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It is known that the square root of the electron density satisfies - (1/2{^2+v_ (n;r) +vₒ (n;r) }n^1/2 (r) =₌n^1/2 (r), where vₒ is the Kohn-Sham potential and ₌ is its highest-occupied orbital energy. The Pauli potential v_ is defined as the functional derivative of the difference between the noninteracting kinetic energy Tₒn and the full von Weizs\"acker kinetic energy. It has already been proven that v_ (n;r) 0 for all r. By starting primarily with a slightly modified version of an equation of Bartolotti and Acharya, new exact properties of v_ (n;r) are derived for the purpose of approximating it. The gradient expansion for Tₒn gives a v_ (n;r) that is found to violate several of the exact conditions. For instance, v_0 is violated unless the full von Weizs\"acker term is employed. A new approximate form for v_ (n;r) is proposed.
Levy et al. (Fri,) studied this question.