1970
DOI: 10.1143/ptp.44.193
|View full text |Cite
|
Sign up to set email alerts
|

Electromagnetic Inelastic Form Factors of ProcessesepeN*in a Relativistic Extended Particle Model Based on the Quark Model

Abstract: 193The electromagnetic inelastic form factors of ep.....o;eN* are calculated in a covariant way, on the basis of a relativistic extended-particle model introduced as a straight-forward extension of the nonrelativistic quark model. It is shown that the inelastic form factors have the same q2-dependence as the elastic one at higher momentum transfers, that is,for q2 larger than the nucleon mass. This theoretical result, coming mainly from the Lorentz contraction of the nucleon as an extended particle, is consist… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
25
0

Year Published

1974
1974
2005
2005

Publication Types

Select...
4
2
1

Relationship

0
7

Authors

Journals

citations
Cited by 67 publications
(25 citation statements)
references
References 1 publication
0
25
0
Order By: Relevance
“…To calculate the third part of form factor (20) related to the purely six-quark contribution we use the relativistic determination 9 ~ Q~ exp( -iq x~(r O6q(~t, ..., is; Pout) (22) J where xi are quark coordinates transformed through Jacobi coordinates r and we take the wave function as a solution of the relativistic harmonic oscillator [14] F~a are the charge (quadrupole) form factors calculated with the RSC wave function [11], and relativistic recoil effects are taken into account [13]; Fe, 6q the six-quark charge form factor, Fc, int, FQ,~n t the interference terms between the nucleon part (RSC) and six-quark part of wave function of the deuteron Substituting (23) into (22) one can obtain…”
Section: F=f;+mentioning
confidence: 99%
“…To calculate the third part of form factor (20) related to the purely six-quark contribution we use the relativistic determination 9 ~ Q~ exp( -iq x~(r O6q(~t, ..., is; Pout) (22) J where xi are quark coordinates transformed through Jacobi coordinates r and we take the wave function as a solution of the relativistic harmonic oscillator [14] F~a are the charge (quadrupole) form factors calculated with the RSC wave function [11], and relativistic recoil effects are taken into account [13]; Fe, 6q the six-quark charge form factor, Fc, int, FQ,~n t the interference terms between the nucleon part (RSC) and six-quark part of wave function of the deuteron Substituting (23) into (22) one can obtain…”
Section: F=f;+mentioning
confidence: 99%
“…The second reason is that the simple form of the wave functions [Eqs. (21)(22)(23)(24)(25)] allows us to express the form factor through the experimentally known distributions of the nuclear charge density and the form factors of simpler systems. Moreover, we consider that the contributions from the colored clusters configurations (e.g.…”
Section: Iic1 Form Factor Of a Nucleus With Multiquark Admixturesmentioning
confidence: 99%
“…The Klein-Gordon equation of a system of "k" nucleons, composed of N=3k quarks moving in the potential of a relativistic harmonic oscillator [25] can be written in the form, 0 ) ,..., ( ) ( where the tensor K µν is defined through the metric tensor g µν . In addition, the form factor of the Nq-system has the form, where M k is the parameter relating the internal motion of quarks in 3kq system with the motion of this system as a whole.…”
Section: Iic2 Relativistic Harmonic Oscillator Wave Functions and Mmentioning
confidence: 99%
See 1 more Smart Citation
“…1 l-sl In order to understand the essential features of such models, it is very important to treat every specific problem in a consistent way within the model. This is the reason why we have chosen normalizable solutions of the wave equation 1 l-sl, 5 l and minimal electromagnetic interaction.…”
mentioning
confidence: 99%