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An introduction to the quark model

An introduction to the quark model

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Few-charge systems His<strong>to</strong>ry of <strong>the</strong> <strong>quark</strong> <strong>model</strong> Mesons Baryons Multi<strong>quark</strong>s and o<strong>the</strong>r exotics Outlook<br />

Molecules<br />

We learned <strong>to</strong> be careful in this sec<strong>to</strong>r<br />

In 1975, Iwazaki suggested ψ ′ = (c¯cq¯q)<br />

In 1976–77, Voloshin & Okun, and De Rujùla, Georgi & Glashow<br />

molecular structures out of D (∗) and ¯ D (∗)<br />

In particular, DGG were puzzled by ψ(4.04) decaying <strong>to</strong>o often in<br />

D ∗ ¯ D ∗ relative <strong>to</strong> D ¯ D and D ¯ D ∗ + c.c., as compared <strong>to</strong> spin<br />

counting and phase-space.<br />

But Le Yaouanc et al., and Eichten et al. have shown this was<br />

due <strong>to</strong> <strong>the</strong> node structure of this state.<br />

We were accus<strong>to</strong>med <strong>to</strong> orbital excitations (Regge trajec<strong>to</strong>ries),<br />

less <strong>to</strong> radial excitations<br />

JMR Quark Model

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