UDC 517.9
MATHEMATICS
Submitted 1970-01-01 | RussiaRxiv: ru-197001.30948 | Translated from Russian

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UDC 517.9

MATHEMATICS

N. V. KRYLOV

A PROBLEM WITH TWO FREE BOUNDARIES FOR AN ELLIPTIC EQUATION AND OPTIMAL STOPPING OF A MARKOV PROCESS

(Presented by Academician A. N. Kolmogorov on 31 III 1970)

1. Let \(E_n\) be \(n\)-dimensional Euclidean space, \(U\) a bounded domain in \(E_n\) with twice continuously differentiable boundary,

\[ Lu(x)=a_{ij}(x)u_{ij}(x)+b_i(x)u_i(x)-c(x)u(x) \]

an elliptic differential operator acting on functions \(u\in W_p^2(U)\) (see \((^1)\)). Here \(u_{ij}\) is the mixed derivative with respect to \(x_i,x_j\); \(u_i\) is the derivative with respect to \(x_i\); summation over the indices \(i,j\) is assumed. Suppose that \(a_{ij}, b_i, c\) are bounded, \(c\ge 0\), the matrix \(a_{ij}\) is uniformly nondegenerate, and, for \(n\le 2\), \(p=2\), while for \(n>2\) the \(a_{ij}(x)\) are continuous in \(E_n\), \(p>n/2\). Let two functions \(\psi_1,\psi_2\in W_p^2(U)\) also be given such that \(\psi_1\ge \psi_2\) in \(U\), \(\psi_1=\psi_2\) on \(\partial U\).

Theorem 1. There exists, and moreover is unique, a function \(u\in W_p^2(U)\) possessing the following two properties: a) \(\psi_1(x)\ge u(x)\ge \psi_2(x)\) for \(x\in U\cup\partial U\); b) \((-1)^iLu\ge 0\) (a.e.) on

\[ \Gamma_i=\{x:\ (-1)^i[u(x)-\psi_i(x)]>0\} \]

for \(i=1,2\). In addition, if \(p>n\), then \(\operatorname{grad}(u-\psi_i)=0\) at all points of the set \(U\setminus\Gamma_i,\ i=1,2\).

The problem consisting in finding a function satisfying conditions a), b) is called a problem with two free boundaries, because when \(\psi_1>\psi_2\) in \(U\) it is equivalent to the problem of finding a function \(u\in W_p^2(U)\) and two closed sets \(G_1,G_2\) such that a) is satisfied, \(u=\psi_1\) and \(Lu\ge 0\) (a.e.) on \(G_1\), \(u=\psi_2\) and \(Lu\le 0\) (a.e.) on \(G_2\), and

\[ Lu=0 \]

(a.e.) on \(U\setminus(G_1\cup G_2)\).

This problem is a generalization of the problem with one free boundary and is directly related to problems with a variational inequality \((^2)\). Namely, if \(L\psi_1<0\), then from Theorem 1 it is not difficult to derive that \(u\) is the unique function in \(W_p^2(U)\) such that

\[ u\ge \psi_2,\qquad (u-\psi_2)|_{\partial U}=0, \]

\[ Lu\le 0 \]

(a.e.) on \(\{x:\ u(x)=\psi_2(x)\}\), and

\[ Lu=0 \]

(a.e.) on \(\{x:\ u(x)>\psi_2(x)\}\).

All these results can be obtained with the aid of certain facts from the theory of Markov processes. They are presented below.

2. Let \(X\) be a standard process in a locally compact space \(E\) (see \((^3)\)), \(B\) the space of Borel bounded functions \(f\) with norm

\[ |f|=\sup\{|f|:\ x\in E\}, \]

\(R_\lambda\) the resolvent of the process \(X\), \(m\) some probabilistic regular measure on \(E\), \(p>1\). Suppose that there exists a constant \(N\) such that for all \(x\in E\), \(f\in B\) the function \(R_0f(x)\) is continuous and

\[ R_0|f|(x)\le N\|f\|_p, \]

where \(\|f\|_p\) is the norm in the space \(L_p\) of functions integrable to the \(p\)-th power with respect to the measure \(m\). Let two Borel functions \(\psi_1(x),\psi_2(x)\) also be given, with \(\psi_1\ge\psi_2\). We want to study the function

\[ v(x)=\inf_{\tau}\sup_{\sigma} M_x\{\psi_1(x_\tau)\chi_{\tau<\sigma}+\psi_2(x_\sigma)\chi_{\sigma\le\tau}\}, \]

where the lower and upper bounds are taken over the set of all Markov times \(\tau\) and \(\sigma\), respectively.

The problem of studying \(v(x)\) is a generalization of the problems considered in \((^{4-6})\). Our method differs from the methods known from \((^{4-6})\); it consists in representing the function \(v(x)\) in the form \(R_0f(x)\), where \(f\in L_p\). In proving this representation we use the method of “continuous” stopping. The main technical tool is the following lemma.

For \(c\in B\) put
\[ R_c f(x)=M_x\int_0^\infty \exp\left[-\int_0^t c(x_s)\,ds\right]f(x_t)\,dt, \]
and, for \(n,m>0\), let
\[ u_{nm}=\inf\sup R_{c_1+c_2}(c_1\psi_1+c_2\psi_2), \]
where the \(\inf(\sup)\) is taken over the set of all functions \(c_1(c_2)\) such that \(0\le c_1\le n\) \((0\le c_2\le m)\),
\[ \delta_{nm}=-(u_{nm}-\psi_1)_+,\qquad \rho_{nm}=(u_{nm}-\psi_2)_-{}^* . \]

Lemma. Suppose that, for some \(f^i\in L_p\), \(\psi_i=R_0 f^i\) \((i=1,2)\). Then:

a) \(u_{nm}=R_c(n\delta_{nm}+m\rho_{nm})\);

b) if \(n>m\), then
\[ |\delta_{nm}|\le R_n f_-^1,\qquad \rho_{nm}\le R_m nR_n f_-^1+R_m f_+^2; \]

c)
\[ u_{nm}(x)=M_x\left[\int_0^{\tau\wedge\sigma}(n\delta_{nm}+m\rho_{nm})(x_t)\,dt +u_{nm}(x_{\tau\wedge\sigma})\right] \]
\[ =\sup_\sigma M_x\left[ \int_0^{\tau\wedge\sigma} n\delta_{nm}(x_t)\,dt -\rho_{nm}(x_\sigma)\chi_{\sigma\le\tau} +\psi_2(x_\sigma)\chi_{\sigma\le\tau} +u_{nm}(x_\tau)\chi_{\tau<\sigma} \right] \]
\[ =\inf_\tau \sup_\sigma M_x\left[ \psi_1(x_\tau)\chi_{\tau<\sigma} +\psi_2(x_\sigma)\chi_{\sigma\le\tau} -\delta_{nm}(x_\tau)\chi_{\tau<\sigma} -\rho_{nm}(x_\sigma)\chi_{\sigma\le\tau} \right]. \]

Proof. Consider the operator
\[ F_{nm}v=R_{n+m}\bigl[(n+m)v-n(v-\psi_1)_+ + m(v-\psi_2)_-\bigr] \]
in the space \(B\). From the inequality
\[ \bigl|[(m+n)t_1-n(t_1-a)_+ + m(t_1-b)_-] -[(m+n)t_2-n(t_2-a)_+ + m(t_2-b)_-]\bigr| \le (n+m)|t_1-t_2| \]
it follows that
\[ |F_{nm}v_1-F_{nm}v_2|\le (n+m)R_{n+m}|v_1-v_2|. \]
Further, note that from the estimate \(|R_0 f|\le N\|f\|\) it follows that
\[ (n+m)\|R_{n+m}f\|\le \varepsilon_{n+m}\|f\|, \]
where \(\varepsilon_{n+m}<1\) and does not depend on \(f\).

Thus the operator \(F_{nm}\) is a contraction in \(B\). By Banach’s theorem there exists \(v_{nm}\in B\) such that
\[ v_{nm}=F_{nm}v_{nm}. \]

Next, for \(0\le d\le k\) the equality
\[ R_d f=\sum_{i=0}^\infty [R_k(k-d)]^i R_k f \]
holds. Hence, for
\[ d=c_1+c_2,\qquad k=n+m,\qquad f=dv_{nm}-n(v_{nm}-\psi_1)_+ + m(v_{nm}-\psi_2)_-, \]
in view of the equality
\[ R_{n+m}f=c_{nm}+R_{n+m}(d-k)v_{nm}, \]
it easily follows that
\[ R_{c_1+c_2}f=v_{nm} \]
for \(0\le c_1\le n,\;0\le c_2\le m\).

From this equality and the inequality
\[ c_2(v_{nm}-\psi_2)+m(v_{nm}-\psi_2)_-\ge 0 \]
we obtain
\[ v_{nm}=\sup R_{c_1+c_2}\bigl[c_1v_{nm}-n(v_{nm}-\psi_1)_+ + c_2\psi_2\bigr], \]
and, as a consequence of the inequality
\[ c_1(v_{nm}-\psi_1)-n(v_{nm}-\psi_1)_+\le 0, \]
this gives
\[ v_{nm}=\inf\sup R_{c_1+c_2}(c_1\psi_1+c_2\psi_2), \]
i.e. \(v_{nm}=u_{nm}\). Assertion a) now follows from the equality
\[ R_{c_1+c_2}f=v_{nm} \]
for \(c_1=c_2=0\).

Let us again turn to the equality
\[ u_{nm}=R_{c_1+c_2}\bigl[(c_1+c_2)u_{nm}+n\delta_{nm}+m\rho_{nm}\bigr]. \]
For \(n>m,\;a\ge b\) we have
\[ nt-n(t-a)_+ + m(t-b)_-\le na, \]
therefore, for \(c_1=n,\;c_2=0,\;n>m\), we obtain
\[ u_{nm}\le nR_n\psi_1, \]
and since
\[ nR_n\psi_1=nR_nR_0 f^1=R_0 f^1-R_n f^1=\psi_1-R_n f^1, \]
it follows that
\[ u_{nm}\le \psi_1-R_n f^1\le \psi_1+R_n f_-^1 \]
and
\[ |\delta_{nm}|\le R_n f_-^1 . \]

If, however, we take \(c_1=0,\;c_2=m\), then
\[ u_{nm}\ge -R_m nR_n f_-^1+R_m[mu_{nm}+m\rho_{nm}] \ge -R_m nR_n f_-^1+mR_m\psi_2, \]
and
\[ \rho_{nm}\le R_m nR_n f_-^1+R_m f_+^2. \]
Assertion b) is proved.

The first equality in c) follows from a) and the strong Markov property of \(X\). The second equality is valid because, on the one hand,
\[ u_{nm}\ge \psi_2-\rho_{nm} \]
and \(\rho_{nm}\ge 0\), while, on the other hand, if
\[ \sigma=\inf\{t:\rho_{nm}(x_t)>0\}, \]
then
\[ \int_0^{\tau\wedge\sigma}\rho_{nm}(x_t)\,dt=0 \]
and
\[ \psi_2(x_\sigma)-\rho_{nm}(x_\sigma)=u_{nm}(x_\sigma). \]
The third equality is obtained by analogous arguments from the second. The lemma is proved.

From this lemma the following theorems are derived rather simply. In their statements,
\[ M_x(\tau,\sigma)=M_x[\psi_1(x_\tau)\chi_{\tau<\sigma}+\psi_2(x_\sigma)\chi_{\sigma\le\tau}]. \]

Theorem 2. Suppose that, for some \(f^i\in B\), \(\psi_i=R_2 f^i\) \((i=1,2)\); then there exists a function \(f\in B\) such that \(v=R_0 f\), and hence \(v\) is continuous. Further,
\[ (-1)^i f\le 0\quad\text{on}\quad \Gamma_i(v)=\{x:(-1)^i[v(x)-\psi_i(x)]>0\}, \]
\[ \lim_{n\to\infty}\lim_{m\to\infty}\|v-u_{nm}\|=0,\qquad v(x)=\sup_\sigma M_x(\tau_1,\sigma)=\inf_\tau M_x(\tau,\tau_2), \]
\[ {}^*\quad a_+=\frac12(|a|+a),\qquad a_-=\frac12(|a|-a). \]

where \(\tau_i=\inf\{t:\ v(x_t)=\psi_i(x_t)\}\) \((i=1,2)\). Moreover, if \(u,h\in B\) are functions related by the relation \(u=R_0h\), \(\psi_1\geq u\geq\psi_2\), and \((-1)^i h\leq 0\) on \(\Gamma_i(u)\), for \(i=1,2\), then \(u=v\).

Theorem 3. Suppose there exists a constant \(N_1\) such that \(\lambda\|R_\lambda f\|_p\leq N_1\|f\|_p\) for all \(f\in B\), \(\lambda>0\). Then in the formulation of Theorem 2 one may replace \(B\) by \(L_p\). Moreover, as \(\tau_i\) one may also take
\[ \inf\{t:\ v(x_t)=\psi_i(x_t),\quad x_t\in \operatorname{supp}[(-1)^i f]^+\}. \]

Before formulating Theorem 4, take two closed sets \(G_1,G_2\) and denote by \(\mathfrak M_i\) the set of Markov times such that
\[ P_x\{x_\tau\in G_i\}=P_x\{\tau<\zeta\} \]
for all \(x\), and by \(\mathfrak N_i\) the set of hitting times of closed subsets of \(G_i\).

Theorem 4. Suppose the assumption of Theorem 3 is satisfied and there exist sequences of functions \(f_n^i\in L_p\) such that
\[ \operatorname{supp}[(-1)^i f_n^i]^+\subset G_i,\qquad R_0 f_n^1\geq R_0 f_n^2,\qquad \lim_{n\to\infty}\|[\psi_i-R_0 f_n^i]\chi_{G_i}\|=0. \]
Then
\[ \inf_{\tau\in\mathfrak M_1}\times \sup_{\sigma\in\mathfrak M_2} M_x(\tau,\sigma) = \inf_{\tau\in\mathfrak N_1}\sup_{\sigma\in\mathfrak M_2} M_x(\tilde\tau,\sigma) = \inf_{\tau\in\mathfrak M_1}\sup_{\sigma\in\mathfrak N_2^{\,x}} M_x(\tau,\sigma). \]
Moreover, all expressions in the last equality are continuous.

We make some remarks concerning the proofs of Theorems 1–4. Theorem 1 is derived from Theorem 3 with the aid of the known properties of \(R_0 f\) for quasidiffusion processes; Theorem 4 is also easily derived from Theorem 3. The proofs of Theorems 2 and 3 follow one and the same plan. First, with the aid of Lemma b), it is proved that
\[ \lim_{n\to\infty}\lim_{m\to\infty}\|\rho_{nm}+|\delta_{nm}|\|=0; \]
then, using Lemma c), that \(\|u_{nm}-v\|\to 0\). After this, from the estimate \(R_0|f|\leq N\|f\|_p\) and Lemmas a), b), one obtains the equality \(v=R_0 f\) and the sign properties of \((-1)^i f\). The equality
\[ v(x)=\sup_{\sigma} M_x(\tau_1,\sigma) \]
follows from the equality of \(u_{nm}\) to the third term in equality c) of the lemma and from the estimates \(|\delta_{nm}|\leq R_n f^{-}\), \(R_0|f|\leq N\|f\|_p\), \(\lambda\|R_\lambda f\|_p\leq N_1\|f\|_p\). The last assertion of Theorem 2 is almost obvious.

Moscow State University
named after M. V. Lomonosov

Received
19 III 1970

CITED LITERATURE

  1. S. L. Sobolev, Some Applications of Functional Analysis in Mathematical Physics, L., 1950.
  2. H. Lewy, Comm. Pure Appl. Math., 22, 2, 153 (1969).
  3. E. B. Dynkin, Markov Processes, M., 1963.
  4. E. B. Dynkin, DAN, 150, No. 2, 238 (1963).
  5. B. I. Grigelionis, A. N. Shiryaev, Theory of Probability and Its Applications, 11, 4, 612 (1966).
  6. S. M. Gusein-Zade, Theory of Probability and Its Applications, 14, 2, 732 (1969).

Submission history

UDC 517.9