Motion of quarks inside the neutron

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SUMMARY

The discussion focuses on the behavior of quarks within the neutron, specifically using electron-neutron scattering to analyze their motion. S. Kopeky's findings from 1995 indicate that the neutron's root mean square (rms) radius can be expressed as -6 ħ (dG_E^n(Q^2)/dQ^2)|_{Q^2=0} = -0.113 ± 0.005 fm². The charge density is theorized to be highest at the neutron's boundary, suggesting equal probability for quarks to be found there, while their charges cancel out, rendering the neutron neutral externally. The conversation highlights the relevance of generalized parton distributions and lattice calculations in modern research.

PREREQUISITES
  • Understanding of electron-neutron scattering techniques
  • Familiarity with quark model and charge distributions
  • Knowledge of generalized parton distributions (GPDs)
  • Basic concepts of lattice quantum chromodynamics (QCD)
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  • Research the implications of generalized parton distributions in particle physics
  • Study lattice quantum chromodynamics (QCD) methods for calculating quark distributions
  • Explore the significance of the Sachs form factors in neutron structure analysis
  • Investigate recent advancements in electron-neutron scattering experiments
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Physicists, researchers in particle physics, and students studying quark dynamics and neutron structure will benefit from this discussion.

TheMan112
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Using electron-neutron scattering I'm trying to find out how the three quarks (udd) behave inside the neutron. S.Kopeky (Phys. Rev. 1995) found that for small Q2 the equation for the neutrons rms-radius goes towards:

-6 \hbar \frac{dG_E ^n (Q^2)}{dQ^2} \right|_{Q^2=0} = -0.113 \pm 0.005 {fm}^2

I'm not sure how to draw conclusions from this. I imagine the charge density being the highest at the neutron boundary and lower towards the center, this leads me to conclude that the probability for finding any of the quarks is equal and the highest at the boundary and lowest at the center. Since the charges are +2/3, -1/3, -1/3 respectively they should then all cancel each other out at the boundary making the neutron appear non-charged from the outside.
 
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I think you have to get this information from the Lattice---I think there's lots of non-perturbative goo that you have to deal with.
 
The assumptions leading to "the slope of the Sachs FF around zero is proprtional to the mean squared radius" are fairly strong. I can go into the details if you want, but basically you have a non-relativistic approximation relying on RM being large (with R the typical size and M the typical mass of the distribution you are probing). For the nucleon, RM~4.

In any case, those approaches are outdated by now. Generalized parton distributions contain the charge distributions in the transverse (spatial) plane as a function of the momentum fraction (xB). They can be (and are) calculated on the lattice. They can be (and are) measured, and modeled. The field is very active on all fronts I think.

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For all and more than you want on that
hep-ph/0504030
 
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