WANG SHEN-WANG
The question of the existence and uniqueness of a solution of the Hammerstein integral equation
Submitted 1964-01-01 | RussiaRxiv: ru-196401.50761 | Translated from Russian

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WANG SHEN-WANG

ON SOLUTIONS OF HAMMERSTEIN INTEGRAL EQUATIONS

(Presented by Academician A. N. Kolmogorov on 17 VII 1963)

The question of the existence and uniqueness of a solution of the Hammerstein integral equation

\[ u(s)=\int_D K(s,t)f(t,u(t))\,dt \tag{1} \]

has been considered by many authors (see, for example, \((^{1-6})\)). I have also obtained some results in this direction \((^7)\). In doing so it was most often assumed that the kernel \(K(s,t)\) is positive definite, quasi-positive, or quasi-negative. The general case, apparently, has not yet been systematically studied. M. M. Vainberg and R. I. Kachurovskii \((^5)\) obtained some interesting results for the general case. In the present article the author also attempts to consider the general case.

For the sake of generality, instead of equation (1) we consider the system

\[ u_i(s)=K_i f_i u(s)\qquad (i=1,2,\ldots,m), \tag{2} \]

where

\[ K_i f_i u(s)=\int_D K_i(s,t) f_i(t,u_1(t),\ldots,u_m(t))\,dt . \]

1. Special case.

Let \(D\) be a measurable set of finite-dimensional Euclidean space and \(mD<\infty\). Let \(M(u)\), \(N(v)\) \((-\infty<u,v<\infty)\) be mutually complementary \(N\)-functions, the second of which satisfies the \(\Delta_2\)-condition. Let \(L_M^*, L_N^*\) be Orlicz spaces of functions defined on \(D\), satisfying the relation \(E_M\subset L_2\subset L_N^*\).

Suppose that the functions \(f_i(t,u_1,\ldots,u_m)\) \((i=1,2,\ldots,m;\ t\in D,\ -\infty<u_j<\infty\ (j=1,\ldots,m))\) satisfy the following conditions:

\(\delta_1)\) the Carathéodory condition, i.e. they are measurable in \(t\) for each \((u_1,\ldots,u_m)\) and continuous in \((u_1,\ldots,u_m)\) for almost all \(t\).

\(\delta_2)\) There exists a function \(F(t,u_1,\ldots,u_m)\), satisfying the Carathéodory condition, such that \(F(t,0,\ldots,0)\in L\) and

\[ f_i(t,u_1,\ldots,u_m)=\frac{\partial}{\partial u_i}F(t,u_1,\ldots,u_m)\qquad (j=1,2,\ldots,m). \]

\(\delta_3)\) The operator

\[ f(u)=(f_1(u),\ldots,f_m(u)), \]

where

\[ f_i(u)=f_i(t,u_1(t),\ldots,u_m(t)), \]

acts continuously from

\[ \mathscr E_M=\underbrace{E_M+\cdots+E_M}_{m} \quad\text{to}\quad \mathscr L_N^*=\underbrace{L_N^*+\cdots+L_N^*}_{m}. \]

Suppose also that the functions \(K_i(s,t)\) are defined on \(D\times D\) and generate bounded linear integral operators \(K_i\), acting from \(L_N^*\) into \(E_M\). Let these operators, considered on \(L_2\), be self-adjoint operators, and let the positive part of the spectrum of each operator \(K_i\) have positive infimum \(\lambda_i\).

Put

\[ T_i=(b_iK_i-I)^{-1}K_i, \]

i.e.

\[ T_i=\int_{m_i}^{M_i}\frac{\lambda}{b_i\lambda-1}\,dE_\lambda^{(i)} =\int_{m_i}^{0}\frac{\lambda}{b_i\lambda-1}\,dE_\lambda^{(i)} +\int_{\lambda_i-\theta}^{M_i}\frac{\lambda}{b_i\lambda-1}\,dE_\lambda^{(i)}, \]

where \(E_\lambda^{(i)}\) is the resolution of the identity for the operator \(K_i\), and \(b_i\lambda_i>1\). Therefore both operators on the right-hand side of the last equality are bounded and positive definite. It follows that the operator \(T_i\) is the same. Moreover, it can be shown that \(T_i\) is bounded as an operator from \(L_N^*\) into \(E_M\).

Theorem 1. Let \(f_i(t,u_1,\ldots,u_m)\) and \(K_i(s,t)\) \((i=1,2,\ldots,m)\) satisfy the conditions stated above. If

\[ F(t,u_1+h_1,\ldots,u_m+h_m)-F(t,u_1,\ldots,u_m)- \sum_{i=1}^{m} f_i(t,u_1,\ldots,u_m)h_i \geq \frac12\sum_{i=1}^{m}(b_i-c_i)h_i^2, \tag{I} \]

where \(b_i\lambda_i>1,\ c_i\|T_i\|<1\), then there exists one and only one solution of system (2).

For the proof, system (2) is replaced by the equivalent system

\[ u_i=T_i g_i u \qquad (i=1,\ldots,m,\ u=(u_1,\ldots,u_m)), \tag{3} \]

where

\[ g_i(t,u_1,\ldots,u_m)=b_i u_i-f_i(t,u_1,\ldots,u_m). \]

Define the operator

\[ Hu=(H_1u_1,\ldots,H_m u_m), \]

where

\[ H_i=T_i^{1/2}\qquad (i=1,2,\ldots,m), \]

and the functional

\[ G(u)=\int_D G(t,u_1(t),\ldots,u_m(t))\,dt, \]

where

\[ G(t,u_1,\ldots,u_m)=\frac12\sum_{i=1}^{m} b_i u_i^2-F(t,u_1,\ldots,u_m). \]

Then the functional defined in \(L_2\),

\[ \varphi(u)=\frac12(u,u)-G(Hu), \]

as is easily verified, satisfies the relation

\[ \varphi(u+h)-\varphi(u)-(\varphi'(u),h)\geq \frac12(1-q)\|h\|^2, \]

where \(q=\max_i c_i\|T_i\|<1\). From the results of \((^{2,8})\) it follows that \(\varphi(u)\) is a convex, weakly lower semicontinuous functional having in \(L_2\) at least one minimum point \(u_0\). Then \(Hu\) is a solution of system (3). It is easy to show that this solution is unique.

Remark 1. Condition (I) can be replaced by the condition

\[ \sum_{i=1}^{m}\left[f_i(t,u_1+h_1,\ldots,u_m+h_m)-f_i(t,u_1,\ldots,u_m)\right]h_i \geq \sum_{i=1}^{m}(b_i-c_i)h_i^2. \tag{I'} \]

Remark 2. It can be shown that every sequence minimizing the functional \(\varphi(u)\) converges to \(u_0\) in \(L_2\).

Remark 3. Theorem 1 can be formulated in a more general form. For simplicity we restrict ourselves to the case of a Hilbert space.

Theorem \(1'\). Let \(K\) be a bounded self-adjoint operator acting in a Hilbert space \(H\). Let the positive part

of the spectrum of the operator \(K\) has a positive infimum \(\lambda_1\). Let \(f(u)\) be a discontinuous potential operator acting in \(H\): \(f(u)=\operatorname{grad} F(u)\).

If

\[ F(u+h)-F(u)-(f(u),h)\geq \frac12 (b-c)\|h\|^2 \]

or

\[ (f(u+h)-f(u),h)\geq (b-c)\|h\|^2, \]

where \(b\lambda_1>1\), \(c\|T\|<1\), and \(T=(bK-I)^{-1}K\), then there exists one and only one solution of the equation

\[ u=Kf(u). \]

2. Nonlocal implicit function theorem.

Theorem 2. Let the functions \(g_i(t,v_1,\ldots,v_n,u_1,\ldots,u_m)\) \((i=1,\ldots,m)\) satisfy the Carathéodory condition.

If

\[ \sum_{i=1}^{m}\bigl[g_i(t,v_1,\ldots,v_n,u_1+h_1,\ldots,u_m+h_m) \]

\[ -g_i(t,v_1,\ldots,v_n,u_1,\ldots,u_m)\bigr]h_i \geq \varepsilon_0\sum_{i=1}^{m}h_i^2\qquad (\varepsilon_0>0), \tag{4} \]

then there exists one and only one system of functions

\[ u_i=\eta_i(t,v_1,\ldots,v_n)\qquad (i=1,\ldots,m), \tag{5} \]

satisfying the equations

\[ g_i(t,v_1,\ldots,v_n,u_1,\ldots,u_m)=0\qquad (i=1,\ldots,m), \]

and each of the functions (5) satisfies the Carathéodory condition.

3. The general case.

In this section we consider only the case of Hilbert space.

Let \(K_i\) be bounded self-adjoint operators acting in \(L_2\). Let \((-a_i,a_i+\lambda_i)\) be a subinterval of the resolvent set of the operator \(K_i\). Put \(\widetilde K_i=K_i+a_i I\), \(T_i=(b_i\widetilde K_i-I)^{-1}\widetilde K_i\), where \(b_i\lambda_i>1\). Then the \(T_i\) are bounded positive definite operators. Let \(c_i>0\) satisfy the inequalities \(c_i\|T\|<1\).

Theorem 3. Let \(K_i\) be the operators defined above, let the functions \(f_i(t,u_1,\ldots,u_m)\) satisfy conditions \(\delta_1)\) and \(\delta_2)\) of item 1, and let the operator \(f(u)\) be continuous in \(L_2\).

Let:

\[ \sum_{i=1}^{m} a_i\bigl[f_i(t,u_1+h_1,\ldots,u_m+h_m)-f_i(t,u_1,\ldots,u_m)\bigr]h_i \geq (\varepsilon_0-1)\sum_{i=1}^{m}h_i^2, \tag{I} \]

where \(\varepsilon_0\) is a sufficiently small positive number,

\[ F(t,u_1+h_1,\ldots,u_m+h_m)-F(t,u_1,\ldots,u_m)- \]

\[ -\sum_{i=1}^{m}\{1-a_i(b_i-c_i)\}\bigl[f_i(t,u_1+h_1,\ldots,u_m+h_m)-f_i(t,u_1,\ldots,u_m)\bigr]h_i \]

\[ \geq \frac12\sum_{i=1}^{m}(b_i-c_i)h_i^2 +\sum_{i=1}^{m} a_i\bigl[f_i(t,u_1+h_1,\ldots,u_m+h_m)-f_i(t,u_1,\ldots,u_m)\bigr]^2. \tag{II} \]

Then there exists one and only one solution of system (2).

Remark 1. The assertion of the theorem remains valid if condition (II) is replaced by the condition

\[ \sum_{i=1}^{m}\bigl[1-2a_i(b_i-c_i)\bigr]\bigl[f_i(t,u_1+h_1,\ldots,u_m+h_m)-f_i(t,u_1,\ldots,u_m)\bigr]h_i \]

\[ \geq \sum_{i=1}^{m}(b_i-c_i)h_i^2 +\sum_{i=1}^{m}\bigl[a_i^2(b_i-c_i)-a_i\bigr]\bigl[f_i(t,u_1+h_1,\ldots,u_m+h_m)- \]

\[ -f_i(t,u_1,\ldots,u_m)\bigr]^2. \tag{II'} \]

Remark 2. The simultaneous fulfillment of conditions (I) and (II), or (I) and (II′), is possible. For example, suppose that \(1-2a_i(b_i-c_i)>0\), \(b_i\geq c_i\). Then (I) and (II′) are simultaneously fulfilled if

\[ \sum_{i=1}^{m}\left[f_i(t,u_1+h_1,\ldots,u_m+h_m)-f_i(t,u_1,\ldots,u_m)\right]h_i\geq \]

\[ \geq \sum_{i=1}^{m}\frac{b_i-c_i}{\alpha}h_i^2, \]

where \(\alpha=\min_i[1-2a_i(b_i-c_i)]\).

For the proof of Theorem 3, put

\[ g_i(t,u_1,\ldots,u_m)=u_i+a_i f_i(t,u_1,\ldots,u_m). \]

Then system (2) is equivalent to the vector equation

\[ g(u)=\widetilde K f(u), \tag{6} \]

where \(\widetilde K=(\widetilde K_1,\ldots,\widetilde K_m)\).

Since

\[ \sum_{i=1}^{m}\left[g_i(t,u_1+h_1,\ldots,u_m+h_m)-g(t,u_1,\ldots,u_m)\right]h_i \geq \varepsilon_0\sum_{i=1}^{m}h_i^2, \tag{7} \]

it follows, by Theorem 2, that there exists one and only one system of functions

\[ u_i=\eta_i(t,v_1,\ldots,v_m)\qquad (i=1,2,\ldots,m), \]

satisfying the equations

\[ v_i=g_i(t,u_1,\ldots,u_m). \]

It follows from (7) that the functions \(\eta_i(t,v_1,\ldots,v_m)\) satisfy the Lipschitz condition. Therefore the operator \(\eta(v)\) is continuous in \(L_2\).

Put

\[ \widetilde f_i(t,v_1,\ldots,v_m) = f_i(t,\eta_1(t,v_1,\ldots,v_m),\ldots,\eta_m(t,v_1,\ldots,v_m)) \]

\[ (i=1,\ldots,m), \]

\[ \widetilde f(v)(t)= (\widetilde f_1(t,v_1(t),\ldots,v_m(t)),\ldots, \widetilde f_m(t,v_1(t),\ldots,v_m(t))). \]

Then the operator \(\widetilde f(v)\) is continuous in \(L_2\), and equation (6) is equivalent to the equation

\[ v=\widetilde K\widetilde f(v). \]

Theorem 1′ is applicable to this equation.

The potentiality of the operator \(\widetilde f(v)\) follows from the following assertion.

Lemma. There exists a function \(\widetilde F(t,v_1,\ldots,v_m)\), satisfying the Carathéodory condition, such that \(\widetilde F(t,0,\ldots,0)\in L\) and

\[ \frac{\partial}{\partial v_i}\widetilde F(t,v_1,\ldots,v_m) = \widetilde f_i(t,v_1,\ldots,v_m). \]

Mathematics Faculty
Nanking University
Nanking, PRC

Received
18 X 1962

REFERENCES

  1. A. Hammerstein, Acta Math., 54 (1929).
  2. M. M. Vainberg, Variational methods for the study of nonlinear integral equations, 1956.
  3. M. A. Krasnosel’skii, Topological methods in the theory of nonlinear integral equations, 1956.
  4. M. M. Vainberg, I. V. Shragin, DAN, 128, No. 1, 9 (1959).
  5. M. M. Vainberg, R. I. Kachurovskii, DAN, 129, No. 6 (1959).
  6. C. L. Dolph, Trans. Am. Math. Soc., 66, No. 2, 289 (1949).
  7. Wang Sheng Wang, Bull. Acad. Polon. Sci., ser. sci. math., astr. et phys., 8, No. 6 (1960).
  8. R. I. Kachurovskii, UMN, 15, No. 4, 213 (1960).

Submission history

WANG SHEN-WANG