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  1. International Journal of Theoretical Physics
  2. International Journal of Theoretical Physics : Volume 37
  3. International Journal of Theoretical Physics : Volume 37, Issue 7, July 1998
  4. Rest Frame Properties of the Proton
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International Journal of Theoretical Physics : Volume 56
International Journal of Theoretical Physics : Volume 55
International Journal of Theoretical Physics : Volume 54
International Journal of Theoretical Physics : Volume 53
International Journal of Theoretical Physics : Volume 52
International Journal of Theoretical Physics : Volume 51
International Journal of Theoretical Physics : Volume 50
International Journal of Theoretical Physics : Volume 49
International Journal of Theoretical Physics : Volume 48
International Journal of Theoretical Physics : Volume 47
International Journal of Theoretical Physics : Volume 46
International Journal of Theoretical Physics : Volume 45
International Journal of Theoretical Physics : Volume 44
International Journal of Theoretical Physics : Volume 43
International Journal of Theoretical Physics : Volume 42
International Journal of Theoretical Physics : Volume 41
International Journal of Theoretical Physics : Volume 40
International Journal of Theoretical Physics : Volume 39
International Journal of Theoretical Physics : Volume 38
International Journal of Theoretical Physics : Volume 37
International Journal of Theoretical Physics : Volume 37, Issue 12, December 1998
International Journal of Theoretical Physics : Volume 37, Issue 11, November 1998
International Journal of Theoretical Physics : Volume 37, Issue 10, October 1998
International Journal of Theoretical Physics : Volume 37, Issue 9, September 1998
International Journal of Theoretical Physics : Volume 37, Issue 8, August 1998
International Journal of Theoretical Physics : Volume 37, Issue 7, July 1998
General Techniques for Evaluating Twistor Diagrams
Relativistic Covariant Equal-Time Equation for Quark-Diquark System
The Second-Order Equation from the (1/2, 0) ⊕ (0, 1/2) Representation of the Poincare Group
Quantized (1, 0) ⊕ (0, 1) Fields
Toward an Octonionic World
Double Soliton Solutions of Belinsky–Zakharov Equation Related to the Self-Dual SU(N) Gauge Fields
Rest Frame Properties of the Proton
Generalization of Supersymmetric Quantum Mechanics
Nuclear Field Theory with Chiral Symmetry on a Calabi–Yau Manifold
Clebsch–Gordan Coefficient for q,s-Deformed Two-Dimensional Hydrogen Atom
Quantum Deformation of the Two-Dimensional Hydrogen Atom in a Magnetic Field
Chiral Actions and Einstein's Vacuum Equations
Spectral Theory of Perturbative Decays
International Journal of Theoretical Physics : Volume 37, Issue 6, June 1998
International Journal of Theoretical Physics : Volume 37, Issue 5, May 1998
International Journal of Theoretical Physics : Volume 37, Issue 4, April 1998
International Journal of Theoretical Physics : Volume 37, Issue 3, March 1998
International Journal of Theoretical Physics : Volume 37, Issue 2, February 1998
International Journal of Theoretical Physics : Volume 37, Issue 1, January 1998
International Journal of Theoretical Physics : Volume 36

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Rest Frame Properties of the Proton

Content Provider Springer Nature Link
Author Strobel, George L.
Copyright Year 1998
Abstract The proton is modeled as three quarks of smallcurrent quark mass. The threebody Dirac equation issolved with spin-independent central diagonal linearconfining potentials with an attractive Coulombic term in a relativistic threequark model.Hyperspherical coordinates are used, and the bound stateis found analytically. After integrating over thehyperangles, the Hamiltonian is an 8 by 8 matrix ofcoupled first-order differential equations in onevariable, the hyperradius. These are analytically solvedin hypercentral approximation. For the(1/2$^{+}$)$^{3}$ ground-state configurationin the nonrelativistic large-quark-mass limit, there are no nodes in the wave function.However, in the extreme relativistic limit of smallcurrent quark masses of a few MeV, the expectation valueof the number of nodes is about 1.30 when the potential parameters are chosen to reproducethe proton rms charge radius. The quarks are assumed topossess a Pauli anomalous magnetic moment, like that ofthe electron and muon of (α/2π)(e/m). Assuming all three quarks have equal mass, one can fitthe rest energy, magnetic moment, rms charge radius, andaxial charge of the proton with this relativisticthree-body Dirac equation model. The solution found shows the necessity of including all componentsof the composite three-quark wave function, as the uppercomponent contributes only 0.585 to the norm.
Starting Page 2001
Ending Page 2019
Page Count 19
File Format PDF
ISSN 00207748
Journal International Journal of Theoretical Physics
Volume Number 37
Issue Number 7
e-ISSN 15729575
Language English
Publisher Kluwer Academic Publishers-Plenum Publishers
Publisher Date 1998-01-01
Publisher Place New York
Access Restriction One Nation One Subscription (ONOS)
Subject Keyword Physics Quantum Physics Mathematical and Computational Physics Elementary Particles, Quantum Field Theory
Content Type Text
Resource Type Article
Subject Physics and Astronomy Mathematics
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