Abstract

We present an implementation of the relativistic three-particle quantization condition including both s- and d-wave two-particle channels. For this, we develop a systematic expansion of the three-particle K matrix, mathcal{K} df,3, about threshold, which is the generalization of the effective range expansion of the two-particle K matrix, mathcal{K} 2. Relativistic invariance plays an important role in this expansion. We find that d-wave two-particle channels enter first at quadratic order. We explain how to implement the resulting multichannel quantization condition, and present several examples of its application. We derive the leading dependence of the threshold three-particle state on the two-particle d-wave scattering amplitude, and use this to test our implementation. We show how strong two-particle d-wave interactions can lead to significant effects on the finite-volume three-particle spectrum, including the possibility of a generalized three-particle Efimov-like bound state. We also explore the application to the 3π+ system, which is accessible to lattice QCD simulations, where we study the sensitivity of the spectrum to the components of mathcal{K} df,3. Finally, we investigate the circumstances under which the quantization condition has unphysical solutions.

Highlights

  • There has been considerable recent progress developing the formalism necessary to extract the properties of resonances coupling to three-particle channels from simulations of lattice QCD, with three different approaches being followed [1,2,3,4,5,6,7]

  • We present an implementation of the relativistic three-particle quantization condition including both s- and d-wave two-particle channels

  • We study the sensitivity of the finite-volume spectrum of the physical 3π+ state, with K2 taken from experiment, to the various terms in Kdf,3

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Summary

Introduction

There has been considerable recent progress developing the formalism necessary to extract the properties of resonances coupling to three-particle channels from simulations of lattice QCD, with three different approaches being followed [1,2,3,4,5,6,7]. The outputs of this work are quantization conditions, which relate the finite-volume spectrum with given quantum numbers to the infinite-volume two- and three-particle interactions. This development is timely since simulations have extensive results for the finite-volume spectrum above the three-particle threshold; see, e.g., refs. Turning the formalism into a practical tool remains, a significant challenge To date, this has been done only for the simplest case, in which all particles are spinless and identical, the total momentum vanishes, the two-particle interaction is purely s-wave, and three particles interact only via a momentum-independent contact interaction [4, 6, 13,14,15].1. This has been done only for the simplest case, in which all particles are spinless and identical, the total momentum vanishes, the two-particle interaction is purely s-wave, and three particles interact only via a momentum-independent contact interaction [4, 6, 13,14,15].1 This is the analog in the three-particle system of the initial implementations of the two-particle quantization condition of Luscher [16, 17], which assumed only s-wave interactions and vanishing total momentum

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