“…Thus, K(r) and G(r) integrate to yield the same value of the total kinetic energy, T. In this sense, the local kinetic energy yielding the correct value of the total kinetic energy is only defined up to C * V2p(r), where C is an arbitrary constant. Although the problem of the reconstruction of the one-electron-density matrix p(r, r') from p(r) obtained from the diffraction experiment has been considered before (Aleksandrov, Tsirelson, Reznik & Ozerov, 1989;Tanaka, 1988;Schmider, Smith & Weyrich, 1992;Howard, Huke, Mallinson & Frampton, 1994), we are going to propose here an alternative less accurate but easier approach for the evaluation of the local kinetic energy density at the bond critical point of the multipolefitted electron density. A simple approximate way of directly relating the kinetic energy density to the electron density was introduced by the semiclassical Thomas-Fermi equation (March, 1957) with gradient quantum corrections (von Weizsacker, 1935;Kirzhnitz, 1957).…”