scholarly journals Hadronic decay width from finite-volume energy spectrum in lattice QCD

Author(s):  
Pietro Giudice ◽  
Michael J. Peardon ◽  
Volker Crede ◽  
Paul Eugenio ◽  
A. Ostrovidov
2008 ◽  
Vol 2008 (08) ◽  
pp. 024-024 ◽  
Author(s):  
V Bernard ◽  
M Lage ◽  
U.-G Meißner ◽  
A Rusetsky

2020 ◽  
Vol 102 (11) ◽  
Author(s):  
Andrei Alexandru ◽  
Ruairí Brett ◽  
Chris Culver ◽  
Michael Döring ◽  
Dehua Guo ◽  
...  

2021 ◽  
Vol 2021 (2) ◽  
Author(s):  
Gavin K. C. Cheung ◽  
◽  
Christopher E. Thomas ◽  
David J. Wilson ◽  
Graham Moir ◽  
...  

Abstract Elastic scattering amplitudes for I = 0 DK and I = 0, 1 $$ D\overline{K} $$ D K ¯ are computed in S, P and D partial waves using lattice QCD with light-quark masses corresponding to mπ = 239 MeV and mπ = 391 MeV. The S-waves contain interesting features including a near-threshold JP = 0+ bound state in I = 0 DK, corresponding to the $$ {D}_{s0}^{\ast } $$ D s 0 ∗ (2317), with an effect that is clearly visible above threshold, and suggestions of a 0+ virtual bound state in I = 0 $$ D\overline{K} $$ D K ¯ . The S-wave I = 1 $$ D\overline{K} $$ D K ¯ amplitude is found to be weakly repulsive. The computed finite-volume spectra also contain a deeply-bound D* vector resonance, but negligibly small P -wave DK interactions are observed in the energy region considered; the P and D-wave $$ D\overline{K} $$ D K ¯ amplitudes are also small. There is some evidence of 1+ and 2+ resonances in I = 0 DK at higher energies.


2012 ◽  
Vol 27 (09) ◽  
pp. 1250050 ◽  
Author(s):  
V. G. BORNYAKOV ◽  
V. K. MITRJUSHKIN

Landau gauge gluon propagators are studied numerically in the SU (3) gluodynamics as well as in the full QCD with the number of flavors nF = 2 using efficient gauge fixing technique. We compare these propagators at temperatures very close to the transition point in two phases: confinement and deconfinement. The electric mass mE has been determined from the momentum space longitudinal gluon propagator. Gribov copy effects are found to be rather strong in the gluodynamics, while in the full QCD case they are weak ("Gribov noise"). Also we analyze finite volume dependence of the transverse and longitudinal propagators.


2014 ◽  
Vol 90 (5) ◽  
Author(s):  
Jia-Jun Wu ◽  
T.-S. H. Lee ◽  
A. W. Thomas ◽  
R. D. Young

2005 ◽  
Vol 9 ◽  
pp. 321-330 ◽  
Author(s):  
Anthony W Thomas ◽  
Jonathan D Ashley ◽  
Derek B Leinweber ◽  
Ross D Young

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