English

The Relativistic Three-Body Bound State in a 3D Formulation

Nuclear Theory 2014-11-17 v1

Abstract

Background: The relativistic three-body problem has a long tradition in few-nucleon physics. Calculations of the triton binding energy based on the solution of the relativistic Faddeev equation in general lead to a weaker binding than the corresponding non-relativistic calculation. Purpose: In this work we solve for the three-body binding energy as well as the wave function and its momentum distribution. The effect of the different relativistic ingredients are studied in detail. Method: Relativistic invariance is incorporated within the framework of Poincar{\'e} invariant quantum mechanics. The relativistic momentum-space Faddeev equation is formulated and directly solved in terms of momentum vectors without employing a partial-wave decomposition. Results: The relativistic calculation gives a three-body binding energy which is about 3% smaller than its non-relativistic counterpart. In the wave function, relativistic effects are manifested in the Fermi motion of the spectator particle. Conclusions: Our calculations show that though the overall relativistic effects in the three-body bound state are small, individual effects by themselves are not necessarily small and must be taken into account consistently.

Keywords

Cite

@article{arxiv.1409.1650,
  title  = {The Relativistic Three-Body Bound State in a 3D Formulation},
  author = {M. R. Hadizadeh and Ch. Elster and W. N. Polyzou},
  journal= {arXiv preprint arXiv:1409.1650},
  year   = {2014}
}

Comments

20 pages, 1 table and 6 figures

R2 v1 2026-06-22T05:49:11.426Z