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Doubly heavy hadrons and the domain of validity of doubly heavy diquark--anti-quark symmetry
High Energy Physics - Phenomenology · Submitted 7 Jun 2006
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We argue on very general grounds that the charm quark mass is substantially too light for the symmetry to emerge automatically via colour coulombic interactions.
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The abstract, sentence by sentence
In the limit of heavy quark masses going to infinity, a symmetry is known to emerge in QCD relating properties of hadrons with two heavy quarks to analogous states with one heavy anti-quark. A key question is whether the charm mass is heavy enough so that this symmetry is manifest in at least an approximate manner. The issue is crucial in attempting to understand the recent reports by the SELEX Collaboration of doubly charmed baryons. We argue on very general grounds that the charm quark mass is substantially too light for the symmetry to emerge automatically via colour coulombic interactions. However, the symmetry could emerge approximately depending on the dynamical details.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In the limit of heavy quark masses going to infinity, a symmetry is known to emerge in QCD relating properties of hadrons with two heavy quarks to analogous states with one heavy anti-quark. | background 1.00 | 0.04 | 0.04 | asserted 1.00 |
| s1 | A key question is whether the charm mass is heavy enough so that this symmetry is manifest in at least an approximate manner. | gap 0.73 | 0.05 | 0.04 | unclear 0.70 |
| s2 | The issue is crucial in attempting to understand the recent reports by the SELEX Collaboration of doubly charmed baryons. | background 0.94 | 0.04 | 0.03 | asserted 0.94 |
| s3 | We argue on very general grounds that the charm quark mass is substantially too light for the symmetry to emerge automatically via colour coulombic interactions. | result 0.77 | 0.63 | 0.68 | asserted 0.89 |
| s4 | However, the symmetry could emerge approximately depending on the dynamical details. | interpretation 0.56 | 0.29 | 0.18 | hedged possibility 1.00 |
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The paper
Original abstract
In the limit of heavy quark masses going to infinity, a symmetry is known to emerge in QCD relating properties of hadrons with two heavy quarks to analogous states with one heavy anti-quark. A key question is whether the charm mass is heavy enough so that this symmetry is manifest in at least an approximate manner. The issue is crucial in attempting to understand the recent reports by the SELEX Collaboration of doubly charmed baryons. We argue on very general grounds that the charm quark mass is substantially too light for the symmetry to emerge automatically via colour coulombic interactions. However, the symmetry could emerge approximately depending on the dynamical details.
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References
How the literature uses it
18 arXiv papers cite this in 20 sentences
Papers citing it · 16 sentences without a confident label
Cites it as background 4 papers
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Numerous theoretical investigations have been conducted on the production, mass spectra, and both strong and weak or radiative decays of doubly heavy baryons, utilizing a variety of methodologies [ref] .
Final-state rescattering mechanism of double-charm baryon decays: $\mathcal{B}_{cc}\to\mathcal{B}_{c}P$ · Introduction · 0.98
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The domain of the validity of the symmetry were discussed a decade ago in Ref. [ref] .
Light pseudoscalar meson and doubly charmed baryon scattering lengths with heavy diquark-antiquark symmetry · Introduction · 0.91
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The doubly-heavy $Q̅Q̅qq$ tetraquarks then become related to singly-heavy $Qqq$ baryons, just like doubly-heavy $Q̅Q̅q̅$ baryons become related to singly-heavy $Qq̅$ mesons [ref] .
Lattice QCD investigation of a doubly-bottom $\bar{b} \bar{b} u d$ tetraquark with quantum numbers $I(J^P) = 0(1^+)$ · Introduction · 0.88
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