simple quark model
Recently Published Documents


TOTAL DOCUMENTS

14
(FIVE YEARS 0)

H-INDEX

8
(FIVE YEARS 0)

2010 ◽  
Vol 842 (1-4) ◽  
pp. 72-81
Author(s):  
E.M. Henley ◽  
Kevin Pham

2003 ◽  
Vol 18 (39) ◽  
pp. 2837-2847 ◽  
Author(s):  
WOLFGANG LUCHA ◽  
FRANZ F. SCHÖBERL

Motivated by the recent surprising discovery of two new meson states with [Formula: see text] quark content but unexpectedly low masses and narrow total decay widths, we work out, in a nonrelativistic potential-model approach developed already some two decades ago, the predictions for the energy levels of the corresponding charm–anti-strange quark bound states. In spite of the fact that this simple quark model reproduces the mass spectrum of the previously observed hadrons remarkably well, we are led to the conclusion that, without considerable modifications, both the new states do not fit into this framework.


2002 ◽  
Vol 65 (6) ◽  
Author(s):  
I. C. Cloet ◽  
D. B. Leinweber ◽  
A. W. Thomas

1998 ◽  
Vol 13 (36) ◽  
pp. 2887-2901
Author(s):  
V. GUPTA ◽  
P. RITTO ◽  
G. SÁNCHEZ-COLÓN

The spin-1/2 baryons are pictured as a composite system made out of a "core" of three valence quarks (as in the simple quark model) surrounded by a "sea" (of gluon and [Formula: see text] pairs) which is specified by its total quantum numbers. We assume that the sea is an SU(3) flavor octet with spin 0 or 1 but no color. This model, considered earlier, is used to obtain simultaneous fits for masses, magnetic moments and GA/GV for semileptonic decays. These fits give predictions for nucleon spin distributions in reasonable agreement with experiment.


1994 ◽  
Vol 568 (4) ◽  
pp. 798-808 ◽  
Author(s):  
F.M. Steffens ◽  
A.W. Thomas

1992 ◽  
Vol 07 (32) ◽  
pp. 3037-3043 ◽  
Author(s):  
T. GOLDMAN ◽  
J.A. HENDERSON ◽  
A.W. THOMAS

In generating a charge-symmetry breaking potential using ρ-ω mixing it is usually assumed that the mixing amplitude is constant (at the on-mass-shell value). Since the exchanged meson is actually far off-shell one must question the validity of this assumption. By constructing a simple quark model in which the mixing is generated by the u-d quark mass difference, we find that the assumption seems to be a very poor one.


1991 ◽  
Vol 266 (3-4) ◽  
pp. 458-462 ◽  
Author(s):  
R.L. Jaffe ◽  
Harry J. Lipkin

1988 ◽  
Vol 37 (5) ◽  
pp. 2088-2097 ◽  
Author(s):  
S. Kumano ◽  
E. J. Moniz

Sign in / Sign up

Export Citation Format

Share Document