Relativistic N-Boson Systems Bound by Oscillator Pair Potentials
Abstract
We study the lowest energy E of a relativistic system of N identical bosons bound by harmonic-oscillator pair potentials in three spatial dimensions. In natural units the system has the semirelativistic ``spinless-Salpeter'' Hamiltonian H = \sum_{i=1}^N \sqrt{m^2 + p_i^2} + \sum_{j>i=1}^N gamma |r_i - r_j|^2, gamma > 0. We derive the following energy bounds: E(N) = min_{r>0} [N (m^2 + 2 (N-1) P^2 / (N r^2))^1/2 + N (N-1) gamma r^2 / 2], N \ge 2, where P=1.376 yields a lower bound and P=3/2 yields an upper bound for all N \ge 2. A sharper lower bound is given by the function P = P(mu), where mu = m(N/(gamma(N-1)^2))^(1/3), which makes the formula for E(2) exact: with this choice of P, the bounds coincide for all N \ge 2 in the Schroedinger limit m --> infinity.
Cite
@article{arxiv.math-ph/0110015,
title = {Relativistic N-Boson Systems Bound by Oscillator Pair Potentials},
author = {Richard L. Hall and Wolfgang Lucha and F. F. Schoeberl},
journal= {arXiv preprint arXiv:math-ph/0110015},
year = {2009}
}
Comments
v2: A scale analysis of P is now included; this leads to revised energy bounds, which coalesce in the large-m limit