
PROGRAM LIBRARY JINRLIB KANTBP  a program package for solution of twodimensional discrete and continuum spectra boundaryvalue problems in Kantorovich (adiabatic) approach 

Language: Fortran 77. Operating system: OC Linux, Unix AIX 5.3, SunOS 5.8, Solaris, Windows XP KANTBP 3.0  new version of a program for computing energy levels, reflection and transmission matrices, and corresponding wave functions in the coupledchannel adiabatic approach KANTBP 2.0  new version of a program for computing energy levels, reaction matrix and radial wave functions in the coupledchannel hyperspherical adiabatic approach KANTBP  a program for computing energy levels, reaction matrix and radial wave functions in the coupledchannel hyperspherical adiabatic approach ODPEVP  a program for computing eigenvalues and eigenfunctions and their first derivatives with respect to the parameter of the parametric selfadjoined SturmLiouville problem POTHMF  a program for computing potential curves and matrix elements of the coupled adiabatic radial equations for a hydrogenlike atom in a homogeneous magnetic field
Authors: A.A.Gusev, O.Chuluunbaatar, S.I.Vinitsky, A.G.Abrashkevich A FORTRAN 77 program for calculating energy values, reflection and transmission matrices, and corresponding wave functions in a coupledchannel approximation of the adiabatic approach is presented. In this approach, a multidimensional Schrödinger equation is reduced to a system of the coupled secondorder ordinary differential equations on a finite interval with the homogeneous boundary conditions of the third type at the left and rightboundary points for continuous spectrum problem, or a set of first, second and third type boundary conditions for discrete spectrum problem. The resulting system of these equations containing the potential matrix elements and firstderivative coupling terms is solved using highorder accuracy approximations of the finite element method. Efficiency of the schemes proposed is demonstrated on an example of solution of quantum transmittance problem for a pair of coupled ions through the repulsive Coulomb barriers. As a test desk, the program is applied to the calculation of the reflection and transmission matrices and corresponding wave functions for the twodimensional problem with different barrier potentials. Sources and detailed description (pdf) are submitted. KANTBP 2.0  NEW VERSION OF A PROGRAM FOR COMPUTING ENERGY LEVELS, Authors: O.Chuluunbaatar, A.A.Gusev, S.I.Vinitsky, A.G.Abrashkevich Nature of problem: In the hyperspherical adiabatic approach [35], a multidimensional Schrödinger equation for a twoelectron system [6] or a hydrogen atom in magnetic field [79] is reduced by separating radial coordinate ρ from the angular variables to a system of the secondorder ordinary differential equations containing the potential matrix elements and firstderivative coupling terms. The purpose of this paper is to present the finite element method procedure based on the use of highorder accuracy approximations for calculating approximate eigensolutions of the continuum spectrum for such systems of coupled differential equations on finite intervals of the radial variable ρ ∈ [ρ_{min}, ρ_{max}]. This approach can be used in the calculations of effects of electron screening on lowenergy fusion cross sections [1012]. Solution method: The boundary problems for the coupled secondorder differential equations are solved by the finite element method using highorder accuracy approximations [13]. The generalized algebraic eigenvalue problem AF = EBF with respect to pair unknowns (E,F) arising after the replacement of the differential problem by the finiteelement approximation is solved by the subspace iteration method using the SSPACE program [14]. The generalized algebraic eigenvalue problem (A EB)F = λDF with respect to pair unknowns (λ,F) arising after the corresponding replacement of the scattering boundary problem in open channels at fixed energy value, E, is solved by the LDL^{T} factorization of symmetric matrix and backsubstitution methods using the DECOMP and REDBAK programs, respectively [14]. As a test desk, the program is applied to the calculation of the reaction matrix and corresponding radial wave functions for 3Dmodel of a hydrogenlike atom in a homogeneous magnetic field described in [9] on finite intervals of the radial variable ρ ∈ [ρ_{min}, ρ_{max}]. For this benchmark model the required analytical expressions for asymptotics of the potential matrix elements and firstderivative coupling terms, and also asymptotics of radial solutions of the boundary problems for coupled differential equations have been produced with help of a MAPLE computer algebra system.
Restrictions: The computer memory requirements depend on: Restrictions due to dimension sizes may be easily alleviated by altering PARAMETER statements (see Long Write Up and listing of [1] for details). The user must also supply subroutine POTCAL for evaluating potential matrix elements. The user should also supply subroutines ASYMEV (when solving the eigenvalue problem) or ASYMS0 and ASYMSC (when solving the scattering problem) which evaluate asymptotics of the radial wave functions at left and right boundary points in case of a boundary condition of the third type for the above problems. Running time: The running time depends critically upon: The test run which accompanies this paper took 2s without calculation of matrix potentials on the Intel Pentium IV 2.4 GHz. External routines: GAULEG and GAUSSJ [2] For details see: http://cpc.cs.qub.ac.uk/summaries/ADZH_v2_0.html References:
KANTBP  A PROGRAM FOR COMPUTING ENERGY LEVELS, REACTION MATRIX AND RADIAL Authors: O.Chuluunbaatar, A.A.Gusev, A.G.Abrashkevich, A.AmayaTapia, M.S.Kaschiev, S.Y.Larsen, S.I.Vinitsky Nature of problem: In the hyperspherical adiabatic approach [24], a multidimensional Schrödinger equation for a twoelectron system [5] or a hydrogen atom in magnetic field [6] is reduced by separating the radial coordinate ρ from the angular variables to a system of secondorder ordinary differential equations which contain potential matrix elements and firstderivative coupling terms. The purpose of this paper is to present the finite element method procedure based on the use of highorder accuracy approximations for calculating approximate eigensolutions for such systems of coupled differential equations. Solution method: The boundary problems for coupled differential equations are solved by the finite element method using highorder accuracy approximations [7]. The generalized algebraic eigenvalue problem A F = E B F with respect to pair unknowns (E, F) arising after the replacement of the differential problem by the finiteelement approximation is solved by the subspace iteration method using the SSPACE program [8]. The generalized algebraic eigenvalue problem (A  EB)F = λD F with respect to pair unknowns (λ,F) arising after the corresponding replacement of the scattering boundary problem in open channels at fixed energy value, E, is solved by the L D L^{T} factorization of symmetric matrix and backsubstitution methods using the DECOMP and REDBAK programs, respectively [8]. As a test desk, the program is applied to the calculation of the energy values and reaction matrix for an exactly solvable 2Dmodel of three identical particles on a line with pair zerorange potentials described in [912]. For this benchmark model the needed analytical expressions for the potential matrix elements and firstderivative coupling terms, their asymptotics and asymptotics of radial solutions of the boundary problems for coupled differential equations have been produced with help of a MAPLE computer algebra system.
Restrictions: The computer memory requirements depend on: Restrictions due to dimension sizes may be easily alleviated by altering PARAMETER statements (see Long WriteUp and listing for details). The user must also supply subroutine POTCAL for evaluating potential matrix elements. The user should supply subroutines ASYMEV (when solving the eigenvalue problem) or ASYMSC (when solving the scattering problem) that evaluate the asymptotics of the radial wave functions at the right boundary point in case of a boundary condition of the third type, respectively. Running time: The running time depends critically upon: External routines: GAULEG and GAUSSJ [1] See also: http://cpc.cs.qub.ac.uk/summaries/ADZH_v1_0.html References:
ODPEVP  A PROGRAM FOR COMPUTING EIGENVALUES AND EIGENFUNCTIONS AND Authors: O.Chuluunbaatar, A.A.Gusev, S.I.Vinitsky, A.G.Abrashkevich Nature of problem: The threedimensional boundary problem for the elliptic partial differential equation with an axial symmetry similar to the Schrödinger equation with the Coulomb and transverse oscillator potentials is reduced to the twodimensional one. The latter finds wide applications in modeling of photoionization and recombination of oppositively charged particles (positrons, antiprotons) in the magnetoptical trap [4], optical absorption in quantum wells [5], and channeling of likely charged particles in thin doped films [6,7] or neutral atoms and molecules in artificial waveguides or surfaces [8,9]. In the adiabatic approach [10] known in mathematics physics as Kantorovich method [11] the solution of the twodimensional elliptic partial differential equation is expanded over basis functions with respect to the fast variable (for example, angular variable) and depended on the slow variable (for example, radial coordinate) as a parameter. An averaging of the problem by such a basis leads to a system of the secondorder ordinary differential equations which contain potential matrix elements and the firstderivative coupling terms, (see, e.g., [12,13,14]). The purpose of this paper is to present the finite element method procedure based on the use of highorder accuracy approximations for calculating eigenvalues, eigenfunctions and their first derivatives with respect to the parameter of the parametric selfadjoined SturmLiouville problem with the parametric third type boundary conditions on the finite interval. The program developed calculates potential matrix elements  integrals of the eigenfunctions multiplied by their derivatives with respect to the parameter. These matrix elements can be used for solving the bound state and multichannel scattering problems for a system of the coupled secondorder ordinary differential equations with the help of the KANTBP programs [1,2]. Solution method: The parametric selfadjoined SturmLiouville problem with the parametric third type boundary conditions is solved by the finite element method using highorder accuracy approximations [15]. The generalized algebraic eigenvalue problem AF = EBF with respect to a pair of unknown (E,F) arising after the replacement of the differential problem by the finiteelement approximation is solved by the subspace iteration method using the SSPACE program [16]. First derivatives of the eigenfunctions with respect to the parameter which contained in potential matrix elements of the coupled system equations are obtained by solving the inhomogeneous algebraic equations. As a test desk, the program is applied to the calculation of the potential matrix elements for an integrable 2Dmodel of three identical particles on a line with pair zerorange potentials described in [1,17,18], a 3Dmodel of a hydrogen atom in a homogeneous magnetic field described in [14,19] and a hydrogen atom on a threedimensional sphere [20]. Restrictions: The computer memory requirements depend on: Restrictions due to dimension sizes may be easily alleviated by altering PARAMETER statements. The user must also supply DOUBLE PRECISION functions POTCCL and POTCC1 for evaluating potential function U(ρ,z) of Eq.(1) and its first derivative with respect to parameter ρ. The user should supply DOUBLE PRECISION functions F1FUNC and F2FUNC that evaluate functions f_{1}(z) and f_{2}(z) of Eq.(1). The user must also supply subroutine BOUNCF for evaluating the parametric third type boundary conditions. Running time: The running time depends critically upon: RAM: depends on External routines: GAULEG [3]. See also: ttp://cpc.cs.qub.ac.uk/summaries/AEDV_v1_0.html References:
POTHMF  A PROGRAM FOR COMPUTING POTENTIAL CURVES AND MATRIX ELEMENTS Authors: O.Chuluunbaatar, A.A.Gusev, V.P.Gerdt, V.A.Rostovtsev, S.I.Vinitsky, A.G.Abrashkevich, M.S.Kaschiev, V.V.Serov Nature of problem: In the multichannel adiabatic approach the Schrödinger equation for a hydrogenlike atom in a homogeneous magnetic field of strength γ (γ = B/B_{0}, B_{0} ≅ 2.35 × 10^{5}T is a dimensionless parameter which determines the field strength B) is reduced by separating the radial coordinate, r, from the angular variables, (θ, φ), and using a basis of the angular oblate spheroidal functions [3] to a system of secondorder ordinary differential equations which contain firstderivative coupling terms [4]. The purpose of this program is to calculate potential curves and matrix elements of radial coupling needed for calculating the lowlying bound and scattering states of hydrogenlike atoms in a homogeneous magnetic field of strength 0 < γ ≤ 1000 within the adiabatic approach [5]. The program evaluates also asymptotic regular and irregular matrix radial solutions of the multichannel scattering problem needed to extract from the Rmatrix a required symmetric shortrange openchannel reaction matrix K [6] independent from matching point [7]. In addition, the program computes the dipole transition matrix elements in the length form between the basis functions that are needed for calculating the dipole transitions between the lowlying bound and scattering states and photoionization cross sections [8]. Solution method: The angular oblate spheroidal eigenvalue problem depending on the radial variable is solved using a series expansion in the Legendre polynomials [3]. The resulting tridiagonal symmetric algebraic eigenvalue problem for the evaluation of selected eigenvalues, i.e. the potential curves, is solved by the LDL^{T} factorization using the DSTEVR program [2]. Derivatives of the eigenfunctions with respect to the radial variable which are contained in matrix elements of the coupled radial equations are obtained by solving the inhomogeneous algebraic equations. The corresponding algebraic problem is solved by using the LDL^{T} factorization with the help of the DPTTRS program [2]. Asymptotics of the matrix elements at large values of radial variable are computed using a series expansion in the associated Laguerre polynomials [9]. The corresponding matching points between the numeric and asymptotic solutions are found automatically. These asymptotics are used for the evaluation of the asymptotic regular and irregular matrix radial solutions of the multichannel scattering problem [7]. As a test desk, the program is applied to the calculation of the energy values of the ground and excited bound states and reaction matrix of multichannel scattering problem for a hydrogen atom in a homogeneous magnetic field using the KANTBP program [10]. Restrictions: The computer memory requirements depend on: Restrictions due to dimension sizes can be changed by resetting a small number of PARAMETER statements before recompiling (see Long Write Up and listing for details). Running time: The running time depends critically upon: The test run which accompanies this paper took 7s required for calculating of potential curves, radial matrix elements, and dipole transition matrix elements on a finiteelement grid on interval [r_{min} = 0, r_{max} = 100] used for solving discrete and continuous spectrum problems and obtaining asymptotic regular and irregular matrix radial solutions at r_{max} = 100 for continuous spectrum problem on the Intel Pentium IV 2.4 GHz. The number of radial differential equations was equal to 6. The accompanying test run using the KANTBP program took 2s for solving discrete and continuous spectrum problems using the above calculated potential curves, matrix elements and asymptotic regular and irregular matrix radial solutions. Note, that in the accompanied benchmark calculations of the photoionization crosssections from the bound states of a hydrogen atom in a homogeneous magnetic field to continuum we have used interval [r_{min} = 0, r_{max} = 1000] for continuous spectrum problem. The total number of radial differential equations was varied from 10 to 18. See also: http://cpc.cs.qub.ac.uk/summaries/AEAA_v1_0.html References:
