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 />
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