Connection of Elastic Electromagnetic Nucleon Form Factors at Large $Q^{2}$ and Deep Inelastic Structure Functions Near Threshold

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26 January 1970

journal article
research article
Published by American Physical Society (APS) in Physical Review Letters

Vol. 24 (4) , 181-186
https://doi.org/10.1103/physrevlett.24.181

Abstract

It is suggested that if the structure function

ν W_{2}

for deep inelastic electron-proton scattering behaves near threshold as

ν W_{2} \sim (\frac{1}{ω}) {(1 - \frac{1}{ω})}^{p} for ω \equiv \frac{2 M ν}{Q^{2}} \to 1,

then the elastic electromagnetic form factor of the proton

F_{1}

behaves for large momentum transfers as

F_{1} (Q^{2}) \sim {(\frac{1}{Q^{2}})}^{\frac{(p + 1)}{2}} for Q^{2} \to \infty

Keywords

This publication has 10 references indexed in Scilit:

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