiε2ui0,ε)=βε2(uiε2ui0,ε)βε1(uiε1ui0,ε)=βε2(uiε2ui0,ε)βε1(uiε2ui0,ε)0, (3.18)

    i=1,2. Combining initial and boundary condition in (3.1), we obtain that the inequality (3.9) holds by Lemma 3.2.

    Lemma 3.4. For any (x,t)ΩT, the solution of problem (3.1) satisfies the estimate

    |uiε|Lpi(QT)QT(|uiε|2+ε)pi22|uiε|2dxdtC, (3.19)

    where C is a constant independent of ε.

    Proof. Choosing φi=uiε in (3.3), we have

    QTtuiεuiεdiv((|uiε|2+ε)pi22uiε)uiεdxdt=QTfi(x,t,u1ε,u2ε)uiεβε(uiεui0)uiεdxdt, (3.20)

    It is easy to see that

    QTtuiεuiεdxdt=12QTt(uiε)2dxdt=12QTuiε(,T)uiε(,0)dx. (3.21)

    Then we substitute (3.21) into (3.20) to arrive at

    QT(|uiε|2+ε)pi22|uiε|2dxdt=QTfi(x,t,u1ε,u2ε)uiεβε(uiεui0)uiεdxdt12QTuiε(,T)uiε(,0)dx.

    By (3.8) and the property of fi,

    |QTfi(x,t,u1ε,u2ε)uiεdxdt|C. (3.22)

    Applying (3.2) and (3.8) obtains

    QTβε(uiεui0)uiεdxdtε|Ω|T|Ω|T. (3.23)

    Then Lemma 3.4 is proved by combining (3.21)–(3.23).

    Lemma 3.5. The solution of problem (3.1) satisfies the estimate

    tuiεL2(QT)C(pi,T,|Ω|),i=1,2. (3.24)

    Proof. From (3.3), we have that

    QT(tuiε)2dxdt=QT(|uiε|2+ε)pi22uiεtuiεdxdt+QT[fi(x,t,u1ε,u2ε)βε(uiεui0)]tuiεdxdt=A1+A2, (3.25)

    where

    A1=QT(|uiε|2+ε)pi22uiεtuiεdxdt,
    A2=QT[fi(x,t,u1ε,u2ε)βε(uiεui0)]tuiεdxdt.

    First, we pay attention to A1. Using some differential transform technique obtains

    A1=12QT(|uiε|2+ε)pi22t(|uiε|2+ε)dxdt=1piQTt(|uiε|2+ε)pi2dxdt.

    Since ui0ε(x)=ui0+ε, then

    A11piQTt(|uiε|pi)dxdtΩ|ui0(,0)|pidx. (3.26)

    Applying Holder inequalities again, we have that

    A212QT[fi(x,t,u1ε,u2ε)βε(uiεui0)]2dxdt+12QT(tuiε)2dxdt. (3.27)

    Using (a+b)22(a2+b2), the property of fi and (3.2), we arrive at

    12QT[fi(x,t,u1ε,u2ε)βε(uiεui0)]2dxdtQTfi(x,t,u1ε,u2ε)2dxdt+QTβε(uiεui0)2dxdtQTfi(x,t,u1ε,u2ε)2dxdt+T|Ω|C. (3.28)

    Then, we obtain Lemma 3.5 by submitting (3.26)–(3.28) into (3.25).

    In this section, we are ready to prove that the system (1.1) has a unique generalized solution. By (3.18), (3.19) and (3.24) and the uniqueness of the weak limits, we know that there are functions

    uiL(QT)L(0,T,W1,pi0(Ω)), as ε0,

    such that for some subsequence of (u1ε,u2ε), denoted again by (u1ε,u2ε),

    uiεui,f(x,t,u1ε,u2ε)f(x,t,u1,u2)a.e.inQT, (4.1)
    uiεwuiinLpi(QT), (4.2)
    |uiε|pi2uiεwwiinLpipi1(QT),forsomewi, (4.3)
    tuiεwtuiinL2(QT), (4.4)

    where w stands for weak convergence, i=1,2.

    Lemma 4.1. For any (x,t)ΩT, wi=|ui|pi2ui, i=1,2.

    Proof. Applying triangle inequality |a+b||a|+|b|, (a,bR), it is easy to see that

    QT||uiε|pi2uiε|ui|pi2ui|dxdtQT||uiε|pi2|ui|pi2||uiε|dxdt+QT|ui|pi2|uiεui|dxdt=I1+I2,

    where

    I1=QT||uiε|pi2|ui|pi2||uiε|dxdt, I2=QT|ui|pi2|uiεui|dxdt.

    By mean of the inequality |arbr||ab|r, (r[0,1],a,b>0), we have

    I1=QT|(|uiε|pi)pi2pi(|ui|pi)pi2pi||uiε|dxdtQT||uiε|pi|ui|pi|pi2pi|uiε|dxdt.

    Applying Holder inequality and (4.2), we have

    I1(QT||uiε|pi|ui|pi|dxdt)pi2pi(QT|uiε|pi2dxdt)2pi0(ε0).

    Now we pay our attention to I2. From (4.2), we know that uiLpi(QT1). By (4.1), we may conclude that

    uiεuia.e.inQT.

    If not, there exists a measurable domain OT satisfying

    OT|uiεui|dxdt>0.

    Then, we obtain a contradiction with (4.2). Applying Holder inequality, we have

    I2=(QT|ui|pidxdt)pi2pi(QT|uiεui|pi2dxdt)2pi0(ε0).

    Hence Lemma 4.1 is proved.

    This proves that any weak convergence subsequence of |uiε|pi2xluiε will have xlwi as its weak limit and hence by a standard argument, and we have that as k,

    |uiε|xluiεw|ui|pi2xluiinLpipi1(QT). (4.5)

    Combining the above results, we have, in fact, proved that u=(u1,u2) is a generalized solution of (1.1).

    Lemma 4.2. For any (x,t)ΩT, it hold that

    βε(uεu0)ξG(uu0) as ε0. (4.6)

    Proof. Using (3.8) and the definition of βε, we have

    βε(uεu0)ξasε0.

    Now, we prove ξG(uu0). According to the definition of G(), we only need to prove that if u(x0,t0)>u0(x0),

    ξ(x0,t0)=0.

    In fact, if u(x0,t0)>u0(x0), there are a constant λ>0 and a δ-neighborhood Bδ(x0,t0) such that if ε is small enough, we have

    uε(x,t)u0(x)+λ,(x,t)Bδ(x0,t0).

    Thus, if ε is small enough, we have

    0βε(uεu0)βε(λ)=0,(x,t)Bδ(x0,t0).

    Furthermore, it follows by ε0 that

    ξ(x,t)=0,(x,t)Bδ(x0,t0).

    Hence, (4.6) holds, and the proof of Lemma 4.3 completes.

    The proof of Theorem 2.1. Applying (3.8), (3.9), and Lemma 4.3, it is clear that

    u(x,t)u0(x),in ΩT, u(x,0)=u0(x),in Ω, ξG(uu0),

    thus (a), (b), and (c) of Definition 1.1 hold. The rest arguments of existence part are the same as those of Theorem 2.1 in [8] by a standard limiting process. Thus, we omit the details.

    The proof of Theorem 2.2. The following is the uniqueness result to the solution of the system. Assume that {(u1,ξ1),(u2,ξ2)} and {(v1,ζ1),(v2,ζ2)} are two solutions of (1.1). Let φi=uivi in Definition 2.1, i=1,2, then by (2.3),

    t0Ωuitφi+|ui|pi2uiφidxdt+Ωui(x,t)φi(x,t)dxΩui(x,0)φi(x,0)dx=t0Ωfi(x,t,u1,u2)φidxdt+t0Ωξiφidxdt,a.e.t(0,T),
    t0Ωvitφi+|vi|pi2viφidxdt+Ωvi(x,t)φi(x,t)dxΩvi(x,0)φi(x,0)dx=t0Ωfi(x,t,v1,v2)φidxdt+t0Ωζiφidxdt,a.e.t(0,T),

    i=1,2. Subtracting the 2 equations, we get

    12Ωφi2dx=t0Ω(|ui|pi2ui|vi|pi2vi)φidxdt+t0Ω(fi(x,t,u1,u2)fi(x,t,v1,v2))φidxdtt0Ω(ξiζi)φidxdt.

    Now we prove

    (ξiζi)φi0,|(ξiζi)φi|φi. (4.7)

    On one hand, if ui(x,t)>vi(x,t), then using Lemma2.1 yields

    ui(x,t)>ui0(x).

    From (2.1) and above inequality, it is easy to see that

    ξi=0ζi. (4.8)

    Combining (2.1) and (4.8),

    (ξiζi)φi=(ξiζi)(uivi)0,(ξiζi)φiφi. (4.9)

    On the other hand, if ui(x,t)<vi(x,t), it is easy to have thatξi0=ζi.In this case,

    (ξiζi)φi=(ξiζi)(uivi)0,(ξiζi)φiφi. (4.10)

    Combining (4.9) and (4.10), (4.7) still holds.

    Using the previous inequality and the Lipschitz condition, a simple calculation shows that

    Ω|u1v1|2+|u2v2|2dx2Kt0Ω(|u1v1|+|u2v2|)2dxdt+t0Ω|u1v1|+|u2v2|dxdt.

    Furthermore, it follows by (a+b)22(a2+b2) and Holder inequalities that

    Ω|u1v1|2+|u2v2|2dx(2K+12T|Ω|)t0Ω|u1v1|2+|u2v2|2dxdt.

    Setting F(t)=t0Ω|u1v1|2+|u2v2|2dxdt, then the above inequality can be written as

    ddtF(t)(2K+12T|Ω|)F(t).

    A standard argument show that F(t)=0 since F(0)=0, and hence ui=vi,i=1,2. The proof is complete.

    In this paper, we study variational inequality systems with quasilinear degenerate parabolic operators in a bounded domain

    {min{Liuifi(x,t,u1,u2),uiui,0}=0,(x,t)QT,ui(0,x)=ui0(x),xΩ,ui(t,x)=0,(x,t)Ω×(0,T),

    with quasilinear degenerate parabolic inequalities, where

    Liui=uitdiv(|ui|pi2ui),i=1,2.

    The existence and uniqueness of the solutions in the weak sense are proved by using the penalty method and the reduction method with assumptions that p1 and p2 are constants satisfying pi>2. However, there are some problems that have not been solved: when 1<pi<2, pi>2 or pi is x-functions, i=1,2, we cannot use Lemmas 3.1 and 3.2 to prove Lemmas 3.3–3.5. We will continue to study this problem in future.

    The author sincerely thanks the editors and anonymous reviewers for their insightful comments and constructive suggestions, which greatly improved the quality of the paper. This work was supported by the Supply and demand docking education employment practice base project of education ministry (No. 20220106223) and the Supply and demand docking education oriented talent training project of education ministry (No. 20220104747).

    The authors declare no conflict of interest.



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