Near-threshold Spectrum from Uniformized Mittag-Leffler Expansion -Pole Structure of -
arXiv:2108.11605 · doi:10.1103/PhysRevD.105.014034
Abstract
We demonstrate how S-matrix poles manifest themselves as the physical spectrum near the upper threshold in the context of the two-channel uniformized Mittag-Leffler expansion, an expression written as a sum of pole terms under an appropriate variable where the S-matrix is made single-valued (uniformization). We show that the transition of the spectrum is continuous as a S-matrix pole moves across the boundaries of the complex energy Riemann sheets and that the physical spectrum peaks at or near the upper threshold when the S-matrix pole is positioned sufficiently close to it on the uniformized plane. There is no essential difference on which sheet the pole is positioned. What is important is the existence of a pole near the upper threshold and the distance between the pole and the physical region, not on which complex energy sheet the pole is positioned. We also point out that when the pole is close to the upper threshold, the complex pole does not have the usual meaning of the resonance. Neither the real part represents the peak energy, nor the imaginary part represents the half width. Subsequently, we try to understand the current status of from the viewpoint of the uniformized Mittag-Leffler expansion reflecting in particular, Phys.Rev.Lett.117, 242001 (2016) in which they concluded that is not a conventional resonance but a threshold cusp. We point out that their results turn out to indicate the existence of S-matrix poles near the threshold, which is most likely the origin of the peak found in their calculation of the near-threshold spectrum. In order to support our argument, we set up a separable potential model which shares common behavior of poles near the threshold to the above-mentioned reference and show in our model that the structures near the threshold are indeed caused by these near-threshold poles.
arXiv comment13 pages, 7 pdf figures
References in corpus (21)
- Hadronic molecules
- The hidden-charm pentaquark and tetraquark states
- Observation of a charged charmoniumlike structure in e+e- to pi+pi-J/psi at \sqrt{s}=4.26 GeV
- The states: experimental and theoretical status and perspectives
- Multiquark Resonances
- Non-Standard Heavy Mesons and Baryons, an Experimental Review
- Pentaquark and Tetraquark states
- Heavy-Quark QCD Exotica
- Study of and Observation of a Charged Charmonium-like State at Belle
- Exotics: Heavy Pentaquarks and Tetraquarks
- Observation of the Charged Hadron and Evidence for the Neutral in at MeV
- Exotic Hadrons with Heavy Flavors -X, Y, Z and Related States-
- Observation of a charged (DD*bar)- mass peak in e+e- --> pi+ (DD*bar)- at Ecm=4.26 GeV
- Threshold cusps and triangle singularities in hadronic reactions
- Multiquark States
- Fate of the Tetraquark Candidate Zc(3900) from Lattice QCD
- Confirmation of a charged charmoniumlike state in with double tag
- Extraction of Resonances from Meson-Nucleon Reactions
- The Tetraquark Candidate Zc(3900) from Dynamical Lattice QCD Simulations
- A New Method to Extract Information of Near-Threshold Resonances: Uniformized Pole-Sum Representation of Green's Function and T-matrix
- Application of the Uniformized Mittag-Leffler Expansion to
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- Interpretation of near-threshold peaks using the method of independent S-matrix poles