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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 />

Permutation symmetry for (qqQ)<br />

For instance Ξ − = (ssd) or Λ = (uds) in <strong>the</strong> limit where SU(2) is<br />

exact<br />

Ψ = ψ(x, y) ψs ψi ψc ,<br />

should be antisymmetric (A), given that ψc is A,<br />

For instance Λ ground state has I = 0 (A), and Sqq = 0 (A), while<br />

ψ(x, y) is symmetric (S) in x,<br />

For instance, ψ(x, y) ∝ exp[−a x 2 − b y 2 ] in HO.<br />

First orbital excitation of Λ? Keep I = 0. If ψ(x, y) is excited in y,<br />

i.e., ℓy = 1, <strong>the</strong>n keep Sqq = 0, thus Sqqs = 1/2 and two<br />

possibilities<br />

J = 1/2<br />

J = 3/2<br />

with <strong>the</strong> possibility of spin-orbit splitting among <strong>the</strong>m<br />

O<strong>the</strong>r orbital excitation of Λ? Yes, with ψ(x, y) now odd in x, and<br />

thus Sqq = 1, and various recoupling for Sqqs and J.<br />

JMR Quark Model

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