scholarly journals Proton tensor charges from a Poincaré-covariant Faddeev equation

2018 ◽  
Vol 98 (5) ◽  
Author(s):  
Qing-Wu Wang ◽  
Si-Xue Qin ◽  
Craig D. Roberts ◽  
Sebastian M. Schmidt
Keyword(s):  
Faddeev Equation

Solution of the relativistic three quark Faddeev equation in the Nambu-Jona-Lasinio (NJL) model

1993 ◽  
Vol 318 (1) ◽  
pp. 26-31 ◽  
Author(s):  
Noriyoshi Ishii ◽  
Wolfgang Bentz ◽  
Koichi Yazaki
Keyword(s):  
Faddeev Equation ◽  
Njl Model

scholarly journals Nucleon Mass from a Covariant Three-Quark Faddeev Equation

2010 ◽  
Vol 104 (20) ◽  
Author(s):  
G. Eichmann ◽  
R. Alkofer ◽  
A. Krassnigg ◽  
D. Nicmorus
Keyword(s):  
Faddeev Equation ◽  
Nucleon Mass

scholarly journals LORENTZ BOOSTED NUCLEON-NUCLEON T-MATRIX AND THE TRITON BINDING ENERGY

2009 ◽  
Vol 24 (11n13) ◽  
pp. 804-809 ◽  
Author(s):  
H. KAMADA ◽  
W. GLÖCKLE ◽  
H. WITAŁA ◽  
J. GOLAK ◽  
R. SKIBIŃSKI ◽  
...  
Keyword(s):  
Binding Energy ◽  
Nonlinear Equation ◽  
Faddeev Equation ◽  
Mass Operator ◽  
Nucleon Nucleon ◽  
Spin Rotation ◽  
Triton Binding Energy ◽  
Nucleon System ◽  
T Matrix

The phase equivalent relativistic NN potential, which is related by a nonlinear equation to the original nonrelativistic potential, is used to construct the mass operator (rest Hamiltonian) of the 3-nucleon system. Employing the CD Bonn NN potential, the solution of the relativistic 3N Faddeev equation for 3 H shows slightly less binding energy than the corresponding nonrelativistic result. The effect of the Wigner spin rotation on the binding is very small.

$\bar KNN$ RESONANCE $\bar KNN - \pi YN$ COUPLED CHANNEL FADDEEV EQUATION

2009 ◽  
Vol 24 (11n13) ◽  
pp. 895-900 ◽  
Author(s):  
T. SATO ◽  
Y. IKEDA
Keyword(s):  
Faddeev Equation ◽  
Resonance Energy ◽  
Body Interaction ◽  
Coupled Channels ◽  
S Matrix ◽  
Body Dynamics ◽  
Unphysical Sheet ◽  
Three Body ◽  
Coupled Channel

The three-body resonance of [Formula: see text] system is investigated by using the [Formula: see text] coupled channels Faddeev equation. The resonance energy is determined from the pole of S -matrix on the unphysical sheet. It is found that the pole positions of the predicted amplitudes are significantly modified when the three-body dynamics is approximately treated by introducing the effective [Formula: see text] two-body interaction.

Accuracy of the Bethe-Faddeev Equation

1967 ◽  
Vol 154 (4) ◽  
pp. 934-935 ◽  
Author(s):  
A. G. Petschek
Keyword(s):  
Faddeev Equation

AVOIDING MOVING LOGARITHMIC SINGULARITIES IN 3N FADDEEV EQUATIONS

2009 ◽  
Vol 24 (11n13) ◽  
pp. 779-784
Author(s):  
H. WITAŁA ◽  
W. GLÖCKLE
Keyword(s):  
Elastic Scattering ◽  
Faddeev Equation ◽  
Breakup Reaction ◽  
Standard Approach ◽  
Faddeev Equations ◽  
Logarithmic Singularities ◽  
Good Agreement

We present an approach to solve the three-nucleon Faddeev equation which avoids the complicated singularity pattern going with the moving logarithmic singularities of the standard approach. Very good agreement of the new and old approaches in the application to nucleon-deuteron elastic scattering and the breakup reaction is found.

scholarly journals On the Equivalence of the LS Triad and the Faddeev Equation

1988 ◽  
Vol 79 (6) ◽  
pp. 1396-1403 ◽  
Author(s):  
T. Sawada ◽  
T. Sasakawa
Keyword(s):  
Faddeev Equation
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