X. Y. Zhou

works on

BESIII experiment 1 branching fractions 1 hyperon decays 1 nonleptonic decay 1 ΔI rule 1

From the 1 of 3 linked papers with an AI index.

most citedEvidence for the semileptonic decays

I^_{c}^{+} \to I^£^{\pm} I ¨ ^{\mp} e^{+} I^½_{e}

1 citations · 1 across the 3 of their papers we have counts for

collaborators

3 papers

hep-ex2026

First measurement of the absolute branching fractions of $I^£^{+}$ nonleptonic decays and test of the $I^ I = 1/2$ rule

BESIII Collaboration, M. Ablikim, M. N. Achasov +689

The paper reports the first absolute measurements of the branching fractions for the Σ⁺ → p π⁰ and Σ⁺ → n π⁺ decays using BESIII J/ψ data, and tests the ΔI = 1/2 rule in Σ hyperon…

hep-ex2025

Measurements of the branching fractions of $I ¨ _{c J} \to I ¨ I ¨ I^\cdot, I ¨ I ¨ I^\cdot^{'}$ and $I ¨ K^{+} K^{-} I^\cdot$

BESIII Collaboration, M. Ablikim, M. N. Achasov +683

Using a sample of $(2712.4 \pm 14.3) \times 1 0^{6} I ¨ $ (3686) events collected by the BESIII detector at the BEPCII collider, we measure the branching fractions of the decays $Ï_{cJ}…

hep-ex2025★ 1 cited

Evidence for the semileptonic decays $I^_{c}^{+} \to I^£^{\pm} I ¨ ^{\mp} e^{+} I^½_{e}$

BESIII Collaboration, M. Ablikim, M. N. Achasov +680

Using $4.5 f b^{- 1}$ of $e^{+} e^{-}$ collision data collected by the BESIII detector at center-of-mass energies between $4.600$ and $4.699 G e V$ , we search for the semileptonic decays…

First measurement of the absolute branching fractions of I^£+ nonleptonic decays and test of the I^I=1/2 rule

Measurements of the branching fractions of I¨cJ​→I¨I¨I^⋅,I¨I¨I^⋅′ and I¨K+K−I^⋅

Evidence for the semileptonic decays I^c+​→I^£±I¨∓e+I^½e​

First measurement of the absolute branching fractions of $I^£^{+}$ nonleptonic decays and test of the $I^ I = 1/2$ rule

Measurements of the branching fractions of $I ¨ _{c J} \to I ¨ I ¨ I^\cdot, I ¨ I ¨ I^\cdot^{'}$ and $I ¨ K^{+} K^{-} I^\cdot$

Evidence for the semileptonic decays $I^_{c}^{+} \to I^£^{\pm} I ¨ ^{\mp} e^{+} I^½_{e}$