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Precision measurements of the proton and deuteron polarized structure functions.

机译:质子和氘核极化结构功能的精确测量。

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Experiment E155 at the Stanford Linear Accelerator Center measured the longitudinal and transverse polarized deep-inelastic scattering asymmetries for the proton and deuteron using longitudinally-polarized electron beams with energies of 48.3 GeV and 38.8 GeV, respectively. The electron beam polarization was measured by Møller polarimetry to be 0.81 ± 0.02. Dynamically-polarized solid 15N3 and 6Li2H were used as the target materials. The scattered electrons were detected in three independent spectrometers at 2.75°, 5.5°, and 10.5°, covering a kinematic range of 0.014 ≤ x ≤ 0.9 and 1.0(GeV/ c)2Q2 ≤ 40(GeV/ c)2. The 10.5° spectrometer was constructed for this experiment. The structure functions gp1 and gd1 were extracted from the asymmetry data, and, in combination with world data, were fit in next-to-leading order perturbative QCD. The Q 2 dependence of g1 differed slightly from that of F1. The g1 results are consistent with the Bjorken sum rule. The structure functions gp2 and gd2 were extracted from the asymmetry data, and were used to extract the twist-3 reduced matrix elements dp2,dd2 , and dn2 .
机译:斯坦福线性加速器中心的实验E155使用能量分别为48.3 GeV和38.8 GeV的纵向极化电子束,测量了质子和氘核的纵向和横向极化深非弹性散射不对称性。电子束极化通过Møller极化法测得为0.81±0.02。以动态极化的固体 15 N 3 6 Li 2 H为目标材料。在2.75°,5.5°和10.5°的三个独立光谱仪中检测到散射电子,其运动学范围为0.014≤ x ≤0.9和1.0(GeV / c 2 Q 2 ≤40(GeV / c 2 。为此实验构造了10.5°光谱仪。结构函数 g p 1 g d 从不对称数据中提取 1 ,并与世界数据结合,以次于前导的扰动QCD进行拟合。 g 1 Q 2 依赖性与 F 1 g 1 结果与Bjorken sum规则一致。结构函数 g p 2 g d 从不对称数据中提取 2 ,并用于提取Twist-3归约矩阵元素 d p 2 ,d d 2 d n 2

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