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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 />

The harmonic oscilla<strong>to</strong>r (HO)<br />

V =<br />

2 K<br />

3<br />

H(m, m, m) = p2 x<br />

m + p2 y<br />

2<br />

r12 + r 2 23 + r 2 <br />

31<br />

m + K (x 2 + y 2 ) ,<br />

<br />

K<br />

E = (6 + 4 nx + 2ℓx + 4 ny + 2 ℓy)<br />

m<br />

N = 2 nx + ℓx + 2 ny + ℓy)<br />

Levels named after <strong>the</strong> multiplicity and ℓ P ,<br />

For instance [56, 0 + ] for <strong>the</strong> ground state with 8 spin 1/2 and 10<br />

spin 3/2, i.e., 2 × 8 + 4 × 10 = 56 states. [56, 0 + ] ′ for Roper.<br />

The first orbital excitation is [70, 1 − ],<br />

<strong>the</strong> first state with a full antisymmetric orbital wave function is<br />

[20, 1 + ].<br />

JMR Quark Model

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