In this paper, we examine, in a systematic fashion, some ill-posed problems arising in the theory of heat conduction. In abstract terms, letH be a Hilbert space andA: D (A)⊂H→H be an unbounded normal operator, we consider the boundary value problemu(t)=Au(t), 0<t<∞,u(0)=u 0∈D(A), $$\mathop {\lim }\limits_{t \to 0} \left\| {u\left( t \right)} \right\| = 0$$ . The problem of recoveringu 0 whenu(T) is known for someT>0 is not well-posed. Suppose we are given approximationsx 1,x 2,…,x N tou(T 1),…,u(T N) with 0<T, <…<T N and positive weightsP i,i=1,…,n, $$\sum\limits_{i = 1}^N {P_i = 1} $$ such that $$Q_2 \left( {u_0 } \right) = \sum\limits_{i = 1}^N {P_i } \left\| {u\left( {T_i } \right) - x_i } \right\|^2 \leqslant \varepsilon ^2 $$ . If ‖u t(0)‖≤E for some a priori constantE, we construct a regularized solution ν(t) such that $$Q\left( {\nu \left( 0 \right)} \right) \leqslant \varepsilon ^2 $$ while $$\left\| {u\left( 0 \right) - \nu \left( 0 \right)} \right\| = 0\left( {ln \left( {E/\varepsilon } \right)} \right)^{ - 1} $$ and $$\left\| {u\left( t \right) - \nu \left( t \right)} \right\| = 0\left( {\varepsilon ^{\beta \left( t \right)} } \right)$$ where 0<β(t)<1 and the constant in the order symbol depends uponE. The function β(t) is larger thant/m whent<T k andk is the largest integer such that $$(\sum\limits_{k = 1}^N {P_i (T_i )} )< (\sum\limits_{k = 1}^N {P_i (T_i )} = m$$ , which β(t)=t/m on [T k, m] and β(t)=1 on [m, ∞). Similar results are obtained if the measurement is made in the maximum norm, i.e.,Q ∞(u 0)=max{‖u(T i)−x i‖, 1≤i≤N}.
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