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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 />

Improvements: fine structure<br />

ψ ′ → χJ + γ , χJ → J/ψ + γ ,<br />

Masses accurately measured with antipro<strong>to</strong>ns<br />

analysed with<br />

<strong>to</strong> first order<br />

M( 3 P0) = Mt − 2 〈Vls〉 − 4 〈Vt〉 ,<br />

M( 3 P1) = Mt − 〈Vls〉 + 2 〈Vt〉 ,<br />

M( 3 P2) = Mt + 〈Vls〉 − 2<br />

〈Vt〉 ,<br />

5<br />

V (r) + Vss(r) σ1.σ2 + Vls(r) ℓ.s + Vt(r) S12 ,<br />

Mt = 1<br />

<br />

M(<br />

9<br />

3 P0) + 3 M( 3 P1) + 5 M( 3 <br />

P2) ,<br />

〈Vls〉 = 1<br />

<br />

−2 M(<br />

12<br />

3 P0) − 3 M( 3 P1) + 5 M( 3 <br />

P1) ,<br />

〈Vt〉 = 5<br />

<br />

2 M(<br />

72<br />

3 P0) − 3 M( 3 P1) + M( 3 <br />

P1) .<br />

JMR Quark Model

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