scholarly journals Relativistic corrections to light-cone distribution amplitudes of S-wave Bc mesons and heavy quarkonia

2017 ◽  
Vol 2017 (12) ◽  
Author(s):  
Wei Wang ◽  
Ji Xu ◽  
Deshan Yang ◽  
Shuai Zhao
2020 ◽  
Vol 59 (7) ◽  
pp. 2016-2028
Author(s):  
Bhaghyesh Azhothkaran ◽  
Nilakanthan V. K.

1997 ◽  
Vol 56 (9) ◽  
pp. 5816-5819 ◽  
Author(s):  
Han-Wen Huang ◽  
Hai-Ming Hu ◽  
Xiao-Fei Zhang

2021 ◽  
Vol 2021 (11) ◽  
Author(s):  
June-Young Kim ◽  
Hyun-Chul Kim ◽  
Maxim V. Polyakov

Abstract We investigate the light-cone wave functions and leading-twist distribution amplitudes for the nucleon and ∆ baryon within the framework of the chiral quark-soliton model. The baryon wave function consists of the valence quark and vacuum wave functions. The vacuum wave functions generate all possible higher Fock states by expanding them. We find that it is essential to consider the five-quark component and relativistic corrections to evaluate the distribution amplitudes of the nucleon and ∆ isobar. Having taken into account them, we derive the distribution amplitudes. The results are in good agreement with the lattice data.


2008 ◽  
Vol 52 (4) ◽  
pp. 1151-1154 ◽  
Author(s):  
Hee Sok Chung ◽  
Jungil Lee ◽  
Daekyoung Kang

2017 ◽  
Vol 96 (1) ◽  
Author(s):  
M. A. Olpak ◽  
A. Ozpineci ◽  
V. Tanriverdi
Keyword(s):  

Author(s):  
Jan Cepila ◽  
Jan Nemchik ◽  
Michal Krelina ◽  
Roman Pasechnik
Keyword(s):  

2017 ◽  
Vol 32 (06n07) ◽  
pp. 1750035 ◽  
Author(s):  
Tianhong Wang ◽  
Hui-Feng Fu ◽  
Yue Jiang ◽  
Qiang Li ◽  
Guo-Li Wang

We calculate the annihilation decay rates of the [Formula: see text] and [Formula: see text] charmonia and bottomonia by using the instantaneous Bethe–Salpeter (BS) method. The wave functions of states with quantum numbers [Formula: see text] and [Formula: see text] are constructed. By solving the corresponding instantaneous BS equations, we obtain the mass spectra and wave functions of the quarkonia. The annihilation amplitude is written within Mandelstam formalism and the relativistic corrections are taken into account properly. This is important, especially for high excited states, since their relativistic corrections are large. The results for the [Formula: see text] channel are as follows: [Formula: see text] keV, [Formula: see text] keV, [Formula: see text] keV and [Formula: see text] keV.


Sign in / Sign up

Export Citation Format

Share Document