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On nucleon electromagnetic form factors

机译:关于核子电磁形状因数

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Poincare-covariant Faddeev equation, which describes baryons as composites of confined-quarks and - nonpointlike-diquarks, is solved to obtain masses and Faddeev amplitudes for the nucleon and D. The amplitudes are a component of a nucleon-photon vertex that automatically fulfills the Ward-Takahashi identity for on-shell nucleons. These elements are sufficient for the calculation of a quark core contribution to the nucleons' electromagnetic form factors. An accurate description of the static properties is not possible with the core alone but the error is uniformly reduced by the incorporation of meson-loop contributions. Such contributions to form factors are noticeable for Q(2) less than or similar to 2 GeV2 but vanish with increasing momentum transfer. Hence, larger Q(2) experiments probe the quark core. The calculated behaviour of G(E)(p)(Q(2))/G(M)(p) (Q(2)) on Q(2) is an element of [2, 6] GeV2 agrees with that inferred from polarization transfer data. Moreover, root Q(2)F(2)(Q(2))/F-1(Q(2)) approximate to constant on this domain. These outcomes result from correlations in the proton's amplitude.
机译:求解Poincare-协变Faddeev方程,该方程将重子描述为受限夸克和-非点状二夸克的复合物,以获取核子和D的质量和Faddeev振幅。振幅是自动满足核子-光子顶点的组成部分带壳核子的Ward-Takahashi身份。这些元素足以计算夸克核对核子电磁形状因子的贡献。单独使用磁芯不可能对静态特性进行准确的描述,但是通过引入介子回路贡献,可以均匀地减少误差。 Q(2)小于或类似于2 GeV2时,这种对形状因数的贡献很明显,但随着动量传递的增加而消失。因此,较大的Q(2)实验探究了夸克核。 G(E)(p)(Q(2))/ G(M)(p)(Q(2))在Q(2)上的计算行为是[2,6]的一个元素GeV2与推断的结果一致从极化传输数据。此外,根Q(2)F(2)(Q(2))/ F-1(Q(2))近似于该域上的常数。这些结果来自质子振幅的相关性。

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