# The hydrogen atom without external fields

Chapter

## Abstract

Schrödinger’s equation
and in Hartree’s atomic units (see Introductory Remarks) is

^{3}in c.g.s. units for an electron in the field of a nucleus of charge*Ze*and of infinite mass is$$\Delta u + \frac{{2m}}{{{\hbar ^2}}}(E + \frac{{Z{e^2}}}{r})u = 0$$

(1.1)

$$\Delta u + 2(E + \frac{Z}{r})u = 0$$

(1.1’)

### Keywords

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### References

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