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An introduction to the quark model

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 />

Heavy-light mesons<br />

Most dangerous sec<strong>to</strong>r<br />

Remember: electron more relativistic in H than in Ps<br />

Never<strong>the</strong>less, some properties of <strong>the</strong> naive <strong>quark</strong> <strong>model</strong> applied<br />

<strong>to</strong> (Q¯q) survive.<br />

Reduced mass<br />

1<br />

µ = 1 1<br />

+<br />

m M<br />

dominated by <strong>the</strong> light <strong>quark</strong>.<br />

1<br />

m ,<br />

Thus universal excitation energies and wave functions<br />

One aspect of Heavy <strong>quark</strong> symmetry<br />

Spin effects ∝ 1/M<br />

D ∗ − D = 2010 − 1870 = 140 MeV<br />

B ∗ − B = 5325 − 5280 = 45 MeV<br />

JMR Quark Model

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