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The inverse scattering problem of some Schrödinger type equation with turning point
Boundary Value Problems volume 2015, Article number: 57 (2015)
Abstract
In this paper the inverse scattering problem is considered for a version of the onedimensional Schrödinger equation with turning point on the halfline \((0, \infty)\). The scattering data of the problem is defined and the fundamental equation is derived. With the help of the derived fundamental equation, in terms of the scattering data, the potential is recovered uniquely.
Introduction and preliminaries
Introduction
Inverse problems of spectral analysis consist in recovering operators from their spectral characteristics. Such problems often appear in mathematics, mechanics, physics, electronics, geophysics, meteorology, and other branches of the natural sciences. Inverse problems also play an important role in solving nonlinear evolution equations in mathematical physics. Interest in this subject has been increasing permanently because of the appearance of new important applications, and nowadays the inverse problem theory is developed intensively all over the world. The greatest success in spectral theory in general, and in particular in inverse spectral problems, has been achieved for the SturmLiouville operator \(y:=y '' +q(x)y\), which also is called the onedimensional Schrödinger operator.
The main results on inverse spectral problems appeared in the second half of the 20th century. We mention here the works by R Beals, G Borg, LD Faddeev, MG Gasymov, IM Gelfand, BM Levitan, N Levinson, VA Marchenko, and others (see [1] for details). An important role in the inverse spectral theory for the SturmLiouville operator was played by the transformation operator method (see [2, 3] and the references therein).
At present, other effective methods for solving inverse spectral problems have been created; among them we point out the method of spectral mappings connected with ideas of the contour integration method. This method seems to offer perspective for inverse spectral problems. The created methods allowed one to solve a number of important problems in various branches of the natural sciences.
The inverse scattering theory on the halfline and on the line was studied in [4–6], and others. In [7–11] KR Mamedov studied the inverse scattering theory on the halfline with spectral parameter contained in the boundary condition. Lately, there grew interest in the investigation of the boundary value problem by numerical methods; e.g. [12] presented an approximate construction of the Jost function for some SturmLiouville boundary value problem in the case \(\rho(x) = 1 \) by means of the collocation method; in addition, [13] is an application of spectral analysis of onedimensional Schrödinger operators in a magnetic field. Also [14, 15] are applications of the discontinuous wave speed problem in a nonhomogeneous medium as in our case.
In the last 30 years there appeared many new areas for applications of inverse SturmLiouville problems, among them boundary value problems with discontinuity conditions inside the interval are connected with discontinuous material properties.
Many further applications were connected with the differential equation of the form \(y'' +q(x)y=r(x)y \) with turning points when the function \(r(x)\) has zeros and/or changes sign. For example, we have turning points connected with physical situations in which zeros correspond to the limit of motion of a wave mechanical particle bound by a potential field. Turning points appear also in elasticity, optics, geophysics, and other branches of natural sciences. Moreover, a wide class of differential equations with Besseltype singularities and their perturbations can be reduced to differential equations having turning points; further inverse problems for equations with turning points and singularities help one to study blowup solutions for some nonlinear integrable evolution equations of mathematical physics (see [16]).
Inverse problems of the SturmLiouville equation with turning points and singularities have been studied in [17–20], and other works.
The aim of the present paper is to investigate the inverse scattering problem on the halfline \([0, \infty)\) for some version of the onedimensional Schrödinger equation with turning. In the case of \(\rho(x)= 1\), the inverse problem of scattering theory for (1.1) with boundary condition not containing a spectral parameter was completely solved by Marchenko [2, 21], Levitan [3, 22], Aktosun [23], and Aktosun and Weder [24]. The discontinuous version of ρ was studied by Gasymov and Levitan [25, 26], Darwish [27], and Gasymov and the author [19, 28]. In these papers, the solution of the inverse scattering problem on the halfline \([0, \infty)\) by using the transformation operator was reduced to the solution of two inverse problems on the intervals \([0,a ]\) and \([a, \infty)\). In the case \(\rho\neq1\) the inverse scattering problem was solved by the author, Guseinov, and Pashaev [19, 29] by using the new nontriangular representation of the Jost solution of (1.1). It turns out that in this case the discontinuity of the function \(\rho(x)\) strongly influences the structure of the representation of the Jost solution and the fundamental equation of the inverse problem.
The direct and inverse problem of (1.1) with \(y(0)h y(0) = 0\) (see [21, 30]) has been solved earlier by the socalled spectral distribution function, while the problem (1.1) with \(y(0) = 0\) has been studied in the works [30, 31] by the inverse scattering method. Furthermore, the inverse scattering problem of the onedimensional Schröodinger’s eigenvalue problem with a discontinuous coefficient was studied when \(y(0) = 0\) and \(y' (0)=0\) [27, 32] and [25]. It should be mentioned that the spectrum of the boundary value problem (1.1)(1.2) has been previously investigated in [33] when \(\rho(x)>0\) and the boundary condition \(y(0)=0\) holds.
The present paper is organized as follows. Section 1 is an introduction and preliminaries in which we demonstrate some historical and scientific survey to inverse scattering problem. We introduce, from [34], the basic definitions and results that are needed in the subsequent investigation. In addition, the scattering data for the boundary value problem (1.1)(1.2) are defined and some of its spectral properties are proved. In Section 2, the main integral equation of the inverse scattering problem is derived, by its scattering data. Finally, Section 3 is devoted to a proof of the uniqueness of both the main integral equation and the solution of the inverse scattering problem.
Preliminaries
Consider the initial value problem
where
\(q(x)\) is a finite real valued function which satisfies
and η is a complex spectral parameter. In [34] the authors completely solved the direct scattering problem of the problem (1.1)(1.4), so that, following [34] we state the main definitions and results that are needed in the subsequent investigations.
The totality of the quantities
is called the scattering data of the problem (1.1)(1.4). Thus, the scattering data completely determines the behavior of the normed eigenfunctions of the problem (1.1)(1.4). Here \(S(\eta)\) is the scattering function, \(\eta_{k} = i\chi_{k}\), \(\eta_{k}^{2}\) the eigenvalues and \(m_{k}\) the normalizing numbers of the problem (1.1)(1.4), where
where \(f'(0,\eta)h f(0,\eta) = 0 \) for \(\operatorname{Re} \eta\neq0 \). From Lemmas 1.2 and 1.3 of [34], the function \(S(\eta)\) is continuous on the real line \(\infty< \eta< \infty\) and admits the properties \(\overline{S(\eta)} = S(\eta)\), \(S(\eta)=1\), \(\infty< \eta< \infty\). The eigenvalues \(\eta_{n}^{2} = (i \chi_{n})^{2} \), \(\chi_{n} > 0 \), \(n = 1,2,\ldots\) , and the normalizing numbers \(m_{n} < 0\), \(n = 1,2,\ldots \) , satisfy the asymptotic formulas
where
For all \(\operatorname{Re} \eta\neq0\) we have the following equality:
where \(\varphi(x,\eta) \) is the solution of the problem (1.1)(1.2) (\(\varphi(0,\eta) = 1\), \(\varphi'(0,\eta)=h \)), and the scattering function \(S(\eta)\) is given by (1.6) and satisfies the properties
In the following lemma we evaluate the asymptotic formula of the scattering function \(S(\eta)\).
Lemma 1.1
For \(\infty< \eta< \infty\), \( \eta\rightarrow\infty\), the scattering function \(S(\eta)\) satisfies the asymptotic formula
where
Proof
By virtue of (2.11) in [34], for \(\operatorname{Im} \eta> 0\), \(\eta\rightarrow\infty\),
from which, in the special case for \(\infty< \eta< \infty\), \( \eta\rightarrow\infty\) we have
On the other hand, it is easy to see that
from (1.15) and (1.16) we deduce, for \(\infty< \eta< \infty\), \( \eta \rightarrow\infty\), that
from which, by substitution into (1.6), the proof is completed. □
Formulation of the inverse scattering problem
The inverse scattering problem for the boundary value problem (1.1)(1.4) consists of recovering the potential function \(q(x)\) and the number h by the scattering data. For this task to be accomplished, we must answer the following two questions:

Are the coefficient \(q(x)\) and the number h uniquely defined by the scattering data (1.5) of the problem (1.1)(1.4)?

What is the effective recovering method of \(q(x)\) and h by the scattering data (1.5)?
Derivation of the main integral equation
In this section we derive the GelfandLevitan integral equation of the inverse scattering problem on the interval \((1,\infty)\); this will be accomplished through Lemmas 2.1, 2.2, and Theorem 2.1. Let \(\Lambda_{n}\) be the rectangular contour
Lemma 2.1
The following inequality holds true from below:
Proof
Let \(\eta= \sigma+ i \chi\), so that on the real line \(\chi= 0 \), \(\eta\in\Lambda_{n}\) it follows that \(\cosh \eta+ i \sinh\eta = \frac{\sqrt{2}}{2} \sqrt{e^{2\sigma}+ e^{2\sigma}}\), from which
On the other hand for η any complex number we have
by which, for \(\sigma= \pi (n+\frac{1}{4})\), it follows that
which completes the proof of the lemma. □
Since, from [34], \(f_{o}(0,\eta) = e^{i \eta} (\cosh\eta+ i \sinh\eta )\), and using Lemma 2.1, we have
Lemma 2.2
For every \(x > 1\) and \(\eta\in\Lambda_{n} \), \(n \rightarrow\infty\), we have the following asymptotic formula:
where \(S_{o}(\eta)\) is given by (1.12).
Proof
Following [2], p.19, we see that the fundamental system \(\varphi_{1}(x, \eta)\), \(\theta_{1}(x, \eta) \) of solutions of (1.1), for \(1 < x <\infty\), with conditions \(\varphi_{1}(1, \eta) = 0\), \(\varphi'_{1}(1, \eta) = 1\), \(\theta_{1}(1, \eta)=1\), \(\theta'_{1}(1, \eta)= 0\), have the representations
where the kernels \(C(x,t)\) and \(D(x,t)\) have summable first order partial derivatives [2]. For \(1 < x < \infty\) the solution \(\varphi (x, \eta) \) of (1.1) is a linear combination of \(\varphi_{1}(x, \eta)\), \(\theta_{1}(x, \eta)\), so that, for \(1 < x < \infty\),
We evaluate the asymptotic formulas for \(\varphi_{1}(x,\eta)\), \(\theta_{1}(x,\eta)\), by integrating (2.5) and (2.6) by parts, we have
Further, by virtue of (2.9) and (2.10) of [34], we have
Substituting (2.8)(2.11) into (2.7), we have
when expressing \(\sin\eta(x1) \), \(\cos \eta(x1) \), in terms of the exponential functions, (2.12) takes the form
where \(f_{o}(0,\eta) \) is given by (1.14). Again from (2.11) of [34], we have
Further, from (2.14) and (2.3), we have
From (2.13) and (2.15) we have
From (1.12), for \(\eta\in\Lambda_{n} \), \(S_{o}(\eta) \) has the asymptotic formula
by the aid of (2.17), (2.16) takes the form
which completes the proof of the lemma. □
The following theorem deals with the formulation of the main integral equation, the socalled (GelfandLevitan) integral equation of the inverse problem by its scattering data. It should be noted, here, that \(\{ S(\eta) , \eta_{k} = i \chi_{k}, m_{k} \}\) is the scattering data of the problem (1.1)(1.2) and \(\{ S_{o}(\eta) , \eta^{o}_{k} = i \chi^{o}_{k}, m^{o}_{k} \}\) is the scattering data of the problem (1.1)(1.2) with \(q(x)= 0\), \(h=0\), \(S_{o}(\eta)\) is given by (1.12)
Theorem 2.1
For \(x > 1 \), we have the following integral equation:
where
\(S_{o}(\eta)\), \(\chi^{o}_{k}\) and \(m^{o}_{k} \) are given by (2.18).
Proof
Following (1.32) and (1.14) of [34], we have
where \(\operatorname{Im} \lambda\geq0\), \(K(x,x) = \frac{1}{2} \int_{0}^{x} q(t)\, dt\), \(1< x < \infty\).
Substituting (2.22) into (2.21), we have
Multiplying both sides of (2.23) by \({\frac{e^{i\eta y}}{2 \pi}}\) and integrating with respect to η on \([ N, N ]\) where N is a positive integer, we have
For convenience, we write (2.24) in the following abbreviated form:
where
We calculate \(I_{\mathrm{CI}1}\), \(I_{\mathrm{CI}2}\) by means of contour integration over the contour \(\Lambda_{n}\), whereas, for \(I_{\mathrm{FP}1}\), \(I_{\mathrm{FP}2}\), and \(I_{\mathrm{FP}3} \), we use the FourierPlancherel formulas. First for \(I_{\mathrm{FP}1}\), we see from (1.11) that the function \([S_{o}(\eta)  S(\eta)] \in L_{2}(\infty, \infty) \), consequently, by the FourierPlancherel theorem, there exists a limiting function \(H_{S}(x) \in L_{2}(\infty, \infty)\), where
and, consequently,
Further, with the aid of the inversion formula of FourierPlancherel, we see that
exists and hence
Now, by using the contour integration method, we calculate \(I_{\mathrm{CI}1}\), \(I_{\mathrm{CI}2}\).
Let \(N_{n}=\pi ( n+\frac{1}{4} )\), where n is an arbitrary positive integer, and \(\Lambda_{n}^{+} = \Lambda_{n}  [\pi ( n+\frac{1}{4} ), \pi ( n+\frac{1}{4} ) ]\), i.e. \(\Lambda_{n}^{+}\) is the part of the contour \(\Lambda_{n}\) which lies in the upper half of imaginary axis, \(\operatorname{Im} \eta> 0\). For simplicity, denote
The function \(\Theta(x,y,\eta)\) is analytic function in the half plane \(\operatorname{Im} \eta> 0\) except for its poles \(\eta_{k}^{o} = i \chi_{k}^{o}\). We have
We prove that
in fact, using integration by parts we see that
Further, from (2.17), (2.35), and (2.38), we have
on the vertical part of \(\Lambda_{n}^{+}\), for \(\eta\in\Lambda_{n}^{+}\), we have
Similarly, for η∈ horizontal part of \(\Lambda^{+}_{n}\), we have
the proof of (2.37) is completed from (2.40) and (2.41).
With the aid of the wellknown residue formula, we have
from (1.14) it follows that \(\frac{f_{o}(0,\eta_{k}^{o})}{\dot{f}_{o}(0,\eta_{k}^{o})} =ie^{2\chi_{k}^{o}} \), for \(\eta_{k}^{o} = i\chi_{k}^{o}\), from this (2.42) becomes
From (2.37) and (2.43), (2.36) takes the form
We evaluate \(I_{\mathrm{CI}1} \). Let
consider the integration
In a similar way to the integration \(I_{\mathrm{CI}2}\), it can be seen that \({ \lim_{n\rightarrow\infty} \frac{1}{2 \pi i}\int_{\Lambda ^{+}_{n}}\Phi(x,y,\eta) \,d\eta= 0}\). Using the residue formula we have
It is easy to see that
Substituting (2.48) into (2.47), we get
From (2.49), as \(n\rightarrow\infty\), (2.29) becomes
By putting \(N=N_{n}\) in (2.25), passing to the limit as \(n\rightarrow\infty\), and taking into account (2.32), (2.33), (2.34), (2.44), and (2.50), we have
The integral equation (2.51) is still valid for \(x = y \), this can be proved by continuity of \({ K(x,y)\leq C\sigma ( \frac{x+y}{2} )} \) and the continuity of \(H(\xi)\) in the metric \(L_{2}(2,\infty)\). □
The uniqueness theorems
In this section we prove two theorems, first, the uniqueness theorem of the solution of the main integral equation (2.51) on the interval \((1,\infty)\), the second is the uniqueness of the inverse scattering problem of (1.1)(1.2) by its scattering data (1.5).
The uniqueness theorem of the main integral equation
We prove the uniqueness of the solution of the integral equation (2.51) with respect to \(K(x,t)\).
Theorem 3.1
For every fixed \(x > 1 \), the solution \(\beta(y)\in L^{2}(x,\infty)\) of the equation
is unique, where \(\alpha(y)\in L^{2}(x,\infty)\) is a given function
Proof
It is sufficient to prove that the homogeneous integral equation
has only the zero solution \(\beta(y)\equiv0 \) in the space \(L^{2}(x,\infty) \).
Beside the boundary value problem (1.1)(1.2), we consider the following boundary value problem:
with the same function \(q(x) \) of (1.1). We denote by \(J(x,\eta )\), where \(z= \eta^{2}\), the Jost solution of (3.3), with the property
We see, from [2], that this solution, uniquely, exists and has the representation
It is clear (1.1) and (3.3) are the same for \(1 < x < \infty\) and satisfy the same condition (3.4). We deduce, from the last discussion, that \(f(x,\eta) = J(x,\eta)\), \(1 < x < \infty\), from which, using (2.22), (3.6), we obtain
Let \(\widetilde{S}(\eta)\) denotes the scattering function of (3.3)(3.4). From [2], and keeping in mined that the problem (3.3)(3.4) has no negative eigenvalues, it can be seen that
where \(\widetilde{H}(x) = \frac{1}{2\pi} \int_{\infty}^{\infty }\{ 1\widetilde{S}(\eta)\} e^{i\eta x} \,d\eta \). Subtracting (3.8) from (2.51) and using (3.7), we obtain
Putting \(y = x \) in (3.9), we have the following Volterra homogeneous integral equation:
which has the zero solution with respect to \(H(2x)  \widetilde{H}(2x) \), so that
from which (3.2) is written in the form
By virtue of [2], the last equation has only the zero solution \(\beta(y)=0\). □
The uniqueness theorem of inverse scattering problem
Theorem 3.2
The scattering data
of the problem (1.1)(1.2) uniquely defines the potential \(q(x)\) of (1.1) and the number h of the condition (1.2).
Proof
In Theorem 2.1, we have constructed the function \(H(x)\), \(x> 2 \), and used it to derive the main integral equation by the scattering data (3.13). From (2.22) we have \(q(x) = 2\frac {d}{dx}K(x,t)\), also from Theorem 3.1, the function \(K(x,t)\) is unique for \(1 < x <\infty\) and consequently the potential \(q(x)\), \(1 < x <\infty\), is unique. As a consequence of the uniqueness of \(q(x) \) the functions \(f(1,\eta)\) and \(f'(1,\eta)\) are uniquely defined.
We prove, now, the uniqueness of \(q(x)\) for \(0\leq x \leq1\). Consider the solution \(\phi(x,\eta)\), \(0\leq x \leq1\), of the problem (1.1) satisfying the initial conditions \(\phi(0,\eta)=1\), \(\phi '(0,\eta) = h \). Let \(W[f,\phi]\) be the Wronskian of the two independent solutions \(f(x,\eta)\), \(\phi(x,\eta)\). By virtue of \(W_{x=1}= W_{x=0}\), we have
Replacing η by −η and keeping in mind that \(\phi(x,\eta) = \phi(x,\eta)\), we have
Solving (3.14) and (3.15) for \(\phi(1,\eta)\), \(\phi '(1,\eta)\), then dividing the results by \(f'(0,\eta)  h f(0,\eta)\), we obtain
from which we have
It should be noted, here, that the function \(N(\eta)\) defined by (3.17) is well defined because of the uniqueness of \(f(1,\eta)\), \(f'(1,\eta)\). The functions \(\phi(1,\eta) \), \(\phi'(1,\eta) \) are entire functions, and then \(N(\eta)\) is a meromorphic function for \(\infty < \eta< \infty\); indeed, by analytic continuation, it is meromorphic in the whole complex plane. Further, the zeros and poles of \(N(\eta)\) are the roots of the equations
respectively. On the other hand, (3.18), (3.19) are regarded as the characteristic equations of the two boundary value problems
The two spectra of (3.20) and (3.21) can be considered known, so that, arguing as in [26], we deduce the uniqueness of \(q(x)\), \(0\leq x \leq 1\). It remains to prove that the number h of the boundary condition (1.2) is uniquely defined by (3.13).
Beside the boundary value problem (1.1)(1.2), consider the boundary value problem of (1.1) subject to the initial condition
with the same weight function \(\rho(x)\) and potential \(q(x) \) of (1.1). Denote by \({\{\eta_{n}\}_{n=1}^{\infty}}\) and \({\{ \widetilde{\eta}_{n}\}_{n=1}^{\infty}}\), the eigenvalues of (1.1)(1.2) and (1.1)(3.22), respectively. Let the characteristic equations of (1.1)(1.2) and (1.1)(3.22) be \(\Phi(\eta)= 0 \) and \(\Phi_{1}(\eta) = 0\), respectively, where
where \(f(x,\eta)\) is the solution of (1.1)(1.2) subject to \(f(0,\eta) = 1\), \(f'(0,\eta) = h\). From (2.21) of [34] and (3.24) we have
From (3.23), (3.24), and (3.25) we have
The functions \(\dot{\Phi}(\eta)\) and \(\Phi_{1}(\eta)\) as entire functions are written in the form
where the constants C, \(C_{1}\) are uniquely defined with the help of the asymptotic formulas
and \(W_{o}(\eta)= e^{i \eta}(\cosh\eta+ i \sinh\eta)\). From (3.26) and (3.27) we see that \(hh_{1}\) is uniquely defined; moreover, h is uniquely defined by (1.19) of [34], \(h = A(0,0)\), so that \(h_{1}\) is uniquely defined, which completes the proof. □
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Acknowledgements
We are indebted to an anonymous referee for a detailed reading of the manuscript and useful comments and suggestions, which helped us improve this work. This work is supported by Office of Scientific Publishing Excellence of Alexandria University.
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ElRaheem, Z.F., Salama, F.A. The inverse scattering problem of some Schrödinger type equation with turning point. Bound Value Probl 2015, 57 (2015). https://doi.org/10.1186/s1366101503166
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MSC
 58C40
 34L25
 34B05
 47A40
Keywords
 Schrödinger equation
 scattering function
 asymptotic formula
 contour integration
 main integral equation
 uniqueness theorem
 inverse scattering problem