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Diquarks as Inspiration and as Objects
High Energy Physics - Phenomenology · Submitted 14 Sep 2004
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim It is plausible that several of the most profound aspects of low-energy QCD dynamics are connected to diquark correlations, including: paucity of exotics (which is the foundation of the quark model and of traditional nuclear physics), similarity of mesons and baryons, color superconductivity at high density, hyperfine splittings, $\Delta I = 1/2$ rule, and some striking features of structure and fragmentation functions.
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The abstract, sentence by sentence
It is plausible that several of the most profound aspects of low-energy QCD dynamics are connected to diquark correlations, including: paucity of exotics (which is the foundation of the quark model and of traditional nuclear physics), similarity of mesons and baryons, color superconductivity at high density, hyperfine splittings, $\Delta I = 1/2$ rule, and some striking features of structure and fragmentation functions. After a brief overview of these issues, I discuss how diquarks can be studied in isolation, both phenomenologically and numerically, and present approximate mass differences for diquarks with different quantum numbers. The mass-loaded generalization of the Chew-Frautschi formula provides an essential tool.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | It is plausible that several of the most profound aspects of low-energy QCD dynamics are connected to diquark correlations, including: paucity of exotics (which is the foundation of the quark model and of traditional nuclear physics), similarity of mesons and baryons, color superconductivity at high density, hyperfine splittings, $\Delta I = 1/2$ rule, and some striking features of structure and fragmentation functions. | background 0.99 | 0.08 | 0.34 | hedged possibility 0.97 |
| s1 | After a brief overview of these issues, I discuss how diquarks can be studied in isolation, both phenomenologically and numerically, and present approximate mass differences for diquarks with different quantum numbers. | contribution 1.00 | 0.90 | 0.12 | asserted 0.97 |
| s2 | The mass-loaded generalization of the Chew-Frautschi formula provides an essential tool. | method 0.93 | 0.29 | 0.08 | asserted 1.00 |
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The paper
Original abstract
It is plausible that several of the most profound aspects of low-energy QCD dynamics are connected to diquark correlations, including: paucity of exotics (which is the foundation of the quark model and of traditional nuclear physics), similarity of mesons and baryons, color superconductivity at high density, hyperfine splittings, $\Delta I = 1/2$ rule, and some striking features of structure and fragmentation functions. After a brief overview of these issues, I discuss how diquarks can be studied in isolation, both phenomenologically and numerically, and present approximate mass differences for diquarks with different quantum numbers. The mass-loaded generalization of the Chew-Frautschi formula provides an essential tool.
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References
How the literature uses it
42 arXiv papers cite this in 68 sentences
Papers citing it · 45 sentences without a confident label
Builds on it 1 paper
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The simplest way to understand Eq. ([ref]) is to view it as an extension of the Selem-Wilczek relation [ref] for the SH hadrons, [equation] which scales as $(M-M_Q)^2∝(α/2)L$ when $L→∞$ but divergent at $L=0$.
Regge behaviors in orbitally excited spectroscopy of charmed and bottom baryons · Spin-independent masses for singly heavy baryons · 0.82
Uses its data or values 2 papers
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Moreover, a generalized Chew-Frautschi formula relating baryon mass to orbital angular momentum is [equation] with $k≈1.15$ GeV $^-1 2$ and $σ≈1.1$ GeV$^2$ [ref] .
Charmed baryon in a Diquark model · Mass Formula and Spectrum · 0.93
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See also Table [ref], where we report some estimations of the masses of axial-vector and scalar diquarks according to some previous studies [ref] .
Strange and nonstrange baryon spectra in the relativistic interacting quark-diquark model with a G\"ursey and Radicati-inspired exchange interaction · Nonrelativistic quark-diquark states · 0.84
Compares with it 1 paper
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Eq. ([ref]) is consistent with the results in Refs. [ref] .
Regge trajectory relations for the universal description of the heavy-light systems: diquarks, mesons, baryons and tetraquarks · relations obtained from the QSSE · 0.87
Cites it as support 1 paper
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This preference for $ud$-type diquarks is corroborated by LQCD studies and deep-inelastic scattering results [ref] .
Quark-diquark effective mass formalism for heavy baryon spectroscopy · Numerical results and discussions · 0.99
Cites it as background 15 papers
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Recall that there is a direct relation between the mass $m$ of a hadron and its orbital excitation quantum number $L$ given by the Regge trajectory equation [ref] : m^2=a+σL ,where $m$ is the mass of the hadron, $a$ is an intercept that depends on the trajectory, and $σ$ is the slope.
No Radial Excitations in Low Energy QCD. II. The Shrinking Radius of Hadrons · Introduction · 0.81
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For simplicity, plots in the $(M, x)$ plane [ref] , $(M-m_R, x)$ plane [ref] , $(M, (x+c_0)^ν)$ plane [ref] , $(M^2, x)$ plane [ref] , $((M-m_R)^2, x)$ plane [ref] or $((M-m_R)^1/ν, x)$ plane [ref] , are all commonly referred as Chew-Frautschi plots. can be plotted in these various planes. ] is one of the effective approaches widely used in the study of hadron spectra [ref] .
Regge trajectories for the doubly heavy triquarks $((Qq)\bar{Q}')$ · Introduction · 0.87
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The overall picture that emerged in the 1980s and 1990s matched the conclusions of Jaffe, Wilczek and Selem&Wilczek [ref] who singled out the spin-0 flavor-antisymmetric diquarks and called them “good diqurks”, as opposed to flavor-symmetric diquark states, referred to as “bad diquarks.” Good diquarks are in the color-antitriplet representation.
QCD Chemistry: Remarks on Diquarks · Introduction · 0.94
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