Determination of quark-antiquark component of the photon wave function for u, d, s quarks

2005 ◽  
Vol 68 (11) ◽  
pp. 1830-1841 ◽  
Author(s):  
A. V. Anisovich ◽  
V. V. Anisovich ◽  
L. G. Dakhno ◽  
V. A. Nikonov ◽  
A. V. Sarantsev
2005 ◽  
Vol 68 (12) ◽  
pp. 2081-2092
Author(s):  
V. V. Anisovich ◽  
L. G. Dakhno ◽  
V. N. Markov ◽  
V. A. Nikonov ◽  
A. V. Sarantsev

2019 ◽  
Vol 28 (10) ◽  
pp. 1950087 ◽  
Author(s):  
S. M. Moosavi Nejad ◽  
A. Armat

Performing a fit procedure on the hyperon masses, we first determine the free parameters in the Cornell-like hypercentral potential between the constituent quarks of hyperons in their ground state. To this end, using the variational principle, we apply the hyperspherical Hamiltonian including the Cornell-like hypercentral potential and the perturbation potentials due to the spin–spin, spin–isospin and isospin–isospin interactions between constituent quarks. In the following, we compute the hyperon magnetic moments as well as radiative decay widths of spin-3/2 hyperons using the spin-flavor wave function of hyperons. Our analysis shows acceptable consistencies between theoretical results and available experimental data. This leads to reliable wave functions for hyperons at their ground state.


1965 ◽  
Vol 61 (1) ◽  
pp. 275-278 ◽  
Author(s):  
W. E. Williams

It has been shown in recent years ((5)–(8), (10)) that it is possible to obtain closed form solutions for the time harmonic wave equation when a linear combination of the wave function and its normal derivative is prescribed on the surface of a wedge. Boundary-value problems of this type occur in the problem of diffraction by a highly conducting wedge or by a wedge whose surfaces are thinly coated with dielectric. In certain circumstances such surfaces can support surface waves and one important aspect of the solution of the boundary-value problem is the determination of the amplitude of the surface wave excited.


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