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