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1.
We consider the spectral problem generated by the Sturm-Liouville operator with complex-valued potential q(x) ∈ L 2(0, π) and degenerate boundary conditions. We show that the set of potentials q(x) for which there exist associated functions of arbitrarily high order in the system of root functions is everywhere dense in L 1(0, π).  相似文献   

2.
We consider a spectral problem generated by a Sturm-Liouville equation on the interval (0, π) with degenerate boundary conditions. We prove the existence of potentials q(x) ∈ L 2(0, π) such that the multiplicities of the eigenvalues λ n monotonically tend to infinity as n → ∞.  相似文献   

3.
We consider the spectral problem generated by the Sturm-Liouville equation with arbitrary complex-valued potential q(x) ∈ L 1(0, π) and with degenerate boundary conditions. We obtain sufficient conditions for the completeness of the system of eigenfunctions and associated functions of this operator.  相似文献   

4.
On the interval (0, τ), we consider the spectral problem generated by the Sturm-Liouville equation with an arbitrary complex-valued potential q(x) ∈ L 2(0, τ) and with regular (but not strengthened-regular) boundary conditions. Under certain additional assumptions, we establish necessary and sufficient conditions for a set of complex numbers to be the spectrum of such an operator.  相似文献   

5.
In the space L 2[0, π], the Sturm-Liouville operator L D(y) = ?y″ + q(x)y with the Dirichlet boundary conditions y(0) = y(π) = 0 is analyzed. The potential q is assumed to be singular; namely, q = σ′, where σL 2[0, π], i.e., qW 2 ?1 [0, π]. The inverse problem of reconstructing the function σ from the spectrum of the operator L D is solved in the subspace of odd real functions σ(π/2 ? x) = ?σ(π/2 + x). The existence and uniqueness of a solution to this inverse problem is proved. A method is proposed that allows one to solve this problem numerically.  相似文献   

6.
We consider the Sturm-Liouville operator L(y) = ?d 2 y/dx 2 + q(x)y in the space L 2[0, π], where the potential q(x) is a complex-valued distribution of the first order of singularity; i.e., q(x) = u′(x), uL 2[0, π]. (Here the derivative is understood in the sense of distributions.) We obtain asymptotic formulas for the eigenvalues and eigenfunctions of the operator in the case of the Neumann-Dirichlet conditions [y [1](0) = 0, y(π) = 0] and Neumann conditions [y [1](0) = 0, y [1](π) = 0] and refine similar formulas for all types of boundary conditions. The leading and second terms of asymptotics are found in closed form.  相似文献   

7.
We obtain uniform asymptotic formulas for the eigenvalues and eigenfunctions of the Sturm-Liouville operators L t (q) with a potential qL 1[0,1] and t-periodic boundary conditions, t ∈ (?π, π]. Using these formulas, we find sufficient conditions on the potential q such that the number of spectral singularities in the spectrum of the Hill operator L(q) in L 2(?∞,∞) is finite. Then we prove that the operator L(q) has no spectral singularities at infinity and it is an asymptotically spectral operator provided that the potential q satisfies sufficient conditions.  相似文献   

8.
We study the Sturm-Liouville operator L = ?d 2/dx 2 + q(x) in the space L 2[0, π] with the Dirichlet boundary conditions. We assume that the potential has the form q(x) = u′(x), uW 2 θ [0, π], 0 < θ < 1/2. We consider the problem on the uniform (on the entire interval [0, π]) equiconvergence of the expansion of a function f(x) in a series in the system of root functions of the operator L with its Fourier expansion in the system of sines. We show that if the antiderivative u(x) of the potential belongs to any of the spaces W 2 θ [0, π], 0 < θ < 1/2, then the equiconvergence rate can be estimated uniformly over the ball u(x) ∈ B R = {v(x) ∈ W 2 θ [0, π] | ∥vW 2 θ R} for any function f(x) ∈ L 2[0, π].  相似文献   

9.
We study a boundary-value periodic problem for the quasilinear equationu ff ?u xx =F[u,u f u x ],u(0,t) =u (π,t),u (x, t + π/q) =u(x, t), 0 ≤xπ,t ∈ ?,q ∈ ?. We establish conditions under which the theorem on the uniqueness of a smooth solution is true.  相似文献   

10.
《Journal of Number Theory》1986,23(2):183-194
Several effective results are proved about oscillatory properties of π(x, q, l1) − π(x, q, l2) and related functions assuming the General Riemann Hypothesis and the absence of real zeros of L-functions.  相似文献   

11.
12.
This paper deals with the behavior of the nonnegative solutions of the problem $$- \Delta u = V(x)u, \left. u \right|\partial \Omega = \varphi (x)$$ in a conical domain Ω ? ? n , n ≥ 3, where 0 ≤ V (x) ∈ L1(Ω), 0 ≤ ?(x) ∈ L1(?Ω) and ?(x) is continuous on the boundary ?Ω. It is proved that there exists a constant C *(n) = (n ? 2)2/4 such that if V 0(x) = (c + λ 1)|x|?2, then, for 0 ≤ cC *(n) and V(x) ≤ V 0(x) in the domain Ω, this problem has a nonnegative solution for any nonnegative boundary function ?(x) ∈ L 1(?Ω); for c > C *(n) and V(x) ≥ V 0(x) in Ω, this problem has no nonnegative solutions if ?(x) > 0.  相似文献   

13.
For a continuous 2π-periodic real-valued function K(t), whose amplitudes decrease as a geometric progression with a denominator q ∈ (0, 1) starting from a given number n ∈ ?, we find sharp upper bounds for q ensuring that K(t) satisfies the Nagy condition N* n .  相似文献   

14.
We consider a boundary value problem where f(x) ∈ Lp(R), p ∈ [1,∞] (L(R) ≔ C(R) and 0 ≤ q(x) ∈ Lloc1( R). Boundary value problem (0.1) is called correctly solvable in the given space Lp(R) if for any f(x) ∈ Lp(R) there is a unique solution y(x) ∞ Lp(R) and the following inequality holds with absolute constant c(p) ∈ (0,∞). We find criteria for correct solvability of the problem (0.1) in Lp(R).  相似文献   

15.
Recently B. Simon proved a remarkable theorem to the effect that the Schrödinger operatorT=?Δ+q(x) is essentially selfadjoint onC 0 (R m if 0≦qL 2(R m). Here we extend the theorem to a more general case,T=?Σ j =1/m (?/?x j ?ib j(x))2 +q 1(x) +q 2(x), whereb j, q1,q 2 are real-valued,b jC(R m),q 1L loc 2 (R m),q 1(x)≧?q*(|x|) withq*(r) monotone nondecreasing inr ando(r 2) asr → ∞, andq 2 satisfies a mild Stummel-type condition. The point is that the assumption on the local behavior ofq 1 is the weakest possible. The proof, unlike Simon’s original one, is of local nature and depends on a distributional inequality and elliptic estimates.  相似文献   

16.
We consider the Sturm-Liouville operator L = ?d 2/dx 2 + q(x) with the Dirichlet boundary conditions in the space L 2[0, π] under the assumption that the potential q(x) belongs to W 2 ?1 [0, π]. We study the problem of uniform equiconvergence on the interval [0, π] of the expansion of a function f(x) in the system of eigenfunctions and associated functions of the operator L and its Fourier sine series expansion. We obtain sufficient conditions on the potential under which this equiconvergence holds for any function f(x) of class L 1. We also consider the case of potentials belonging to the scale of Sobolev spaces W 2 ?θ [0, π] with ½ < θ ≤ 1. We show that if the antiderivative u(x) of the potential belongs to some space W 2 θ [0, π] with 0 < θ < 1/2, then, for any function in the space L 2[0, π], the rate of equiconvergence can be estimated uniformly in a ball lying in the corresponding space and containing u(x). We also give an explicit estimate for the rate of equiconvergence.  相似文献   

17.
We consider the spectral problem generated by the Sturm-Liouville operator with an arbitrary complex-valued potential q(x) ?? L 1(0, ??) and with degenerate boundary conditions. We show that, under some additional condition, the system of root functions of that operator is not a basis in the space L 2(0, ??).  相似文献   

18.
The spectral problem for the Sturm–Liouville operator with an arbitrary complex-valued potential q(x) of the class L1(0, π) and degenerate boundary conditions is considered. We prove that the system of root functions of this operator is not a basis in the space L2(0, π).  相似文献   

19.
We consider weak solutions to the nonlinear boundary value problem (r, (x, u(x)) u′(x))′ = (Fu)′(x) with r(0, u(0)) u′(0) = ku(0), r(L, u(L)) u′(L) = hu(L) and k, h are suitable elements of [0, ∞]. In addition to studying some new boundary conditions, we also relax the constraints on r(x, u) and (Fu)(x). r(x, u) > 0 may have a countable set of jump discontinuities in u and r(x, u)?1?Lq((0, L) × (0, p)). F is an operator from a suitable set of functions to a subset of Lp(0, L) which have nonnegative values. F includes, among others, examples of the form (Fu)(x) = (1 ? H(x ? x0)) u(x0), (Fu)(x) = ∫xLf(y, u(y)) dy where f(y, u) may have a countable set of jump discontinuities in u or F may be chosen so that (Fu)′(x) = ? g(x, u(x)) u′(x) ? q(x) u(x) ? f(x, u(x)) where q is a distributional derivative of an L2(0, L) function.  相似文献   

20.
For the class W(r)Lq (M;a, b), 1≤q≤∞, we construct the best method of approximation of the functionalf (x), x∈ [a, b], among all the methods using only information about the values off (k)(xi) (k=0, 1, ..., r?1; i=1, 2, ..., N).  相似文献   

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