Hartree equation

In 1927, a year after the publication of the Schrödinger equation, Hartree formulated what are now known as the Hartree equations for atoms, using the concept of self-consistency that Lindsay had introduced in his study of many electron systems in the context of Bohr theory.[1] Hartree assumed that the nucleus together with the electrons formed a spherically symmetric field. The charge distribution of each electron was the solution of the Schrödinger equation for an electron in a potential , derived from the field. Self-consistency required that the final field, computed from the solutions, was self-consistent with the initial field, and he thus called his method the self-consistent field method.

  1. ^ Lindsay, Robert Bruce (1924). "On the Atomic Models of the Alkali Metals". Journal of Mathematics and Physics. 3 (4). Wiley: 191–236. Bibcode:1924PhDT.........3L. doi:10.1002/sapm192434191. ISSN 0097-1421.

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