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Through the interaction of Higgs with heavy quarks in standard model, we have systematically studied and predicted the production of excited doubly heavy baryons based on non-relativistic QCD theory. The decay widths, differential distributions, and major theoretical uncertainties of the excited doubly heavy baryons via the process H → QQ' [n] → Ξ QQ'+ Q'̄ + Q̄ H → ⟨ Q Q ′ ⟩ [ n ] → Ξ Q Q ′ + Q ′ ¯ + Q ¯ are discussed in detail. The spin and color quantum number of the intermediate P-wave diquark state QQ' [n] ⟨ Q Q ′ ⟩ [ n ] can be cc [¹P₁]_3̄ ⟨ c c ⟩ [ 1 P 1 ] 3 ¯ , cc [³PJ]_6 ⟨ c c ⟩ [ 3 P J ] 6 , bc [¹P₁]_3̄/ 6 ⟨ b c ⟩ [ 1 P 1 ] 3 ¯ / 6 , bc [³PJ]_3̄/ 6 ⟨ b c ⟩ [ 3 P J ] 3 ¯ / 6 , bb [¹P₁]_3̄ ⟨ b b ⟩ [ 1 P 1
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Ma et al. (2023) studied this question.
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