Beihang University

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20032011

most citedNew parametrization for the nuclear covariant energy density functional with point-coupling interaction

674 citations

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hep-ph2010★ 16 cited

Light quark mass dependence of the $D$ and $D_{s}$ decay constants

L. S. Geng, M. Altenbuchinger, W. Weise

We study the light quark mass dependence of the $D$ and $D_{s}$ meson decay constants, $f_{D}$ and $f_{D_{s}}$ , using a covariant formulation of chiral perturbation theory ( $χ$ PT) at nex…

hep-ph2010★ 2 cited

The $f_{0} (1370)$ , $f_{0} (1710)$ , $f_{2} (1270)$ , $f_{2}^{'} (1525)$ , and $K_{2}^{*} (1430)$ as dynamically generated states from vector meson - vector meson interaction

L. S. Geng, E. Oset, R. Molina +5

We report on some recent developments in understanding the nature of the low-lying mesonic resonances $f_{0} (1370)$ , $f_{0} (1710)$ , $f_{2} (1270)$ , $f_{2}^{'} (1525)$ , and $K_{2}^{*} (1430)$ . In par…

hep-ph2010

Properties of the ground-state baryons in chiral perturbation theory

J. Martin-Camalich, L. S. Geng, M. J. Vicente Vacas

We review recent progress in the understanding of low-energy baryon structure by means of chiral perturbation theory. In particular, we discuss the application of this formalism to…

hep-ph2010★ 51 cited

Low-lying even parity meson resonances and spin-flavor symmetry

C. Garcia-Recio, L. S. Geng, J. Nieves +1

A study is presented of the $s -$ wave meson-meson interactions involving members of the $ρ -$ nonet and of the $π -$ octet. The starting point is an SU(6) spin-flavor extension of the S…

Light quark mass dependence of the D and Ds​ decay constants

The f0​(1370), f0​(1710), f2​(1270), f2′​(1525), and K2∗​(1430) as dynamically generated states from vector meson - vector meson interaction

Properties of the ground-state baryons in chiral perturbation theory

Low-lying even parity meson resonances and spin-flavor symmetry

Light quark mass dependence of the $D$ and $D_{s}$ decay constants

The $f_{0} (1370)$ , $f_{0} (1710)$ , $f_{2} (1270)$ , $f_{2}^{'} (1525)$ , and $K_{2}^{*} (1430)$ as dynamically generated states from vector meson - vector meson interaction