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Hydrogen atom energy eigenfunctions

It is of interest to calculate the energy corresponding to the single eigenfunction p (or hydrogen atom that would result if the electron... [Pg.44]

The system to be treated consists of two nuclei A and B and two electrons 1 and 2. In the unperturbed state two hydrogen atoms are assumed, so that the zeroth-order energy is 2WH-If the first electron is attached to nucleus A and the second to nucleus B, the zeroth-order eigenfunction is ip (1)

zeroth-order energy, so that the system... [Pg.48]

We shall next consider whether or not the antisymmetric eigenfunction Hl for two hydrogen atoms (Equation 29b) would lead to an excited state of the hydrogen molecule. The perturbation energy is found to be... [Pg.55]

Figure 7.1 Radial eigenfunctions Pn((r) = rR fr) for the electron in the hydrogen atom (in atomic units) where n is the principal quantum number, Figure 7.1 Radial eigenfunctions Pn((r) = rR fr) for the electron in the hydrogen atom (in atomic units) where n is the principal quantum number, <f the orbital angular momentum. Note that all functions start with a positive slope given by P g(r) rf 1, have n — i — 1 zero crossings (nodes), and go outside the atomic region to zero with P Ar) e, l " where tn( is the single-particle energy of the electron in the orbital n<f. From J. C. Slater, Quanthum theory of atomic structure (1960) with kind permission of J. F. Slater and The...
The ionization limit of the Schrodinger equation and its eigenfunctions for the free hydrogen atom, at a vanishing energy value, corresponds to Bessel functions in the radial coordinate as known in the literature and illustrated in 2.1. The counterparts for paraboloidal [21], hyperboloidal [9], and polar angle [22] coordinates have also been shown to involve Bessel functions. These limits and their counterparts for the other coordinates are reviewed successively in this section. [Pg.91]

Energy eigenvalue and eigenfunction for hydrogen atom> polar coordinate expression of Hamiltonian... [Pg.22]

For the particle in a box with infinitely high walls and for the harmonic oscillator, there are no continuum eigenfunctions, whereas for the hydrogen atom we do have continuum functions. Explain this in terms of the nature of the potential-energy function for each problem. [Pg.159]

In Section 2 we define the symmetrized hyperspherical coordinates for the electron-hydrogen atom system and express the hamiltonian in these coordinates. In Section 3 symmetry is discussed. The appropriate symmetry wave functions are introduced in Section 4, the local surface eigenfunctions and energy eigenvalues in Section 5, and the scattering equations and asymptotic analysis in Section 6. Finally, some representative results are given and discussed in Section 7 and a summary of the conclusions is presented in Section 8. [Pg.193]


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See also in sourсe #XX -- [ Pg.742 , Pg.743 , Pg.744 , Pg.760 , Pg.1280 ]




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