Abstract

We study the so-called magic mixing angles for doubly heavy baryons. Defining that a magic mixing angle rotates states with definite 2S+1(lλ)J^{2S+1}(l_λ)_J to make them heavy-quark symmetric states, we derive the magic mixing angle only in the case Lρ=0L_ρ=0 between the heavy quark symmetric states with quantum numbers (J,jℓ)\left(J, j_\ell\right) and the states with (J,sq+jρ)=(J,{4lλ/2lλ})\left(J, s_q+j_ρ\right)=\left(J, \{^4l_λ/^2l_λ\}\right) for a doubly heavy baryon in the standard ρ−λρ-λ configuration, where j⃗ℓ=l⃗λ+s⃗q\vec j_\ell=\vec l_λ+\vec s_q, s⃗ρ=s⃗Q1+s⃗Q2\vec s_ρ=\vec s_{Q1}+\vec s_{Q2}, and j⃗ρ=s⃗ρ+L⃗ρ\vec j_ρ=\vec s_ρ+\vec L_ρ. We discuss how this mixing angle affects model building for a doubly heavy baryon.

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