An introduction to the quark model

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Few-charge systems History of the quark model Mesons Baryons Multiquarks and other exotics Outlook Few-Charge systems Why few-charge systems in lectures about quarks? a if it is allowed to compare small things with great Content 1 Binary atoms 2 Spin-dependent forces 3 Three-body ions 4 (+, +, −, −) molecules Si parva licet componere magnis a JMR Quark Model Virgil
Few-charge systems History of the quark model Mesons Baryons Multiquarks and other exotics Outlook Binary atoms p 2 1 2 m1 + p2 1 − 2 m1 e2 , r12 The centre of mass motion can be removed, The intrinsic Hamiltonian can be rescaled to H = p2 e2 − , 2 µ r h = −∆ − r −1 , with 2 µ e 4 for E and (2 µ e 2 ) −1 for r. Similarly, any oscillator can be reduced to −d/dx 2 + x 2 . JMR Quark Model
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An introduction to the quark model

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