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The Heavy Hadron Spectrum
High Energy Physics - Phenomenology · Submitted 17 Oct 1997
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Useful insights come from potential models and applications of Heavy Quark Symmetry and these can be compared with new numerical results from the ab initio methods of Lattice QCD.
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The abstract, sentence by sentence
I discuss the spectrum of hadrons containing heavy quarks ($b$ or $c$), and how well the experimental results are matched by theoretical ideas. Useful insights come from potential models and applications of Heavy Quark Symmetry and these can be compared with new numerical results from the ab initio methods of Lattice QCD.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | I discuss the spectrum of hadrons containing heavy quarks ($b$ or $c$), and how well the experimental results are matched by theoretical ideas. | contribution 0.87 | 0.55 | 0.12 | unclear 0.66 |
| s1 | Useful insights come from potential models and applications of Heavy Quark Symmetry and these can be compared with new numerical results from the ab initio methods of Lattice QCD. | method 0.83 | 0.25 | 0.13 | asserted 0.84 |
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The paper
Original abstract
I discuss the spectrum of hadrons containing heavy quarks ($b$ or $c$), and how well the experimental results are matched by theoretical ideas. Useful insights come from potential models and applications of Heavy Quark Symmetry and these can be compared with new numerical results from the ab initio methods of Lattice QCD.
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References
How the literature uses it
2 arXiv papers cite this in 2 sentences
Papers citing it
Cites it as background 2 papers
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Then, as we change the quark's reduced mass, $μ≡m/2$, we obtain the same solution for a rescaled distance $λr$ where [ref] [equation] A $√(μ)$ behaviour for $A^potl ≡⟨α_QED/r ⟩$ would then correspond to $N≈0$.
QED interaction effects on heavy meson masses from lattice QCD+QED · Discussion · 0.81
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In the language of potential models the heavyonium vector and pseudoscalar mesons differ only through spin-dependent relativistic corrections to the central potential [ref] .
Bottomonium precision tests from full lattice QCD: hyperfine splitting, $\Upsilon$ leptonic width and $b$ quark contribution to $e^+e^- \rightarrow$ hadrons · Discussion : Decay constants · 0.95
Discussion
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