Relativistic three-particle quantization condition for nondegenerate scalars
arXiv:2011.05520 · doi:10.1103/PhysRevD.103.054503
Abstract
The formalism relating the relativistic three-particle infinite-volume scattering amplitude to the finite-volume spectrum has been developed thus far only for identical or degenerate particles. We provide the generalization to the case of three nondegenerate scalar particles with arbitrary masses. A key quantity in this formalism is the quantization condition, which relates the spectrum to an intermediate K matrix. We derive three versions of this quantization condition, each a natural generalization of the corresponding results for identical particles. In each case we also determine the integral equations relating the intermediate K matrix to the three-particle scattering amplitude, . The version that is likely to be most practical involves a single Lorentz-invariant intermediate K matrix, . The other versions involve a matrix of K matrices, with elements distinguished by the choice of which initial and final particles are the spectators. Our approach should allow a straightforward generalization of the relativistic approach to all other three-particle systems of interest.
34 pages, 7 figures; v2: added section 2 providing general recipe for developing formalism; fixed typos; matches with published version
References in corpus (9)
- A relativistic, model-independent, three-particle quantization condition
- Three particle quantization condition in a finite volume: 2. general formalism and the analysis of data
- Three-body Unitarity in the Finite Volume
- Three-particle quantization condition in a finite volume: 1. The role of the three-particle force
- Implementing the three-particle quantization condition including higher partial waves
- Three-body Unitarity with Isobars Revisited
- Alternative derivation of the relativistic three-particle quantization condition
- Equivalence of relativistic three-particle quantization conditions
- Modeling few-body resonances in finite volume