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首页> 外文期刊>European physical journal >The Q-dependence of the generalised Gerasimov-Drell-Hearn integral for the deuteron, proton and neutron
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The Q-dependence of the generalised Gerasimov-Drell-Hearn integral for the deuteron, proton and neutron

机译:氘,质子和中子的广义Gerasimov-Drell-Hearn积分的Q相关性

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The Gerasimov-Drell-Hearn (GDH) sum rule connects the anomalous contribution to the magnetic moment of the target nucleus with an energy-weighted integral of the difference of the helicity-dependent photoabsorption cross sections. Originally conceived for real photons, the GDH integral can be generalised to the case of photons with virtuality Q2. For spin-1/2 targets such as the nucleon, it then represents the non-perturbative limit of the first moment (Gamma_1) of the spin structure function g1(x,Q2) in deep inelastic scattering (DIS). The data collected by HERMES with a deuterium target are presented together with a re-analysis of previous measurements on the proton. This provides an unprecedented and complete measurement of the generalised GDH integral for photon-virtuality ranging over 1.2Q212.0 GeV2 and for photon-nucleon invariant mass squared W2 ranging over 1W245 GeV2, thus covering simultaneously the nucleon-resonance and the deep inelastic scattering regions. These data allow the study of the Q2-dependence of the full GDH integral, which is sensitive to both the Q2-evolution of the resonance form factors and contributions of higher twist. The contribution of the nucleon-resonance region is seen to decrease rapidly with increasing Q2. The DIS contribution is sizeable over the full measured range, even down to the lowest measured Q2. As expected, at higher Q2 the data are found to be in agreement with previous measurements of the first moment of g1. From data on the deuteron and proton, the GDH integral for the neutron has been derived and the proton-neutron difference evaluated. This difference is found to satisfy the fundamental Bjorken sum rule at Q2 = 5 GeV2.
机译:Gerasimov-Drell-Hearn(GDH)求和规则将对目标原子核的磁矩的反常贡献与依赖于螺旋度的光吸收横截面之差的能量加权积分联系起来。 GDH积分最初是为真实的光子所设想的,可以推广到具有虚度Q2的光子的情况。对于自旋1/2的目标(例如核子),它代表了深非弹性散射(DIS)中自旋结构函数g1(x,Q2)的第一矩(Gamma_1)的非摄动极限。 HERMES收集到的具有氘靶的数据与对质子先前测量值的重新分析一起显示。这为广义GDH积分提供了前所未有的,完整的测量,其光子虚拟度范围超过1.2

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