Rayleigh - Schrödinger perturbation series
for two-dimensional anharmonic oscillator
wx2 x2/2 + wy2 y2/2 +
g1/2 x y2
| H = H0 + g1/2 x y2 |
Hamiltonian of the problem |
| E(g) = E0 + E1 g + ...
+ EN gN |
Perturbation expansion of energy |
| H0 = px2/2 + py2/2
+ wx2 x2/2 + wy2 y2/2 |
Hamiltonian of harmonic oscillator |
| E0 = (nx + 1/2)wx
+ (ny + 1/2)wy |
Unperturbed harmonic-oscillator energy |
| wx, wy |
Frequencies of normal-mode vibrations |
| g |
Small perturbation parameter |
| nx, ny |
Harmonic oscillator quantum numbers |
| N |
Order of perturbation theory |
|

Mathematica
program for this calculation

19
coefficients for
nx=9, ny=1,
wx=1, wy=11/10 in exact form
calculated earlier

4 coefficients for
nx=9, ny=1,
wx=1 and arbitrary wy in exact form
calculated earlier

110 coefficients for wx=1, wy=1.1, and
nx=0, nx=0,
nx=0, nx=1,
nx=0, nx=2,
nx=0, nx=4,
nx=1, nx=0,
nx=1, nx=2,
nx=2, nx=0,
nx=2, nx=1,
nx=2, nx=2,
nx=3, nx=0,
nx=3, nx=1,
nx=4, nx=0,
nx=5, nx=0,
calculated earlier

On-line
calculation of Rayleigh - Schrödinger perturbation series

Online
calculations
Designed by A. Sergeev