Abstract
A formalism is developed for using geometric probability techniques to evaluate interaction energies arising from a general radial potential V(r12), where r12 =|r2-r1|. The integrals that arise in calculating these energies can be separated into a radial piece that depends on r12 and a nonradial piece that describes the geometry of the system, including the density distribution. We show that all geometric information can be encoded into a "radial density function" G(r12;p1,P2), which depends on r12 and the densities p1 and p2 of two interacting regions. G(r12;p1,p2) is calculated explicitly for several geometries and is then used to evaluate interaction energies for several cases of interest. Our results find application in elementary particle, nuclear, and atomic physics.
| Original language | English |
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| Pages (from-to) | 1103-1112 |
| Number of pages | 10 |
| Journal | Journal of Mathematical Physics |
| Volume | 40 |
| Issue number | 2 |
| DOIs | |
| State | Published - 02 1999 |
| Externally published | Yes |