A method implemented here for the numerical solution of the gpe consists in obtaining the hartree potential iteratively, starting with the thomas fermi approximation to this potential. Trefethen, spectral methods in matlab, siam, philadelphia, 2000. Siam journal on numerical analysis siam society for. A spectral method in time for initialvalue problems. The employed method is based on chebyshevgausslobbato quadrature. Solution of the schrtidinger equation by a spectral method m. The timesplitting fourier spectral method for the coupled. Journal of applied mathematics and physics, 4, 16001609. In pure mathematics, the schrodinger equation and its variants is one of the basic equations studied in. Three sets of analytical solution are obtained if the factor rl is not neglected. Mixed fourierlegendre spectral methods for the multiple. The space variable is discretized by means of a finite difference and a fourier. Abstract the solution of a radial schrodinger equation for. The dynamics of onesoliton solution and twosoliton interactions are also.
The equation with ux ax2results from schrodingers equation for a free particle with n space coordinates if one passes to spherical cylindrical coordinates and separates the angular variables. The spectral method utilizes numerical solutions to the time. Let us begin by considering how the lowest energy state wave function is affected by having finite instead of. Journal of computational physics 47, 412433 1982 solution of the schrodinger equation by a spectral method m. I have little to add but if you need some explanation on the basics of spectral method you may read lloyd n. Solution of the schrtidinger equation by a spectral method. Suppose wx,t is a solution of the schrodinger equation in question. There is n o tru e deriv ation of thi s equ ation, b ut its for m can b e m oti vated b y p h ysical and mathematic al argu m en ts at a wid e var iety of levels of sophi stication. Steiger university of california, lawrence livermore national laboratory, livermore, calfornia 94550 received. The fgh is a pseudospectral method and yields a simple recipe for constructing the discretized. Basis set expansion method the orbital i in the rhf equation is a function of a set of oneelectron variables, x 1, y 1, z 1, and thus it can be represented by an expansion in a basis set.
Quantum mechanics numerical solutions of the schrodinger. A spectral integral equation solution of the gross. Conventional methods for solving this problem rely on. Et any linear combination of stationary states each with a different allowed energy of the system is also a valid. However, physically interpreting the wave is one of the main philosophical problems of. Large timestepping spectral methods for the semiclassical. On the timesplitting fourier spectral method for the. About general solutions to schrodinger equation physics. It is a classical field equation whose principal applications are to. Multisymplectic fourier pseudospectral method for the kawahara equation volume 16 issue 1 yuezheng gong, jiaxiang cai, yushun wang skip to main content accessibility help we use. The solution to this equation is a wave that describes the quantum aspects of a system. Numerical methods for a class of generalized nonlinear. A simple and systematic algorithm based on the perfectly matched layer pml method and spectral element method sem is introduced to solve the 3d schrodinger equation with tensor effective mass.
The last equation we can solve by the quadratures method 23. Abstract a new computational method for determining the eigenvalues and eigenfunctions of the schrodinger equation is described. Then the spectral collocation method using nonpolynomial basis functions is adopted for spatial discretization. Siam journal on scientific computing siam society for. How can i write the schrodinger code with spectral method. Multisymplectic fourier pseudospectral method for the. What is the schrodinger equation, and how is it used.
422 11 1640 79 608 385 1466 288 1204 1057 1152 1565 1252 554 213 1041 233 409 18 1246 331 811 1316 1396 721 1308 99 275 1153 727 179 1176 446 4 268 1350 897 1223 88 1398 354 827 1477 1357