Abstract

We present a study of a $1+1$ dimensional heavy-light three-body system in finite volume. The heavy-light system is simulated by a coupled-channel $\phi^4$ type lattice model, and both ground state and excited states of multiparticle energy spectra are measured on various lattices. The lattice simulation data analysis is performed based on variational approach.

Highlights

  • Much of strong interaction phenomenology manifests itself in few-body systems

  • We explore the possibility of separating finite-volume and infinite volume dynamics; the two scenarios are connected by interaction potentials instead of scattering amplitudes

  • Though that framework presents a clean and simple illustration of how the quantization conditions of three-body systems in a finite volume arise, the nonrelativistic nature of the energy-momentum dispersion relation may not be capable of describing the lattice spectra; (2) since the simulation of the lattice model is done in discrete rather than continuous spacetime, there is the effect of finite lattice

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Summary

INTRODUCTION

Much of strong interaction phenomenology manifests itself in few-body systems. Due to the many degrees of freedom their quantitative description is more complicated than in the two-body case. Formulating quantization conditions by using reaction amplitudes as input to producing discrete energy spectra or vice versa presents a more conventional foundation of dealing with multiparticle dynamics, one is confronted to deal simultaneously with questions regarding infinite and finite-volume physics. The discretized finite-volume wave functions may be treated as coefficients of secular equations, the quantization condition given by the determinant of secular equations is free of infinite volume reaction amplitudes, and is presented in terms of finitevolume Green’s function and particle interactions. The quantization conditions are applied to extract the parameters of the heavy-light three-body system: the mass of particles and the coupling strength of short-range interactions.

A NONRELATIVISTIC HEAVY-LIGHT THREE-BODY SYSTEM IN FINITE VOLUME
Quantization condition in coordinate representation
Quantization condition in momentum representation
Consistency check at extreme limits
The lattice model action of a heavy-light system
Monte Carlo updating algorithm for a heavy-light system
Operator construction and particle spectra
DATA ANALYSIS
Quantization condition in a discrete finite box
Two-body quantization condition
Three-body quantization condition
G D0 ðp0
SUMMARY
Reduction of two-body system
Reduction of three-body system
Scattering solutions of Faddeev equation with an incoming plane wave
Full Text
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