Abstract

We test the consistency of the data on the nucleon structure functions with analyticity and the Regge asymptotics of the virtual Compton amplitude. By solving a functional extremal problem, we derive an optimal lower bound on the maximum difference between the exact amplitude and the dominant Reggeon contribution for energies nu above a certain high value nu _h(Q^2). Considering in particular the difference of the amplitudes T_1^text {inel}(nu , Q^2) for the proton and neutron, we find that the lower bound decreases in an impressive way when nu _h(Q^2) is increased, and represents a very small fraction of the magnitude of the dominant Reggeon. While the method cannot rule out the hypothesis of a fixed Regge pole, the results indicate that the data on the structure function are consistent with an asymptotic behaviour given by leading Reggeon contributions. We also show that the minimum of the lower bound as a function of the subtraction constant S_1^text {inel}(Q^2) provides a reasonable estimate of this quantity, in a frame similar, but not identical to the Reggeon dominance hypothesis.

Highlights

  • While the method cannot rule out the hypothesis of a fixed Regge pole, the results indicate that the data on the structure function are consistent with an asymptotic behaviour given by leading Reggeon contributions

  • The virtual Compton scattering on the nucleon, in particular the doubly-virtual forward scattering γ ∗(q) + N ( p) → γ ∗(q) + N ( p), is of much interest for the calculation of the electromagnetic mass difference between the proton and the neutron by Cottingham formula [1] and for the study of nucleon polarizabilities

  • The purpose of this work was to investigate the validity of Regge asymptotics for the amplitude of virtual Compton scattering on the nucleon

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Summary

Introduction

The virtual Compton scattering on the nucleon, in particular the doubly-virtual forward scattering γ ∗(q) + N ( p) → γ ∗(q) + N ( p), is of much interest for the calculation of the electromagnetic mass difference between the proton and the neutron by Cottingham formula [1] and for the study of nucleon polarizabilities. The invariant amplitudes are even functions of ν due to crossing symmetry They are real analytic functions in the ν2 complex plane, with singularities along the real axis imposed by unitarity: poles due to the elastic contributions, and cuts produced by the inelastic states. The contribution of the inelastic states is: 309 Page 2 of 12

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