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Describing non-$q\bar q$ candidates
High Energy Physics - Phenomenology · Submitted 12 Jul 2004
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim In this work we present a possible description of these states in terms of tetraquarks.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
Despite the apparent simplicity of meson spectroscopy there are some states which cannot be accommodated in the usual $q\bar q$ structure. Among them there are either exotic states as the X(1600) or the recently measured charm states $D_{sJ}^*$ and X(3872) and some of the light scalar mesons. In this work we present a possible description of these states in terms of tetraquarks.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Despite the apparent simplicity of meson spectroscopy there are some states which cannot be accommodated in the usual $q\bar q$ structure. | background 0.97 | 0.05 | 0.04 | asserted 0.98 |
| s1 | Among them there are either exotic states as the X(1600) or the recently measured charm states $D_{sJ}^*$ and X(3872) and some of the light scalar mesons. | background 1.00 | 0.09 | 0.05 | asserted 0.81 |
| s2 | In this work we present a possible description of these states in terms of tetraquarks. | contribution 1.00 | 0.89 | 0.58 | hedged possibility 0.97 |
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Original abstract
Despite the apparent simplicity of meson spectroscopy there are some states which cannot be accommodated in the usual $q\bar q$ structure. Among them there are either exotic states as the X(1600) or the recently measured charm states $D_{sJ}^*$ and X(3872) and some of the light scalar mesons. In this work we present a possible description of these states in terms of tetraquarks.
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References
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1 arXiv paper cite this in 1 sentence
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Cites it as background 1 paper
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In the literature, $X(3872)$ has been interpreted as a $cc̅g$ hybrid state [ref] , a diquark-antidiquark state [ref] , a $cc̅$ and meson cloudy mixing state [ref] or a deuteron-like molecular state concerning its mass is approximate to the threshold of $D^0D^∗ 0$ [ref] .
Strong and radiative decays of X(3872) as a hadronic molecule with a negative parity · Introduction · 0.99
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