Yu Zhou

most citedDynamically generated

J^{P} = 1/ 2^{-} (3/ 2^{-})

singly charmed and bottom heavy baryons

76 citations · 134 across the 3 of their papers we have counts for

collaborators

3 papers

hep-ph2015★ 2 cited

$S$ -wave $K K^{*}$ interaction in a finite volume and the $f_{1} (1285)$

Li-Sheng Geng, Xiu-Lei Ren, Yu Zhou +2

Lattice QCD simulations provide a promising way to disentangle different interpretations of hadronic resonances, which might be of particular relevance to understand the nature of…

hep-ph2014★ 76 cited

Dynamically generated $J^{P} = 1/ 2^{-} (3/ 2^{-})$ singly charmed and bottom heavy baryons

Jun-Xu Lu, Yu Zhou, Hua-Xing Chen +2

Approximate heavy-quark spin and flavor symmetry and chiral symmetry play an important role in our understanding of the nonperturbative regime of strong interactions. In this work,…

nucl-th2014★ 56 cited

Pseudocalar meson and vector meson interactions and dynamically generated axial-vector mesons

Yu Zhou, Xiu-Lei Ren, Hua-Xing Chen +1

The axial-vector mesons $a_{1} (1260)$ , $b_{1} (1235)$ , $f_{1} (1285)$ , $h_{1} (1170)$ , $h_{1} (1380)$ , and $K_{1} (1270)$ are dynamically generated in the unitized chiral perturbation theory. Such…

S-wave KK∗ interaction in a finite volume and the f1​(1285)

Dynamically generated JP=1/2−(3/2−) singly charmed and bottom heavy baryons

Pseudocalar meson and vector meson interactions and dynamically generated axial-vector mesons

$S$ -wave $K K^{*}$ interaction in a finite volume and the $f_{1} (1285)$

Dynamically generated $J^{P} = 1/ 2^{-} (3/ 2^{-})$ singly charmed and bottom heavy baryons