9.12: Numerical Solutions for Morse Oscillator

Quantum Tutorials · LibreTexts

0%

Contents

    Text

    Size
    100%
    Theme
    Typeface
    Line length
    Spacing

    From LibreTexts, under CC BY 4.0, as the source states it; its equations are written in TeX, which the PDF shows typeset. This page at LibreTexts.

    9.12: Numerical Solutions for Morse Oscillator

    Schrödinger's equation is integrated numerically for the first three energy states for the Morse oscillator. The integration algorithm is taken from J. C. Hansen, J. Chem. Educ. Software, 8C2, 1996.

    Set parameters:

    n = 300

    xmin = -2

    xmax = 12

    \[ \Delta = \frac{xmax - xmin}{n-1} \nonumber \]

    \( \mu\) = 1

    D = 2

    \( \beta\) = 2

    xe = 0

    Calculate position vector, the potential energy matrix, and the kinetic energy matrix. Then combine them into a total energy matrix.

    i = 1 .. n j = 1 .. n xi = xmin + (i - 1) \( \Delta\)

    \[ V_{i,~j} = if \bigg[ i =j,~D [ 1 - exp [ \beta ( x_i - x_e )]]^2 ,~0 \bigg] \nonumber \]

    \[ T_{i,~j} = if \left[ i=j, \frac{ \pi ^{2}}{6 \mu \Delta ^{2}}, \frac{ (-1)^{i-j}}{ (i-j)^{2} \mu \Delta^{2}} \right] \nonumber \]

    Hamiltonian matrix: H = T + V

    Find eigenvalues: E = sort(eigenvals(H))

    Display three eigenvalues: m = 1 .. 3

    Em =

    \( \begin{array}{|r|}
    \hline \\
    0.8750 \\
    \hline \\
    1.8750 \\
    \hline \\
    2.0596 \\
    \hline
    \end{array} \)

    Calculate associated eigenfunctions:

    k = 1 .. 3

    \[ \psi (k) = eigenvec (H, E_k) \nonumber \]

    Plot the potential energy and selected eigenfunctions:

    Screen Shot 2019-02-06 at 7.32.57 PM.png

    For \(V = ax^n\), the virial theorem requires the following relationship between the expectation values for kinetic and potential energy:

    \[<T> = 0.5n<V>. \nonumber \]

    The calculations below show that virial theorem is not satisfied for the Morse oscillator. The reason is revealed in the following series expansion in \(x\). The expansion contains cubic, quartic and higher order terms in \(x\), so the virial theorem does not apply to the quartic oscillator.

    \( D (1 - exp( - \beta x))^2\) converts to the series \( D \beta ^2 x^2 + (-D) \beta ^3 x^3 + \frac{7}{12} D \beta ^4 x^4 + O(x^5)\)

    \( \begin{pmatrix}
    "Kinetic~Energy" & "Potential~Energy" & "Total~Energy" \\
    \psi (1)^{T} T \psi(1) & \psi (1)^{T} V \psi(1) & E_{1} \\
    \psi (2)^{T} T \psi(2) & \psi (2)^{T} V \psi(2) & E_{2}
    \end{pmatrix} = \begin{pmatrix}
    "Kinetic~Energy" & "Potential~Energy" & "Total~Energy" \\
    0.3750 & 0.5000 & 0.8750 \\
    0.3754 & 1.4996 & 1.8750
    \end{pmatrix} \)


    This page titled 9.12: Numerical Solutions for Morse Oscillator was last modified on Wed, 11 Jan 2023 07:23:42 GMT and is shared under a CC BY 4.0 license and was authored, remixed, and/or curated by Frank Rioux via source content that was edited to the style and standards of the LibreTexts platform.