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Open AccessJournal ArticleDOI

Relativistic, model-independent, three-particle quantization condition

Maxwell T. Hansen, +1 more
- 15 Dec 2014 - 
- Vol. 90, Iss: 11, pp 116003
TLDR
In this paper, a generalization of Luescher's relation between the finite-volume spectrum and scattering amplitudes to the case of three particles is presented, where the couplings are arbitrary aside from a Z2 symmetry that removes vertices with an odd number of particles.
Abstract
We present a generalization of Luescher's relation between the finite-volume spectrum and scattering amplitudes to the case of three particles. We consider a relativistic scalar field theory in which the couplings are arbitrary aside from a Z2 symmetry that removes vertices with an odd number of particles. The theory is assumed to have two-particle phase shifts that are bounded by \pi/2 in the regime of elastic scattering. We determine the spectrum of the finite-volume theory from the poles in the odd-particle-number finite-volume correlator, which we analyze to all orders in perturbation theory. We show that it depends on the infinite-volume two-to-two K-matrix as well as a nonstandard infinite-volume three-to-three K-matrix. A key feature of our result is the need to subtract physical singularities in the three-to-three amplitude and thus deal with a divergence-free quantity. This allows our initial, formal result to be truncated to a finite dimensional determinant equation. At present, the relation of the three-to-three K-matrix to the corresponding scattering amplitude is not known, although previous results in the non-relativistic limit suggest that such a relation exists.

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Hadronic molecules

TL;DR: In this article, the authors review experimental evidences of various candidates of hadronic molecules, and methods of identifying such structures Nonrelativistic effective field theories are the suitable framework for studying hadronic molecule, and are discussed in both the continuum and finite volumes.
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Nonstandard heavy mesons and baryons: Experimental evidence

TL;DR: Recently, a variety of QCD inspired phenomenological models have been proposed, such as meson-gluon hybrids and pentaquark baryons that contain heavy (charm or bottom) quarks as mentioned in this paper.
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Scattering processes and resonances from lattice QCD

TL;DR: In this paper, the authors review progress in the study of few-hadron reactions in which resonances and bound states appear using lattice QCD techniques and present a leading approach that takes advantage of the periodic finite spatial volume used in lattice-QCD calculations to extract scattering amplitudes from the discrete spectrum of QCD eigenstates in a box.
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Nuclear effective field theory: status and perspectives

TL;DR: The nuclear physics landscape has been redesigned as a sequence of effective field theories (EFTs) connected to the Standard Model through symmetries and lattice simulations of Quantum Chromodynamics (QCD) as mentioned in this paper.
References
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Journal ArticleDOI

Introduction to Quantum Field Theory

George Sterman, +1 more
- 01 Nov 1994 - 
TL;DR: In this paper, the authors present a model for scalar fields with spin and canonical quantization, and the nature of perturbative cross-sections for high-energy scattering.
Journal ArticleDOI

Resonance scattering phase shifts on a non-rest frame lattice

TL;DR: In this article, the authors generalize the formalism to the case where the total momentum of the particles is non-zero, i.e. the lattice frame is not the center-of-mass frame of the scattering particles.
Journal ArticleDOI

Weak transition matrix elements from finite volume correlation functions

TL;DR: The two-body decay rate of a weakly decaying particle (such as the kaon) is shown to be proportional to the square of a well-defined transition matrix element in finite volume.
Journal ArticleDOI

Finite-volume effects for two-hadron states in moving frames

TL;DR: In this paper, the authors determine the finite-volume corrections to the spectrum and matrix elements of two-hadron states in a moving frame, i.e., one in which the total momentum of the two hadrons is non-zero.
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