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arXiv:2307.15815·v2·High Energy Physics — Phenomenology

Light-Quark Flavour Splitting of Heavy-Light Constituent Diquark Masses and Doubly-Strange Diquarks from QCD Sum-Rules

T. de Oliveira🇨🇦 · D. Harnett🇨🇦 · R. Kleiv🇨🇦 · A. Palameta🇨🇦 · T.G. Steele🇨🇦

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Abstract

QCD Laplace sum-rules are used to examine the constituent mass spectrum of heavy-light [Qq] diquarks with and . As in previous sum-rule studies, the negative parity [Qq] diquark mass predictions do not stabilize, so the sum-rule analysis focuses on positive parity [Qq] diquarks. Doubly-strange [ss] diquarks are also examined, but the resulting sum rules do not stabilize. Hence there is no sum-rule evidence for [ss] diquark states, aiding the interpretation of sum-rule analyses of fully-strange tetraquark states. The SU(3) flavour splitting effects for [Qq] diquarks are obtained by calculating QCD correlation functions of diquark composite operators up to next-to-leading order in perturbation theory, leading-order in the strange quark mass, and in the chiral limit for non-strange (u,d) quarks with an isospin-symmetric vacuum . Apart from the strange quark mass parameter , the strange quark condensate parameter has an important impact on SU(3) flavour splittings. A Laplace sum-rule analysis methodology is developed for the mass difference between the strange and non-strange heavy-light diquarks to reduce the theoretical uncertainties from all other QCD input parameters. The mass splitting is found to decrease with increasing , providing an upper bound on where the mass hierarchy reverses. In the typical QCD sum-rule range , and , with a slight tendency for larger splittings for the channels. These constituent mass splitting results are discussed in comparison with values used in constituent diquark models for tetraquark and pentaquark hadronic states.

Comments: 30 pages, 19 figures, 7 tables. v2 contains extended discussion

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