1993
DOI: 10.1103/physrevd.47.46
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What do we know about theQ2evolution of the Gerasimov-Drell-Hearn sum rule?

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Cited by 100 publications
(96 citation statements)
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“…AO (Amplitude and Observables) [35]. The amplitudes are parameterized as follows: S-channel resonances are parameterized with relativistic Breit-Wigner forms with momentum-dependent widths.…”
Section: Functions (19)mentioning
confidence: 99%
“…AO (Amplitude and Observables) [35]. The amplitudes are parameterized as follows: S-channel resonances are parameterized with relativistic Breit-Wigner forms with momentum-dependent widths.…”
Section: Functions (19)mentioning
confidence: 99%
“…[15,27], is absorbed into Eq. (19), and the first term in the above equation is just the usual charge operator. All of those charge operators related to the two-body exchange currents are O (1/m 3 ), and can be neglected in the calculation of σ T L , although they are crucial in the case of the γN → ∆ E2 transition [9] process and in reproducing the neutron charge radius [10].…”
Section: The Nucleon Spin Structure In the Resonance Regionmentioning
confidence: 99%
“…(2). Burkert and Li [9] parameterised the experimental Q 2 -evolution of the main nucleon resonances (P 33 (1232), P 11 (1440), S 11 (1535), D 13 (1520), F 15 (1680)), and assumed single-quark transitions to evaluate the contributions from other resonances. Aznauryan [10] described the resonance excitation in the approximation of infinitely narrow resonances, and included a contribution from one-pion exchange in the near-threshold region.…”
mentioning
confidence: 99%
“…As Q 2 → 0, I GDH (Q 2 ) must change sign in order to reach the negative value predicted by the GDH sum rule at Q 2 = 0. Several phenomenological models have been proposed to describe the dependence of the generalised GDH integral on Q 2 [7][8][9][10][11]. Some of these models predict large effects from nucleon-resonance excitation [9,10] or from higher twist [7,11], even for Q 2 up to a few GeV 2 .…”
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confidence: 99%
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