Density Functional Theory of Stopping Power
Chapter
Abstract
The density-functional (DF) formalism provides a very useful tool to tackle many-body problems in a simplified manner. In this approach, the many-body problem is replaced by a Hartree-like equation, such as
$$
\left[ { - \frac{{{\nabla ^{\text{2}}}}}{2} + {{\text{V}}_{{\text{eff}}}}\left( {\text{r}} \right)} \right]{\text{ }}{\psi _{\text{i}}}\left( {\text{r}} \right) = {\varepsilon _{\text{i}}}{\psi _{\text{i}}}\left( {\text{r}} \right).
$$
(1)
(We use atomic units, e2 = h = m = 1 throughout except where otherwise indicated. The unit of energy is the Hartree (27.2 eV) and the Bohr’s radius a0 = 0.529 Å is the unit of length).
Keywords
Effective Charge Yukawa Potential Bear Approximation Scatter Phase Shift Transport Cross Section
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.
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