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Mixing angle between $^3P_1$ and $^1P_1$ in HQET
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abstract
Some claim that there are two independent mixing angles ($\theta = 35.3^\circ$, $-54.7^\circ$) between $^3P_1$ and $^1P_1$ states of heavy-light mesons in heavy quark symmetric limit, and others claim there is only one ($\theta = 35.3^\circ$). We clarify the difference between these two and suggest which should be adopted. General arguments on the mixing angle between $^3L_L$ and $^1L_L$ of heavy-light mesons are given in HQET and a general relation is derived in heavy quark mass limit as well as that including the first order correction in $1/m_Q$.
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Cited by 1 Pith paper
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Phenomenology of $D_{s1}$ mesons radiative transitions
Relativistic spin-dependent corrections to the electric dipole operator reverse the expected radiative width hierarchy of the D_s1 mesons.
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