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Ground-state of He-like ions

let us consider the helium ground state. As a first step, we solve the Hartree-Fock equation [Pg.144]

To go further, we must evaluate the higher-order corrections. Setting a = 6 = Is in [Pg.145]

Partial wave contributions (a.u.) to the second-order ground-state energy in helium. [Pg.146]

we obtain the following simple expression for the second-order energy  [Pg.146]

Taking the radial wave functions and energies for states n from the B-spline basis set, we may easily carry out the double sums in (128). The partial-wave contributions to from terms in square bracket are listed in Table 2. These terms fall-off approximately as L for large L and may easily be extrapolated. We find E = —0.0373736 a.u., leading to a binding energy of -0.8990800 a.u., differing from experiment by 0.5%. [Pg.146]


Lowdin, P.-O., and Redei, L., Combined use of the methods of superposition of configurations and correlation factor on the ground states of He-like ions."... [Pg.359]

Interesting results were found for the partial wave expansions. If one expands the wave function of the ground state of He-like ions as... [Pg.746]


See other pages where Ground-state of He-like ions is mentioned: [Pg.144]    [Pg.178]   


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Ground State of

He + ,- states

He-like

He-like ions

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