Abstract
The 3-dimensional plane wave is the product of one-dimensional plane waves and the kinetic energy is the sum of the contributions of motions along x, y, z. More generally, the problem is separable into Cartesian coordinates if the potential energy is of the form
where \(U_{x}(x), U_{y}(y)\) e \(U_{z}(z)\) are arbitrary functions.
The partial differential equations are quite a bit harder to solve than the ordinary ones, unless the symmetry allows us to separate the variables. Fortunately, among the most interesting stationary problems, there are some that can be solved analytically.
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Notes
- 1.
Lev Davidovic Landau (Baku 1908- Moscow 1968), was the most important Soviet physicist. He won the Nobel prize in 1962 for his works on superfluid He.
- 2.
The special role of the y direction is due to the gauge; by a gauge transformation we can rotate the pair x, y as we like.
- 3.
Recall that
$$ \delta (g(x))= { \sum _{\alpha } \delta \left( x-x_{\alpha } \right) \over \left| {d g \over d x} \right| }. $$.
- 4.
W. Pauli, Z. Phys. 36, 336 (1926).
- 5.
The states with \(l=0,1,2,3, \ldots \), are called s, p, d, f, g, h, i, etc., and so on, in alphabetic order.
- 6.
An ad hoc model by N. Bohr in 1913 gave the same levels but nothing else.
- 7.
The associated Laguerre polynomials
$$ L_{q-p}^{p}(x)= (-1)^{p}\left( {d \over dx} \right) ^{p} L_{q}(x) $$are defined in terms of the Laguerre polynomials
$$ L_{q}(x) =e^{x}\left( {d \over dx} \right) ^{q} \left( e^{-x}x^{q}\right) . $$.
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Cini, M. (2018). Stationary States of One Particle in 3 Dimensions. In: Elements of Classical and Quantum Physics. UNITEXT for Physics. Springer, Cham. https://doi.org/10.1007/978-3-319-71330-4_17
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DOI: https://doi.org/10.1007/978-3-319-71330-4_17
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